Hi everyone. As several people have pointed out, the audio doesn't quite sound right. I can't fix this -- I can only take the video down and replace it in the next couple of days. As it seems to at least be clearly understandable I'll let it up. Will make sure that next week we're back to the normal quality. Sorry about that.
I didn't notice a problem at all, even at a second hearing. So the audio track is in a superposition of weird/not weird. But there is nothing spooky about it.
@@SabineHossenfelder Dont worry about the sound Sabine.. When will you physicists finally get real and admit that we're all living inside a super-advanced, hyper-realistic holodeck complex super-structure.. That would explain emergence, fine-tuning and the holographic nature of our reality. The organic big bang theory doesn't explain any of that 😲😲😲
I'm happy that my teacher of quantum physics was Paweł Horodecki, he showed us in 2008 at one of the first lessons this insane topic of Elitzur and Vaidman bomb experiment. I still treat my notes from it like some sacral artifact. I talked to all my friends about it even when they had nothing to do with physics .Great memories
The bomb experiment may not actually be very weird at all. It may just come from the fact we arbitrarily choose to treat photons differently than other states. As shown with the second beam splitter, beam splitters are sort of like a logic gate with _two_ inputs and _two_ outputs. It is basically equivalent to the Givens logic gate with the angle π/4. If both inputs are 0, it outputs 00, which is the analogue to no light on the beam splitter, then no light comes out. If both inputs are 1, it outputs 11, which is the analogue to light on both angles of the beam splitter just producing light on both angles of the output. If only one of the inputs is 1, meaning you only shine light at it from one angle, then the output is 50% chance 01 or 50% chance 10, meaning it has a 50% chance to redirect the photon to either path. Since it is a logic gate and all quantum, logic gates are unitary, applying it twice cancels itself out, so if your input is 10 and you apply it twice, your put is 10. If you apply a phase shifter on one of the paths, basically the Pauli-Z logic gate, then it ends up flipping the final path the photon takes, so if you pass in 10 into the first beam splitter, apply a phase shift on one of the paths, then 01 will come out the second beam splitter. This also replicates what happens if you make a measurement, the state undergoes decoherence after the first beam splitter and becomes either exactly 01 or 10, and thus when it hits the second beam splitter it will have a 50% chance of leaving as a 01 or 10. If you implemented this circuit into anything _else_ besides photons, all the mystery immediately disappears. For example, if you assign 1 to an electron with spin up and 0 to an electron with spin down, two tangible electrons both take the two paths. There isn't much of a mystery here because both electrons are tangible objects that carry a bit of information as well as some phase related information, so when they recombine on the other end they can interfere based on that information, and making a measurement to the tangible electron causes decoherence. This can be explained in entirely classical terms, you don't even need to resort to quantum mechanics. The potential fallacious reasoning arises from the fact that we treat photons differently from other quantum states. We assume that a photon in the 0 state does not actually exist and thus cannot carry any information at all. But if we don't treat it differently, if we treat it like any other state, then a photon in the 0 state could indeed carry information and propagate through the system. It would show up on any detector as a 0 because it only carries phase-related information, but it may or may not interact with a detector (depending on whether or not the bomb is a dud), may or may not causing decoherence, and then when it recombines with the other photon, it could alter how they recombine. That would mean it is not an "interaction free measurement," it is an interaction with a photon in the 0 state. Just food for thought.
I started watching quantum physics a few years ago because I thought it was weird...no what if it's not weird it's no fun Guess I will go back to the why files and heckelfish to get my daily weird...😊😊
@@amihart9269 I think you are misunderstanding why its weird. Why its actually weird is because all of this only happens once you add a live bomb, and you can use it to tell if the bomb is live without the photon ever going down the bottom path and activating the bomb. Before you add a bomb, the photon always acts like a wave and goes through both paths which causing it to interfere with itself making it to where it never goes to detector B. But after, and when the bomb is live, the photon starts to act like a particle and only goes through one path. Just the potential interaction with the bomb is enough to collapse the wave function somehow.
I believe interpretations are that which is weird. In quantum physics particles are NOT in multiple places at once, we just cannot say for certain where a particle is until measured.
Well yes and no. That's the whole idea of the superposition. The particle is located at all of the possible places at the same time before the observation is made. In short - all that is possible, IS possible. It's just about how probable it is. If you were to repeat the measurement over and over again, you would get a probability chart. Without the observation the particle isn't at any single position, instead the particle is the tautology of "it being" from the sum of all the probabilities (where it could be when observed). Bomb experiment seems to indicate that we can find out information that COULD be possible without actually it happening, which is really neat.
@@Fex. The idea of it being at all possible places at the same time before the measurement is made..is cool but ultimately bollocks.No different to placing a ping pong ball in a box and shaking it.Would you say the ping pong ball is in superposition?
@@philip851 by your hypothesis, interference pattern should not exist. A single electron can exist at multiple places at the same time and interfere with itself and produce interference pattern.
I thought the main weirdness of entanglement was the idea of no hidden variables. That is, it’s not that the two particles have correlated values the whole time that are simply measured at some point for particle A, thus implying what B’s value was all along, but rather that A and B do not in any way have those values, or have them in a non-privileged way along with every other option in superposition, and only when you measure A does B in fact take on the correlated value at that instant, where prior to the measurement it could not have been said to have that value at least not exclusively.
You are absolutely right. Entanglement is incredibly weird, I am always disappointed when people try to "demystify" it. The fact that we have a mathematical model to describe it does not mean that things that it describes are not completely in contrast to our normal understanding and preception of the world.
To be precise, the violation of Bell inequalities breaks local realism, you can keep locality if you throw realism down the drain, that is the idea that it is possible to stitch observers experiences into one global description of the universe. If all systems are quantum systems, Alice/Bob can't tell that Bob/Alice has chosen a measurement basis before they communicate their results/measure each other, and that can only be done in a way that preserve locality. That's the idea behind Relational quantum mechanics : en.wikipedia.org/wiki/Relational_quantum_mechanics.
Yeah, the weird thing about entanglement is that if one particle has the value X, and the other -X, you can in fact change the value of one to Y, and when you measure the other it will be -Y... You do not really know what is X or Y either, but you can show with an experiment they are not the same. It is weird.
@@NetAndyCz correct me if I'm wrong but, entangled "particles" must always originate locally. Then, the entangled particles are separated by an arbitrary distance and remain "connected" in so far as their properties must compliment each other. Why is this weird? If particles are really waves in a quantum field(s), then the entangled particles are really just complimentary parts of a wave which remains consistent at any distance. The peak of the wave (particle A) remains a peak, and the trough (particle B) remains a trough, always. If we measure A as a peak, of course B will be the trough, and vice versa. Why is this weird?
7:32 - is this correct, though? There's a 50% chance it gets blocked by the dud, and in the rest of the cases it either goes into detector A or detector B, with 25% chance each. Exactly the same as if the bomb were live. Unless the wave function somehow magically passes through the dud and recombines with the upper ray to cancel out...?
It was a real experiment, ofc it didn't use a real bomb, but a detector that had the same textbook use as the bomb. The dud (or detector) DID indeed allow the particle to pass through it
@@Christopher-ye6cv Isn't this then only a test about whether there's a photon sensor or not. If you formulate the experiment as "is there a photon-blocking sensor here that does something 50% of the time", it feels pretty trivial, doesn't it? Just shoot a photon through it, if you didn't measure it, it got trapped, but nothing happened.
I got a thought - isn't this just consequence of photon being a wave ? Since wave takes both paths and only collapses after interaction, it travelled a little in the other path that was'nt detected, so it can have some information about it ?
About the "weirdness" of wave functions: I think it's worthwhile to remember that wave functions are NOT the particles themselves, rather they are mathematical models for some aspects of the particles' behavior. It's easy to lose track of the distinction, but it is important. Among other things, it means that there may be aspects of a particle's behavior that the wave function doesn't model very well, and that's fine. It just means we need to understand the limits of our model. We've been down this road before incidentally. Remember the Bohr model of the atom, and how it was derived with the concept of an electron traveling in a circular path around the nucleus? The model was initially held to be correct, since it proved useful for many purposes. In fact it was based on some faulty assumptions about how electrons function, but it so happens that the math worked out pretty well anyway, and the Bohr model was accepted as the correct model. Until we understood that it wasn't as correct as we thought and discovered its shortcomings. Wave functions seem to be holding up much much better than that, and they remain a useful model. But it's only a model.
Good comment. Much of the confusing, so-called "weirdness" of QT comes from making a literal exposition out of the Statistical Interpretation of the Wave-function ("Nature is Uncertain/Indeterministic"). If we regard the Statistical Interpretation as it was first set-out - in Max Born's 1926 letter to Einstein - it is merely a pragmatic, absolute limit on empirical observation, not a statement about the Nature of Reality.
@@donthesitatebegin9283 Well said. And, I suspect that some ideas (like the Many Worlds Interpretation) start with the mistake of confusing the wave function with reality. Maybe there are a billionty jillionty new universes created every nanosecond, or MAYBE it's simply that our model is imperfect. I know which one I'm leaning towards.
Well, wave-particle duality is not weird, it's misleading thinking that only one entity is involved with two roles; one a diffuse and wavy but at the same time compact. The way to see this is to visualize two entities that coexist together, one the wavy quantum package space and the other the compact particle that exists inside the package. This existence changes aleatorily inside the package between valid solutions, on each fluctuation only one eigenstate express. Now, over time the quantum package will have inside a probabilistic distribution of all the particle eigenstates i.e., Psi wavefunction describes space fluctuation but particle physical values depend on a probabilistic distribution of particle existence. So, taking Psi one will conclude that the position will be where it exists, momentum will be where the particle exists, energy will be where the particle is, and so on... all the parameters are developed by an operator over the existence Psi... weirdness has diminished
some people view the wave function as something like a physical wave that pushes the particles around. this interpretation is as valid as any other, unless we find something more fundamental about reality
@@heliusuniverse7460 Yes, but two entities that coexist together solve wave-particle duality, it also explains how communication is achieved in entangled particles, besides, it solves the trajectory problem between eigenstates, explains the collapse situation, and eliminates superposition ideas of simultaneous existence of all the eigenstate with the plausible ultra-high oscillation between them, one at a time idea... many fresh ideas that can be read in a short amazon book "Space, main actor of quantum and relativistic theories."
I don't think the issue is ripping the photo in two and shipping one to New York. The issue would be if you threw one of them in the shredder and the other *instantly* shredded too. That's what Einstein thought was spooky, and he was right.
I have the DEFINITIVE solution to the Schrödinger's cat "paradox" I can with significant statistical certainty say that after 10 weeks in a box THE CAT IS DEAD. This is empirical evidence after a hell of a lot of boxes (and cats) and you can skip the whole "radioactive" part of the experiment, it makes no differense
Thank you Sabine. I'm an utter layman and if not for your videos, I very may have fallen into the "quantam woo" trap. You are doing an invaluable service with your videos, it cannot be overstated.
I disagree with her re entanglement. Check it out for yourself. She over simplifies entanglement. I more or less agree re the quantum eraser experiment.
Your channel is wonderful, a much needed counter to the Deepak Chopra type folks who keep misusing Feymans's "nobody understands quantum mechanics mechanics" statement. Also- I never had heard of the bomb experiment till this time. You are a true educator in the finest way.
I tried to understand that experiment earlier, but couldn't wrap my head around it. After your explanation, it is much clearer (but still totally weird). Thank you (again) for being such a great teacher!
@@WeirdMedicine I don't know what you mean by "debunked". This is simply a boring like drying paint physics experiment which doesn't tell us anything about quantum mechanics.
It would sound less weird if you had mentioned what being a dud means, i.e. there is no functioning detector in the "bomb" path. So the weird thing is that the presence of a detector, or anything that can interact with the photon, leads to the change .
Maybe talking about bombs is distracting, but that's the way the original paper described it. For experimental purposes, using a detector that may or not interact with photons works the same.
If I understand the point correctly, what is being described here is essentially the same as the double slit experiment where the attempt to detect which slit the particle went through results in a corruption of the wavefunction such that the interference pattern no longer appears. Which I think is perfectly understandable; introducing "detectors" in the path of the interaction most certainly modifies the wavefunction of the overall physical arrangement.
@@kenlogsdon7095 Sure, but the difference here is that in the double slit, the detector interacts with the particle, or at least could potentially interact with it. Here, we have it setup in such a way that even if the particle never goes on the path that leads to the detector (and thus shouldn't possibly have the information of its existence) and yet it behaves differently *anyway* simply because it could have interacted with it, even though it didn't. That's what is the crazy thing. The particle somehow knows if it's live or a dud before it interacts with the bomb and changes its behaviour accordingly.
Given that a single particle will exploding the bomb, how does a single particle tell you anything? A detection at B means the bomb went off, which is the same info you get from just trying to set it off directly. A detection at A tells you nothing.
My brain can tell me something that didn't happen, which is, understanding this lecture. Whenever I think I'm overly intelligent, I simply watch a video on this channel, and I'm immediately brought back to reality.
@@Goldenretriever-k8m LMAO same, by the time I finished the video the inside of my head was just like ????????????? If you scanned my head right now you wouldn't see a brain, you'd just see an endless question marks filling up an otherwise empty skull I came to the comments hoping to find an ELI5, or at the very least, reassurance I found the latter so I'm content.
Too many incoherent interpretations in QM. Nature doesn't work with probabilities and uncertainty. The only reason we tolerate all those speculations is the fact that they assert to have more or less 5% knowledge of the functioning of the universe; so, not bad for the superior beings of a small planet called Earth.
It's a bit weird to say, "it's not weird, it's just counter-intuitive." Counter-intuitive is a plausible definition of 'weird,' and since quantum mechanics also violates long held, informed suppositions about physics, it seems counter to even informed intuitions. To then say you can't even imagine what would satisfy the equations, but it's not weird... I'm having a hard time imagining what 'weird' must mean.
Nothing is intrinsically weird or not weird. Things are what they are. We can put whatever labels onto them that we want but nature doesn't care what we call things.
Yes Bubba, even more... one can say all valid solutions are almost classical (eigenstates). The great difference with classics is that quantum existence is in an oscillatory situation with a frequency depending on its energy. The other great difference is that on each fluctuation, nature doesn't have defined information on which solution is, so it will assume aleatorily a temporary valid solution (one eigenstate per fluctuation). These two quantum realities are the so call weird QM; not just... because we can imagine a world with these two additional conditions over the classical ones. Hope this will reinforce your comment, regards
Maybe she thinks of "weird" in physics as something that defy explanation whereas "counterintuitive" would be something that have an explanation that seems illogical to most people. I don´t know, but her language would make more sense if she defined it that way.
Will, I think that some words as weird just express a reaction that gives interest to the reader to continue... the important issue is the reasoning in quantum world, how we must adjust it to the real nature atomic behavior and not only with the classical experience.... the arguments over just a sensational word.
If there is a "bomb" (detector) in the lower path, and it's live but doesn't go boom, do we really know that the photon takes the upper path? Could it not be that photon is still taking both paths with 50% probability, but that the detector, even if it does not go boom, disturbs the anticipated interference pattern, so that the photon has a 25 % chance of being detected at A and a 25 % percent of being detected at B? Not because the photon "took the upper path" - (in some clear sense as if it was a classical setting), but because the interference pattern is disturbed?
I'm trying to wrap my head around this and I'm struggling. A - Assuming the bomb is live: A1 - In 50% of the cases the bomb won't blow up, because the beam takes the upper path. Therefore the beam splits into 2 possible paths in the second beam splitter, with 25% of the cases ending in detector A and the other 25% in detector B. A2 - In the remaining 50% of the cases the bomb blows up, because the beam takes the lower path. And in this video it isn't made clear what, if anything, is detected in A or in B. Are we assuming that the bomb "absorbs" the beam when it travels to it, therefore blowing up, and ending the beam's path right then and there (both detector A and B will have nothing)? Or is the bomb detecting the beam in such a manner that the beam resumes it's travel in a similar manner as in A1, therefore splitting again into 2 possible paths with 25% ending in A and 25% ending in B? This is Important to know, because it implies how the bomb should influence the beam's behavior in the case where it's a dud, as I will explain below. B - Assuming the bomb a dud: B1 - In 50% of the cases the beam takes the upper path. In this case, it should split into 2 possible paths, being detected 25% of the cases in A and 25% of the cases B. B2 - In the remaining 50% of the cases the beam takes the lower path. Now it's important to know how exactly the bomb is detecting the beam in A2, because the way the bomb detects the beam has to be the same in both cases, or else the experiment doesn't make sense. Again, is the bomb "absorbing" the beam, therefore nothing appears in A and B. Or is it measuring the beam in such a manner that the beam resumes it's travel? In the way that this video presents it, it leaves me believing that the bomb measures the beam differently depending on it being a dud or live. If that's not the case, then for this experiment to make any sort of sense to me, the beam alternates between having a fixed path (no recombination) and possible paths (that recombine in the second beam splitter) depending if there is a reactionary element (live bomb) in the midst of one of it's paths. The beam "knows" that there is a live bomb measuring it, and therefore changes the way it travels from the source to the possible destinations. On the case where it's live, it rejects recombination, but when it's a dud, it accepts recombination. If anyone can help me see what I'm missing here, I would greatly appreciate it.
To get this I think you need to know the phase shift of the photon at beam splitter and why in dud case you can't see detection in both A and B (Hong-Ou-Mandel effect). What I understand is that the experiment uses single photons. At the first beam splitter this single photon enters superposition. It is going both ways (lower and upper pathway), acts like 2 photons! Beam splitters cause phase shift to photon and the arrangement is such that destructive interference is detected in direction to B (i.e no detection). Constructive interference is detected at A. So, if there is nothing in lower or upper pathways, then the photon is always detected in A (dud bomb can be counted as nothing). If there is live bomb in lower pathway, follows 3 different possibilities. - No detection at all means live bomb detonated and photon "really" went lower pathway. Why no detection in A? Must be because bomb itself acted as an observer and caused the superposition to collapse (i guess) - Detection at A: Photon "really" went upper path and when in second beam splitter it had 50/50 chance to be observed in A or B. This scenario is indistinguishable from a dud bomb by the way. - Detection at B: Photon "really" went upper path and again at the second beam splitter it had 50/50 chance to get detected at A or B. Detection at B can only happen can in the absence of interference! Detection at A means bomb is a dud at 50% probability Detection at B means bomb is live ad 100% probability Detection at B means we know that bomb is live even tough we never went to peek there!
Hmm, you mean no bomb at all at start and then putting a bomb midway at lower pathway just before detection is made? I think it's giving result for the original setup. I mean changing "post photon" setup does not affect detection result. Like pouring oil to a racetrack after race car has passed does not affect it. I might be wrong...And thanks for reply!@@Jhakaas_Jai
The thing I don't understand is that why the beam splitter split the photon into two for the dud but doesn't split the beam, instead only create one path for the live.
@@edward3190 Hi! Photon enters superposition when passes 1st beam splitter on both cases (live or dud). After beam splitter the same photon goes both upper and lower path. Dud case is easier to understand. Live bomb case is harder. I understand what you mean (why no explosion always if photon goes both ways as said). In live bomb case we sort of look back what really happened. Detection at B happens only in the absence of interference (no photon lower pathway). Detection at B kind of destroyed photon in lower pathway, so is it influencing backwards in time? There is many world interpretation, but that, I think, makes problems for dud case (we should then see also detection at B 50/50, but we don't, so photon must really go "both ways", not one way in this world and other way in other world). I have not seen good fundamental explanation to this detection at B case. I am a layperson.
Thanks for the video. Brilliant experiment! It illustrates the power of the quantum wave function to describe the real world. I have spotted a trend in QM: anytime there is a disagreement between the math of the wave function and our intuition (or other ideas), the wave function wins out. In Ψ we trust.
This is a great example of Sabine thinking like the highly trained physicist and mathematician she is rather than like the ordinary person she is addressing. "Weird" in this context means essentially that we don't know what it means (which Sabine recognizes too), but we ordinary folk can't help but still try to make sense of what it means *in non-mathematical terms* and when we try to do that we fail. Sabine, I suspect, is so at home with the mathematics that she does not need to "make sense" of it in non-mathematical terms. "Weird" is just this tension between the ordinary person's inability to make sense of such things as superposition in concrete terms and their impulse to still try to make concrete sense of it. The fact that such things can be handled perfectly simply (and non-weirdly) in mathematical terms does nothing to take aware that weirdness. When ordinary people try to make sense of superposition they are not thinking of it as the addition of wave functions - they are wondering what that addition of wave functions in the equation represents concretely in the world. "I think I can safely say that no one understands quantum mechanics". - Richard Feynman. That's why it *is* weird.
The odd thing is not that the we gain knowledge about a path not taken, the odd thing is that the behavior of the photon changes at the splitter depending if there is a bomb and depending on whether it's live or not. If there is no detector, it seems to take both paths, if there is, it takes only one of them. That's the only odd thing here and it may not be really odd if we one day find out what space really is. Consider this: Space is not empty room, it consists of threads and energy traveling through space must travel along one of the threads. E.g. energy always is a wave on a thread and thus it can only travel along a thread. For simplicity, ignore that threads may join, split up, be bend, or many threads may be knotted together. For a photon arriving at the splitter, there are two threads its energy could take; so it could take one or the other one or it split up and part of its energy could go either way. Nothing odd so far. But what happens if you put an active detector in its path? How about this: An active detector changes the tension of the thread that it interrupts or forces to "go around it". This change of tension is detectable all the way back to the splitter. If now a photon arrives at the splitter, there are two threads it could take, but unlike before, these threads don't have an equal tension level anymore, their tension level is different and the photon can detect that already at the splitter, long before will hit any detector. This may change things a lot and maybe different tension levels, or let's call them stress levels force a photon to make a decision to take one thread or the other thread, as it will only split up if the stress level of both threads is equal. It's like an electron in an electric circle getting to a point where it can either pass through a 100 or a 200 kOhm resistor. It will have to make a decision which way to go as both paths will be used, even though the 100 kOhm one will be used a lot more. How it makes that decision? Sure, that would still be a mystery. I'm talking about the photon here, we know it for the electron. And an electron will also not split up if both paths are 100 kOhm, so the photon behavior is different here but adding those threads (or paths or whatever you want to call them) to the mix and giving them a stress level, it's less spooky that the photon changes behavior at the splitter depending on whether there is an active detector or not if only an active detector changes the stress level. How is an active detector different from an inactive one? How about that: An active detector forces energy, at least certain kind of it, passing by to interact with it, while an inactive one would energy just allow to pass by. Maybe anything that is reactive to at least some form of energy changes the stress level of a path and as path may not be limited in length and could spawn from one end to the other one of the universe, assuming for a second there is such a thing as an end, this could influence the behavior of energy that could take this path and is million of light years away from us. In reality these threads would rather by a super complex asymmetric 3D grid, you could also say a field and this brings us back to quantum field theory. If our universe is made up out of fields then an active detector would just change these fields in some way and this will change how energy is traveling through these fields, wouldn't it? And from that perspective, I don't think this experiment is weird at all. It's not intuitive to us as the world we live in is full of detectors. E.g. there is matter all around us pretty much all the time that will interact with photons and thus behave like a detector. The stress level of all possible paths is pretty much always different and that's why we see particles only taking distinct paths in our world. Yet that is like if someone who was born on an island completely covered by forest and who also staid there his entry life would believe the entire world must be covered by forest which isn't the case but that's how the only world he knows and has ever seen.
I didn't understand the bomb allegory until realized that the "dud" bomb does not detect anything IE it does not exist. And the live bomb is detecting the electron. Thus decohering the system. So all the thought experiment is doing is detecting the presence of a detector in one of the possible paths without triggering the detector....25% of a time.
@@adamjondo The dud could simply take the signal and reemit it and the entangled photon would be retarded. Depending on the inherent delay in that scheme, it would not be measurable and so 'nothing happens'. Thinks... a Fresnel rhomb would pass the electric field and absorb the magnetic component, such that the emission is colinear with the source. Such a system existing in the path of one of two entangled beams would retard the phase of both of them due to inductance at the source (not magical or instantaneity (which still introduces a phase shift, a problem for single photon interference), simply inductance). Failing that a Fresnel rhomb could be introduced into both paths. It would take a long age explain just how rigged it is in the favour of generating the paradox, but you have to give them credit for putting in the work. Then why does the live bomb collapse the wavefunction? it doesn't explode. So 'nothing happens'. It can superposition. All the jack-in-the-boxes have been defused and can only be sprung by a trainee.
Thank you! I first learned of this a couple years ago, and I have periodically read the wikipedia page on it multiple times since then, but I was never able to properly wrap my head around what actually is happening in this experiment. Seeing the process built up step by step finally made it click for me!
If you understand QM, it is easy. If you do not know QM, it is genuinely weird. It represents a kind of non-locality different from EPR, which is not really that weird. It is based on correlations. Interestingly, EPR shows that QM does not obey the ordinary rules of probability as Bells Theorem showed (amongst other things).
@@nikoszaronakis1862 Many, many people understand QM. But there are many different interpretations of what it means, largely IMHO because we do not have direct experience with the Quantum World, so do not have an intuition to guide us. It is to emphasise this non-intuitive nature that some come up with such thought experiments - they understand very well how QM explains it. Remember, QM is a model of the QM world, a map if you want to use that sort of language, but as the saying goes - the map is not the territory.
@@bhobba Thank you! So they understand how it works (which I don't fully) but they don't understand why it works that unintuitive way (so there comes interpretation). But it seems like this experiment doesn't add to what we already know about how QM works. To me all these experiments sound like "what would be the analogue of QM behaviour in the macroscopic world and are there really any interactions/ impact on it".
@@nikoszaronakis1862 The way I look at them is to hammer home you can understand something and know why it works, but it still is weird. That occurs not just in QM but in many other areas as well. Take 1+2+3+4...... Any ninny can see it is infinity - but believe it or not, it is -1/12. I know why (it boils down to something in complex analysis called analytic continuation without going into the details), but it is still counterintuitive and weird. The root cause of the problem here is we make an unwarranted assumption the integers are just part of the real numbers - in fact, they are also part of the complex numbers, and powerful theorems from that area of math can be used. So one reason for these 'experiments' is to flesh out the unwarranted assumptions you are making.
This is second part of Entropy, which includes entropy in terms of arrangement and probability. Suppose there are three color balls, r(red), g(green), b(blue) arranged in three places available for them. So they arranged like; rgb, rbg, bgr, brg, grb, gbr. There are six ways in which they can arranged this is permutation. If one more different color ball or place is added, pernutation or number of arrangement increases to twenty four, that is four multiply to six previous arrangements. Now as there is no preference of any arrangement and all are equally likelihood, so probability of any one selection is 1/6. Thus we see that probability of any selection decreases with increase in permutation or arrangements, and which is related to number of particles or participants which is ball in this case. Decrease in probability is increase in uncertainity or randomness or chaos. Now if in above case if two of ball are of same color, suppose there are three balls of two colors r(red) and b(blue). Then above six arrangements reduces to three; rbb, brb, bbr. So when particles becomes indistinguishable, permutation or arrangements decreases and thus probability of any one arrangement is increase. This type of permutation is equivalent to combination of choosing two balls from three balls of different colors. Probability distribution function of maxwellian particles which are considered as distinguishable is given by suppose, 1/X. Where X is permutation of particles. Similarly permutations of fermions and boson are X+1 and X-1. Both fermions and bosons are considered as indistinguishable particles but their probability distribution function is higher than maxwellian for boson is okay but lower than maxwellian for fermions shows that fermions are distinguishable particles and that is indicated by their spin half property which is basis for exclusion principle. Does there are three kind of particles, two of them are governed by quantum statics or there is one kind of particle given as classical one and there are three kind of distribution density states. Suppose permutation of particles having given higher energy is X, then its probability density function is given by, 1/X. This is known as Maxwell-Boltzmann distribution function where it gives probability of a particle having given energy at temperature. On increasing temperature, probability of particle having given energy increased. Probability of a particle having given energy is 1/X and probability of a particle to not have given energy is, 1 - 1/X or (X - 1)/X. Now ration of a particle having given energy to a particle not having energy is, 1/(X - 1). This is known as Bose-Einstein distribution function and it tells about probability of a particle to have given energy if there is no particle have that given energy before or say ratio of probability of a particle to have given energy to go higher energy level to release given energy to come back to lower energy level. In textbooks it is interpreted entirely different. Again probability of a particle having given energy is 1/X, and probability of another particle to have that same given energy is, 1 + 1/X or (X + 1)/ X. Now ratio of a particle having given energy and another particle to have same energy is given by, 1/(X + 1). Thus the probability of a particle having same energy as by another particle is decreased to if that energy is not occupied. This is known as Fermi-Dirac distribution. So we see that there are no more two other kinds of particles obeying quantum statics but conditional probability distribution of same kind of particles.
I was following for a while but the grammar got me confused at the end >< are you saying that the particles have to be distinguishable, because if they weren’t, you could lower the probability distribution by having particles change into different particles?
Neil you are clearly very intelligent and your point seems good but the detail is lost because of grammar twists and turns.. if you could rework it … well I’d love to try to understand cause i think i know what your saying but its just not so clear for me to really get it…. Appreciate.
@@5ty717 May be my words stumble because I want to write in brief and second thing, to write against established conception is difficult due to people misunderstand that I lack understanding. Also this topic is tedious.
"If the bomb is a dud, nothing happens. The photon splits, takes both paths..." But surely the bomb (or its detector) would still block the photon even if it's a dud?
In the scenario of the article, with a 100%-efficient 100%-absorbing detector in one of the arms, the odds are: 25% D1 clicks (let's say D1 is the detector that always clicks when there is nothing in the paths), 25% D2 clicks, 50% neither D1 or D2 clicks and the photon is absorbed in the bomb's detector. Forget the bomb, the scenario is about what happens along the photon paths and tells us nothing about the quality of bombs eventually wired to a detector along the photon paths. In fact, the "detector" itself might be damaged and it doesn't register anything. We have no information about this by the click in D2. What we know is that the state of the photon has been altered by the presence of something along the paths, at least one of them. Could be the lab assistant's elbow.
@@ThePinkus Yes, I realise it's not about the bomb. But the detector would still block the photon no matter if the detector works or not. Why does she say "If the bomb's a dud, nothing happens"? 07:27 I guess she should have said "if the bomb is not there..."
@@Tom_Quixote I rechecked the article to see if I was missing something before answering. Btw, You can find it on arXive, though I am not posting the link since the last time I did YT deleted my comment, or at least that was the correlation between link and deletion...why!?!? The authors specify the sense in which the bomb is a dud at page 8 of their article. A bomb is a dud when it doesn't have the detector that would absorb or scatter (prevent it to go on through the interferometer) the photon, so, they mean "dud" = "no obstacle". When "dud" means just that, then the reasoning goes on as described. Ok, in this way it makes sense. You made quite the right question. No other type of "dudness" can be detected by the apparatus, so it is very important to make this clear. Thank You for asking!
@@yecril71pl I am of course well aware of it. ;) That is why the authors of the article take care to explicitly state that by "dud" they mean just that, so that they can make the subsequent reasoning. They also are explicit on the fact that all of the bomb narration is just a dramatization of their reasoning, and I would add, so that it is not relevant. It is totally obvious that the apparatus does not divine the quality of things in the common sense of parlance, but it only detects an obstacle along one of the paths. So, given that the article is written in that manner, if we don't specify that by "dud", in this case, we have to intend nothing else than "no obstacle" we cannot follow their reasoning.
IIRC the success chance of detection without going boom can also be boosted quite a bit with more elaborate setups, right? (Though the chance that the bomb blows up in your face can't be brought to 0)
Adding more beam splitters after the bomb part should do it. Each time the photon splits and moves the direction or A or B2. Put a bunch of beam splitters (n) and the chance for the photon to always move to A is (0,5)^n. I could be wrong.
@@leolafortune1255 I think once you do the split, the particle will always take the same path in subsequent splinters. It's like a particle can have a probability less than 100% to be in a certain location, but after you measured it there, you can be certain that is where it is and it's not going to jump to one of the other probabilities in a later measurement.
What you want to bias the setup for is a situation where the probability of the photon to go to the bomb is near zero and the probability of going to the detector B when a bomb is live to be near 1. This requires more beam splitters in series before the bomb to increase the probability of the photon not blowing up the bomb. Then, when we go to where the beams recombine, we can sum all wave functions and get something converging on 25% and 75% for B and A respectively. To further increase the accuracy would require increasing the number of times you sum "the path not taken" - and I don't think there is a way to do this. You simply reduce the odds the path taken is the one that blows up the bomb and allow for multiple sample cycles - if you shoot 100 cycles and don't get a response from B or an explosion, then you have whatever the probability of flipping a coin with a 75% chance to be heads is 100 times and getting only heads. Or... 74.999x - or whatever the probability has been reduced to. I think ... It may converge on 50/50, but I don't think so. Bear in mind I have had no formal education or experience with this; I am well beyond my math.
Of course, if we take the suggestive scenario too seriously, the better strategy is to detach any explosive or otherwise dangerous part from the apparatus, since the experiment doesn't really tell us anything about their quality.
I thought "entanglement" was different from a ripped photo because the particles don't decide which property they have until they are measured. IIRC there was an experiment where you measure spin axis direction which shows a result different to the expected result for a "ripped photo" example.
The quantitative results are different because we aren't dealing with objects, but the basic idea about entangled pairs, be they classical or quantum mechanical, is fairly similar.
@@daanschone1548 There were already no hidden variables before Bell. The entire idea of hidden variables is just one big intellectual mistake. The point is that entanglement is the consequence of conservation laws and those are the same for both classical and quantum mechanical systems.
@@schmetterling4477 sounds logical. The entangled particle has the opposite state of the other and conservates energy etc. But do you think the outcome of measuring an entangled particle in quantum state is pre determined? Because that is what the photo analogy suggests. And that differs from what I understand of quantum states.
@@daanschone1548 A quantum mechanical measurement outcome is not fully pre-determined. We don't need entanglement to see that. When an individual unstable nucleus decays is not predictable but the average decay energy is. In case of a pure spin (1/2 or 1) state the spin projection statistics depends on the orientation of the measurement device, but there are angles at which all outcomes are either up or down. So, no, the quantum system does not carry all the necessary information about the measurement outcome, but it carries some. This is all fully expressed in Copenhagen, already.
Isn't this equivalent to putting a wall between the first splitter and one of the mirrors? It also deletes one of the paths and prevents destructive interference. Also, are we experimentally sure about the premise to the experiment, aka that it would only activate detector A without the bomb?
Yes, this is exactly the same result as the classic double slit experiment except the output is binary not a distribution. The weird part is that with the entanglement apparatus described by Sabine you can perform stuff like nondestructive testing on a sample. Using Sabine's example and assuming 50/50 live vs dud population of bombs, you can separate 25% of the live bombs from a mixed population on each pass (meanwhile 50% will blow up and 25% will remain in the mixed population, which can be sampled again). This could have major implications in many areas of science,.medicine, computing, etc.
@@everfree2532 Superposition is a sum in the sense that two entangled states are combined to represent the entire system. Consider a simple oscillation (as a.proxy for the wave function); a superposition would mean the single oscillation is divided into two (or more) oscillations that can be added back together to derive the initial oscillation. Without a "live bomb", they are always added back together. But the presence of the live bomb sometimes "collapses" the wave function whereby the divided oscillation cannot be recombined, and this fundamentally changes the observable behavoir of the quantum object that the oscillation defines (in this case, a photon).
if i understand correctly, the dud is like empty space and does nothing. the bomb is like a detector and a wall and collapses the wave function and destroys the entanglement. this seems similar to the interference pattern disappearing when you introduce a measurement into the double slit experiment. i think you could do something similar rig a bomb/detector or a dud-nothing to the double slit apparatus. if you detected a photon in the "dark" region of the interference pattern you would have a much better than 50% confidence that there was a bomb/detector attached to the apparatus. if it was in the "bright" region of the interference pattern, you might get into a monty-hall style debate about whether there was a still 50% chance the thing was a dud.
A common confusion with quantum mechanics is people are taught to view particles as a point like object, which there is no evidence for. Hence wave duality "paradoxes". In reality they are more like fuzzy balls that can spread, which explains why an electron can form superposition bond with two protons symmetrically apart, as it spreads. We cannot assume every mathematical description has a realistic counterpart.
Elementary particles are point-like in a certain sense. The probability function is not the same as the particle being spread out. You can actually tell the difference. There is something called a form factor in particle physics which accounts for extended structures of particles. The electron has a charge, and when a particle interacts, the way it is deflected depends on whether the charge is spread out, or located at an infintessimal point in space. It's mathematics, so I can't really explain it any better than that. It is one of the reasons we know that electrons are point-like, but protons are not.
@@alienzenx There is absolutely no evidence that it is located at an infinitessimal point in space and it's not necessary to interpret it that way from the mathematics, please refer to "No Evidence for Particles" by Casey Blood to see the myths answered surrounding the conception of particle.
That's not true. Experiments in colliders have given an upper bound of the size of the electron, and it is much smaller than a proton, _a fortiori_ of an atom. The corpuscular aspect of a particle is that if it is observed (as a point say) at a position, it can't be observed at another position. When the position or the momentum of an electron in an atom is measured with a good enough precision, the atom ceases to exist.
@@JL-fh4qw We can never measure with infinite accuracy and there are fundamental physical limits to what can even be theoretically measured. Never-the-less, the electron is as far as we can tell point-like, and the spread of the wavefunction is not the same as the particle itself being spread out. The wavefunction has a finite value at every point in space, so you would have to consider particles to be of infinite size.
I'm not a physicist but I've watched a video talking about some scientists proving Einstein wrong in that there are no hidden variables in entangled particles, so wouldn't that mean that even if the correlation between the entangled pairs was locally created, their future states should not be dependent on each other (but they are)?
It is attributed to Einstein that he thought quantum mechanics is not complete, and a more complete description would entail further variables. But we don't exactly what he meant since his famous paper was written by one of his students, and of course he has a more subtle take. He saw what nobody then saw, and in addition he was essential in the discovery of quantum mechanics. Since then there have been the theorem of Bell and the experience of Aspect that showed quantum mechanics is complete. But that doesn't mean it is right. Actually it is weird and doesn't fulfill the criteria of a scientific theory.
That’s correct, the Bell theorem experimental results prove (independent of any possible theory) that there can not be any local hidden variables that would reproduce the correlations predicted by quantum mechanics. Sabine’s analogy of tearing a photo and sending them off, is not in accord with QM,… which is to say, it is invalid to presume that the measured attribute/results exists before a measurement is made. [The act of measurement supplies the conceptual form, as a condition for observability,…. so the attribute is created at observation]
It took me ages to get my head around this. You did say ‘when the bomb is live and it doesn’t explode then you know the beam is in the upper portion only. I couldn’t see how this extrapolation would in its self collapse the wave function and I had previously thought that detection and collapse of the wave function only worked positively ie when you observe you see a distinct discrete position. I didn’t realise that a negative observation (nothing observed) also collapsed the wave function to an alternate discrete location.
I was thinking about it the other way around, like, it is the (theorical) collapse of the wave fuction through one path that results in a negative observation.
"The photon goes through one path, so the results tells you something about the path it didnt take"... i think it is the change in the wave fuction that actually causes the result, so i would say it is the wave fuction that tells you something about the possible path it could've taken
If you're still having trouble figuring out why this is better than a coinflip (after all it still explodes 50% of the time), think about the problem this way: we want to test if the bomb is live so that we can store it for use later. In classical physics this is impossible, there is no way to ensure that the bomb is live without blowing it up. But in quantum mechanics, using the method shown in the video, there is a 25% chance it will NOT blow up but we WILL know that it's live.
But I still don’t understand even from the video why we know it’s live. It seems like she is saying that the beam splitter in some cases directs the photon in one direction vs the other and in other cases it splits it into two (half photons? Different type of of photons?) and half a photon won’t blow it up?
@@JayMutzafi Yes, this is confusing in the video because of some of the words she uses (splits/beam splitter/recombines). If I understand it correctly, it's not a beam "splitter", instead it causes the photon to choose a direction with a 50% probability. The superposition property allows the photon to interfere with itself at the second "splitter" so if the bomb isn't detected the probabilities of travel (+50/-50) add back up to direction of travel to A. If detected by the bomb being triggered, the superposition property of the photon is removed and the photon is then forced to choose a path at the second splitter with 50% probability once again. In my mind, this still doesn't explain the superposition property.
Yeah it took me 2 hours to figure this out because half of the key terminology Sabine used in this video were misnomers. While beam splitters tend to be used in the context of splitting up a photon, in the video it is used to indicate a split in the photon’s decision tree. At least per my understanding. This material is still too advanced for my head to wrap around properly at the moment 😅
What is she on about? The weird thing about entanglement is that the particles seem to interact with each other instantly faster than the speed of light. Isn't that what they mean by non-locality?
After watching the 'bomb' experiment several times, it appears to be an equivalent of the double slit experiment if having two clear paths makes detection at 'B' never happen, even with a single photon. Definitely goes against how I always thought a beam-splitter worked; one path or the other with a probability (50-50 in the example shown). If equivalent to the 'double-slit experiment', then any detector (bomb or otherwise) placed in the lower path will cause detection at 'B'. It would seem that the experiment is only telling you that you are attempting to determine the path.
@@larswillems9886 there is no classical counterpart to a detector. There is no way to destroy the coherence of a classical wave in a two-slit experiment without closing one of the slit. In the video, both “slits” are open (it is just one of the slit has a detector) but still the coherence is totally destroyed.
If the wave who goes trought the uper path hits the second beam-splitter a long time before the wave who goes trough the bottom path hits it, then should we expected the detector B lights up (with 25% chance of happen) regardless what happens in the bottom path?
What you described was classical superposition; it would be disingenuous to call quantum superposition just 'simple addition and not weird when it has extra properties due to the matrix math involved which makes the 'simple addition' non commutative.
I don't remember addition of wave functions being non-commutative. I only remember that the product, which is what expresses successive measurements, is non-commutative. That is also the case for generic (square) matrix math.
In science, any interpretation is only an analogy and nothing more than that, as long at it is trying to communicate more than the experimental facts. And interpretation will, more often than not, bring much more to the table than just that.
Yes, this is a good example of how mathematical physicists interpret the world. Unfortunately, when they do this, they give us incredibly bad ideas, like Quantum Computers, based on the mathematical idea of the superposition of "Quantum States." Math should be applied to physical reality, instead of creating new fantasies about nature and then using propaganda to get people to believe in these fantasies.
Can someone tell me how the 2nd beam splitter results in constructive interference to detector A, but destructive interference toward detector B? What is happening at this beam splitter to cause the light to not come out the top?
Phase shifts occur when light is reflected on the front side of a mirror. This is described by the Fresnel equations. See the Wikipedia article on the Mach-Zehnder interferometer, for instance.
@@MrCrystalm8yeah, and because of thst i asked why a hundred times, than i tried to explain why could that be, i think it's because if the photon reflects at the beam splitter nothing happens but instead if it goes through the splitter some properties of the photons change
Sabine says: “There’s nothing intrinsically weird about (quantum measurement), people just think there’s something weird about it because they have beliefs about how nature should be.” I say, "Maybe, Sabine, but the greatest physicists of all time would not have agreed with you: They would say that there’s really something weird about it. Niels Bohr: “If quantum mechanics hasn’t profoundly shocked you, you haven’t understood it yet. Everything we call real is made of things that cannot be regarded as real.” Richard Feynman "I think I can safely say that nobody understands quantum mechanics." (Statement made the year he won the Noble Prize for work in quantum mechanics) Wojciech Zurech - one of the theoriticians of decoherence “Reality is what we agree on. In that sense, it’s what’s invariant. But that invariance-and hence quantum reality--is not fundamental. It’s emergent and approximate.” Roger Penrose: “Somehow, our consciousness is the reason the universe is here.” Bernard d'Espagnat - French physicist and philosopher and researcher into the philosophical foundations of quantum physics . "The doctrine that the world is made up of objects whose existence is independent of human consciousness turns out to be in conflict with quantum mechanics and with facts established by experiment." Werner Heisenger (German theoretical physicist and director of the Max Planck Institute for Physics and Astrophysics from 1960 to 1970): "The idea of an objective real world whose smallest parts exist objectively in the same sense as stones or trees exist, independently of whether or not we observe them ... is impossible." David Albert and Rivka Galchen: “We believe that everything there is to say about the world can in principle be put into the form of a narrative sequence of propositions about spatial configurations of the world at specific times. But entanglement and special relativity together imply that the physical history of the world is far too rich for that.”
Hi Sabine, I am confused about something from your video. When you first start the bomb experiment, you imply that the photon has a 50% chance of going to the top path and the bottom path, but then you only show the results of the photon taking both paths at the same time. In the case where the photon takes both paths at the same time, the split photon will either interfere with itself destructively (nothing detected) or it will interfere with itself constructively (detected only at A). My first question arises here. Why is it that it is only ever going to detector A when it constructively interferes, yet later you imply that if the photon makes it through only the top path, there is an equal chance that it is detected at A or B? Next, you show the bomb scenarios where if it is a dud and the photons go through both the top and bottom paths, the bomb doesn't explode and therefore we should get a detection at A, same as if there was no bomb. When you add the live bomb, somehow the photon is allowed to take only the top path, which makes it possible for the detection at B. As far as I can tell, this has absolutely nothing to do with the bomb being live or a dud. It has everything to do with the inconsistency between two variables. First, whether or not the photon is allowed to take only one path, or if it has to take both paths. If it is allowed to take only one path in any scenario, then if it takes the top path only, you will get the same result whether the bomb is live or a dud, since there is no photon at the lower path to determine if the bomb would explode, and no lower photon energy to interfere with the upper photon energy prior to detection. Second, it makes no sense that the energy making it through the final splitter only has a chance of going to detector B when it only takes the upper path. If energy going through has a 50/50 chance to go to detector A and B, then the entire nature of the experiment changes, and it should have a 50/50 chance of being detected at B when it is constructively interfered with after taking both paths. If the energy going through the final splitter doesn't have a chance of being detected at B when it is taking both paths and is constructively interfered with, it shouldn't have a chance of being detected at B when it only takes one path. If detector A only detects energy that was constructively interfered with, then it wouldn't detect the photon taking only one path, because that energy wouldn't be constructively interfered with. Either way I look at it, the results aren't based on whether the bomb was live or a dud, the results are based on when you do or do not permit the beam to take both paths vs a single path, and when the detectors do and do not have an equal chance of detecting energy that makes it through the final splitter. Can you please help me understand?
A live bomb acts as a measuring device, and takes a measurement of the photon after the beam is split. When you measure the photon, then it can only have taken a single path. But when you don't measure the photon, then the photon takes both paths and interferes with itself at the second beam splitter. Also, when the photon interferes with itself at the second beam splitter, it's always detected at A. It's not either interfering with itself destructively or constructively. It's at the same time interfering with itself destructively in the direction of B, and therefore nothing is detected at B; and interfering with itself constructively in the direction of A, therefore leading to a detection at A. Hope this clears things up.
@@Fred-gs1ur It clears up the fact that it's a poor analogy. The live bomb is being treated as a measuring device, but the dud bomb is essentially being treated as if it doesn't exist at all. Why bother including the dud bomb, then? It only muddies the water. Just give the analogy with the live bomb only. In reality, the photon could care less whether you hear the bomb go off. That would be like saying if a detector had an alarm attached to it to let you know when it detected a photon, but the alarm broke, that the photon would completely ignore the detector. The photon is detected because it's interacting with a system that changes the nature of the photon, not because you hear the alarm go off. It's silly to assume that a dud bomb wouldn't cause the exact same result as the live bomb, but it doesn't matter, I get what was intended. Thank you for your time.
A + for effort from me even though I didn't fully read your question due to you not adding linebreaks and me not understanding the explanation anyways.
you say “it’s silly to assume a dud bomb wouldn’t create exactly the same result as a live bomb”…it doesn’t create the same result. In the live bomb scenario, the photon cannot interfere with itself, and is then capable of being detected at B.
@@leif1075 This is essentially a double slit experiment. If the photon really took both paths, it will combine with itself and create an interference pattern. You place one detector in the bright band of this pattern, and the other detector in the dark band. 50% of the time it will be constructive interference and land in a bright band, and 50% of the time it will be destructive and NOT land in the dark band. If the photon only takes one path, there will be no interference pattern, and 50% of the time it'll land where the bright band would have been, and 50% of the time it lands where the dark band would have been, making it bright. Therefore, if you ever actually detect a photon in the dark band area (and that will happen 25% of the time), that means the photon could only take one path, and the bomb is real and didn't go off. If you detect it in the bright band area (50%) or don't detect it at all (25%) then you don't know if the bomb is real or not, except in the 25% of cases where the bomb does go off. If this isn't clear, imagine a regular double slit experiment, and you're placing the bomb in front of one of the slits. If the bomb is a dud, the light passes through the bomb (she didn't actually mention this, and I had to go look at the paper to understand that bit) and both slits forming an interference pattern. If the bomb is real, it intercepts the photon, thus blocking one slit, and you get a regular single peak distribution instead of an interference pattern. Though since you're doing this one photon at a time, you can only tell the difference in the patterns if the photon happens to land where normally there'd be darkness in case of interference.
@@stargazer7644 see she did NOT explain it that way in the video..sidnt thr video confuse you too..and you don't mean the photon can literally take both paths at the same time right..since it's not possible for a photon to be in 2 places at once so why did you say that?
@@leif1075 The photon can be in two places at once - it takes both paths at the same time - actually it takes all paths and interferes with itself. That's fundamental to Quantum Mechanics. That's why you get an interference pattern in the double slit experiment instead of just a band of light behind each slit. Look for some videos on the double slit experiment.
@@stargazer7644 but isn't I just the PROBABILITY that the photon cam be in one or the other path right? Think about it a photon is a tiny particle it is not large enough to be in both places at once? It's just the probabikity..the double slit interference can be due to multiple photons interfering with each other
This seems misleading. The difference between "live bomb" and "dud bomb" isn't just the explosion, but the fact that the "dud bomb" lets the photon pass through unaffected. The "live bomb" does not let the photon pass through. The results (i.e detector A&B probabilities) for the live bomb are the same as if you stick your hand in the chamber (at the same location as the bomb) to block one of the paths. In other words, by observing a photon in detector B, you know interference didn't happen because a path has been blocked. Does "information that a path has been blocked" really translate to "information about the bomb"? I'd call that misleading - the real hidden assumption is that we engineered a bomb that only obstructs the path when it's live.
Please answer this. Without an answer to this, this video just translates to "quantum mechanics allows you to tell if a path is blocked". What's weird? You can already tell if a path is blocked without quantum mechanics!
This brings to mind something that I’ve wondered about. Regarding photon emitters: Is it really possible to just emit 1-photon at a time? I believe that I read somewhere that those photon-emitters actually emit a very small quantity of them, but that technology isn’t good enough yet to emit just one.
@@SabineHossenfelder Thanks, but that phrasing needs a little correction. "... until there's only one left according to the accepted theories (in particular QM)". Is there any way to prove that there only one photon at the end without using all of our theoretical framework? Using just an intuitive experiment? That is where one can see the distance and possibly "weirdness" from our 'normal average' human experience (which are in them selves just as much assumptions). As an aside i will add that I personally do mainly agree with your demonstrated pragmatic attitude in this video. That is more like what i think as science. As for my earlier case, it is not that it is wrong to assume anything, but it is wrong to forget that it is an assumption. That is how basic logic works after all. It is just that we must work with some axioms, but that doesn't mean that they automatically apply outside our argumentation. Here the outside could be some kind of 'reality' vs our theories.
@Sabine Hossenfelder the problem is scientis made assumptions from their beliefs of how things should work and use experiments to proof their assumptins the experimets dont proof at all, actualy the experiments brings more problems, but they continue with their ideas making other teoris to try to explain the results of the experimets so when new experiments can prove those teories them think the initial assumption was rigth if I assume that 1- universe is filled with minuscle particles that are slightly repeled by electrons, the think that qe call vacuum 2- the movement of the electron produce a wave in this particles, the phenomenon that we call light 3- those waves interfer in the movement of the electrons so a lot of problems in qunatum mecanics will be solved an experiments will prove this assumptions. it will bring a lot of other problems too what it means? nothing i just think that scientists shouldnt trust so much in the outcome of experiments and the matematics.
@@estranhokonsta There are actual sources called single-photon emitters, name self-explanatory, and there are single photon detectors or SPD sometimes called single photon counters. The SPDs are different from basic light detectors which measure the flux density of light and are DESIGNED to detect one photon. The construction and theory into building SPDs goes back decades and are sold ubiquitously. Nothing tricky about detecting light. Solar panels do it. The only difference is scale. If you measure the electrical pulse you've detected the photon using whatever math to balance equation when going from what your input is "light" to what that should yield at the output: the electrical which represents a detection. Some things to note, your eye is sensitive enough to detect a single photon. Also if you're thinking of the Young Double Slit experiment just know that the same quantum results has been done with not just photons but with molecules. Last I read it was with the "bucky-ball" molecule: fullerene so I wouldn't get too caught up with dissecting the peculiarities of quantum physics with light.
Entanglement is said to be weird not because the entangled particles are simply like a left shoe and the matching right shoe each inside a sealed box and we just don’t know which is which, rather the weird part is that we have a method and choice to change one shoe to either left or right and the other shoe will always be instantaneously opposite, so reality is not grounded until observed and when observed, that information seems to propagate instantaneously (faster than light).
I am not an expert. But no "we have a method and choice to change one shoe to either left or right", we don't have a way to change one shoe to either left or right. It's just that if one shoe, when observed, turns out to be right, then other will turn out to be left.
@@abhay8437 Not true. You can flip the spin of one particle (without knowing what it was to begin with), and the two particles will still have opposite spins when observed. That is one aspect of entanglement that makes the universe not “locally real” and is pretty weird. If it helps, there is no way to check that the entangled flip actually happened until an observer physically travels to and confirms the observation on the other distant particle, so speed of light limits verification, but the flip still happens instantaneously. We have done lab experiments where we sometimes flip one particle and other times don’t flip it, and confirmed that the entangled particle instantaneously flipped to the opposite with the same probability distribution as in the setting without any flips and did so before light could have had time to travel the distance between the two particles. The above can’t be used to transmit information faster than light because you don’t know what the spin was to begin with and flipping it immediately collapses the wave function, so for information transmission purposes, the left shoe and right shoe analogy holds, but it’s an inaccurate analogy otherwise.
@@abhay8437 yeah, and what's so weird about that? I thought they were able to change the entangled particles or move them around and teleport them etc. didn't they do that with quantum mechanics? What about that?
6:44 - Why would the 2nd beam splitter always Just Reverse the effect of the first beam splitter? Wouldn't it create another 50%/50%? It doesn't know what the first beam splitter does. You are shooting a single photon, so it will go one way or the other. You are not splitting a photon into 2 photons.
This is how I understood: Those are 2 different kinds of "splitters" the "2nd beam splitter" acts as a mirror while the others are half reflective mirrors (that's why 50% goes to one direction opposed to 100% from the "2nd beam splitters aka mirrors"
Sounds like a dangerous version of what I like to call the rectangle experiment, except instead of a bomb you have an ultra-fast LCD "disk." You can set up the same thing and put the LCD in one of the paths. Now, turn the brightness down until you get only one photon at a time going through the apparatus. After the photon leaves the source you can decide whether to make the LCD opaque or transparent. If transparent, you get an interference pattern where the two beams collide. If opaque, you don't. But you can change the state of the LCD _after_ the photon leaves the source. So you can imagine a wave function with the photon going down both arms (actually in a superposition of the two). And while the photon is in transit you turn the LCD opaque. So what happens? One of two things: (1) The photon is now only in the arm with the LCD and gets absorbed. Or, (2) the photon is now _only_ in the other arm -- _after_ you turn the LCD dark. So in case two, the photon starts by being in both arms, but when the LCD goes dark, suddenly it's all in the other arm. The one on its way to the detector suddenly ceases to exist! Now recall this is a superposition of the photon being in either arm or both arms or whatever. So it's like the bomb experiment, but a lot safer!!! It's kind of like the 2-slit experiment, but stretched out to make the weirdness of it quite salient.
A quantum state describes more than just determined events. E.g., it describes correlations (in the form of entanglement). Since (quantum) mechanics is the evolution of these states, we can have a physically significant (quantum) mechanical evolution of correlations that does not entails the occurrence of any determined event. In the scenario of the article, the photon's state enters the apparatus "going through both arms", and it always "interacts", in the above sense, with the system placed in one of the paths. This is necessary for the possibility of the second detector to click, it wouldn't if the state went through unaltered. Yet, when this detector clicks it never happens together with any other determined event occurring between the photon and the system placed in the arm. In this sense, which is entirely different than the previous one, the scenario is narrated as "interaction-free detection".
@@ThePinkus Let me rephrase my question, since it seems to me that you did not adress at all: The sensor (bomb) that (clearly has to) interact with the particle does not change the particle with this interaction?
@@oceanliketeacher The interaction changes the particle state, and one could say that the particle is changed or affected while meaning just that. The particle going into the EV apparatus with an obstacle ("bomb", for dramatization I guess, but quite irrelevant what it is) is always affected/changed by the presence of the obstacle on one of its path in this sense, whatever the end result. Formally, this is probably the more correct description -- the state changes, and when we say that a particle changes we just mean that its state changes. But with this meaning, it is already impossible to give a positive answer to Your question "the sensor that interacts with the particle does not change the particle with this interaction?". By definition, the interaction does change the particle. There is no way to interact without changing the particle, in this sense (a trivial interaction that doesn't affect the particle is the identity operator, eventually multiplied by a complex scalar, but we probably want to call that "no interaction at all"). But! One might want to reserve "interaction", "change", "being affected" (and I am not suggesting that one should, in fact, I'd rather suggest that one shouldn't) for a stricter meaning, such as the particle being absorbed, or scattered from one of its undisturbed paths, or exchange some amount of energy, or some determined occurrence in general (which is vague...). When one says "interaction-free detection", he/she refers to this second meaning. And this meaning is open to a positive answer to Your question. I'll try the "how is this possible?". The first thing that the "bomb-detector" does to the particle state is decohering its state in the basis resolving the two paths. For the first meaning the particle is changed by this, but not for the second (for a very ideal, decoherence-only, effect on the particle state). If the "bomb-detector" does nothing else than this to the particle, both states along the two paths propagate to the final beam splitter and end up to the interferometer detectors. The particle has not been absorbed, scattered, it had no exchange of energy, nothing whatsoever (of this sort). Maybe, according to the second meaning we want to sat that the particle has not changed due to its interaction (which occurred!) with the obstacle? Maybe. But is its behavior at the end of the apparatus the same? No, its different because its state has changed. Statistics? No bomb-detector yields odds for clicks in the two detectors that are 100% D1 and 0% for D2. Bomb-detector yields odds that are 50% for D1 and 50% for D2. So the change is physically significant. Do we want to call this change in behavior a change of the particle or not? I guess it depends on preferences, context, what one wants to express. For certain reasons that I have, to me this is already a very dramatic and significant change. Formally the particle going into the apparatus can be represented as a superposition of the states going through the separate arms of the interferometers. If it is not disturbed, i.e., there is no "bomb-detector", this choice of basis is just a matter of convenience for the computation of the effects of beam splitters and mirrors. It exits directed toward D1 with 100% probability. In the basis picture, there is a constructive interference toward D1 and a destructive interference toward D2. If instead there is our ideal decohering "detector" in one of the arms, no matter which or both, the state is changed from a superposition into a mixture of the states going through each path. The mixture (a matrix, not a vector as a pure state) is diagonal in the basis resolving the two paths, by the construction of the scenario. So this basis is no longer just a matter of preference. You can practically think of this mixture as a classical statistical distribution over alternatives, i.e. that the photon state is travelling in either one of the paths, but not both. Or You can just say that the mixture has the interference terms which prevented the photon to reach the D2 detector suppressed. What we get is that now the photon clicks the two detectors with equal probability. Note that in the article setup the bomb-detector prevents the photon on its own path to reach the other side of the interferometer. When it clicks, the click occurs together with a change of the particle in both of the previous meaning. When it doesn't click, we are back to the question of the two meanings we can intend for a "changed particle". I don't know if this makes it clearer how I am trying to answer Your question, or if I intended it as You meant it.
This is explained so well in so few words, and with a scheme, that I don't get what is supposed to be weird. It sounds and looks quite intuitive. What I am missing?
the second beamsplitter should let 50% through, but she says it does not, it would reverse the effect of the first. But what is the reason for the second beamsplitter to work totally different all of a sudden.
Its only possible when the photon wave duplicates at the splitter, and then interferes at the second splitter to go back to a non splitted wave. I think the weird thing is that we still think of light as partickes, though they obviously are a wave, as the inerference pattern of the double slit shows. I wonder how these experiments change using polarized lighhtwaves
I don't understand the cancellations at time 6:48. I need to keep watching the video. Update: I coupled this video with another video. I believe that I now have a better understanding about the destructive interference part of this video.
The reasoning is a quite off and unnecessarily confusing : Sabine repeatedly said that there is nothing weird about entanglement or superpositions. However this bomb tester is simply an application of these tools to achieve the bomb test task. If these two tools aren't weird, then there is certainly nothing weird at all in exploiting the tools' unique properties to reveal information about a path even though the particle didn't take that path. Because that's basically what the tools enable: revealing the lower path has a detector while the particle travels via the upper path. Do you find that weird? well that's what's exactly weird about the tool itself, not the logical application of it!
That’s looking at it objectively from the experiments point of view. What’s interesting is how this is applied to the real world. Your eyes are your detectors, so you only see the end result, you don’t always see the path taken. The merit in this is to keep an open mind. That nothing is really absolute. Because we don’t know everything about time space we can never say for sure. Calling something a theory doesn’t it’s weak or a challenge to refute it but welcoming of a better understanding that could help us.
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For people who dont understand this at first, you need to know that if there is no bomb (no measurement between the photon splitters), the photon will ALWAYS be in superposition (both trasectories at the same time), thus always hitting A (100% probability). If you add the bomb (measurement between the splitters) than there will be NO superposition and the photon will follow only 1 path, either top or bottom. If if follows the bottom path the bomb explodes and if it follows the top path there's a 50% chance it'l hit either A or B.
As per the video, the first and second detectors behave differently when hit by a photon from just one path. First detector splits the beam into two paths and the photon travels along both paths. Second detector (when bomb destroys photon on the lower path) sends the photon from the upper path to either detector A or detector B, but not both. WHY? Why is the photon not sent along both paths like for the first detector? Is it because the 1st detector is intentionally designed and created to send the photon along two different paths while the second detector is designed and created to send the photon along just one of the two paths?
In the case where the photon is detected by B with a live bomb that does not go off, this means that the superposition collapses without interacting with the live bomb, what exactly makes it collapse? does the bomb observe the superposition without exploding? Is it possible to create a bomb that explodes if it observes a photon ie breaks the superposition without necessiraly interacting with it?
One thing I've always found weird: videos on the internet says that if you measure the photon in the double slit experiment, you get a particle, and if you don't, you get a wave interference pattern. Isn't both cases interference patterns? Only one is highly focused on the slits because you are measuring close to the slits? Also, is it possible to measure the photon close to the slit and still let it hit the detector far away?
The "particle vs wave" narration in 2021 is... anachronistic? I would use other terms for those "explanations" in a private and informal context. A measurement is first and foremost decoherence. A possible measurement is distinguishing (resolving) which slit the particle travels through. You don't need to observe the result, and it doesn't need to be recorded in any recoverable way. It only needs to correlate the resolution of the state of the particle through the slit with some state of other systems (e.g. the environment). This destroys interference from the two slit. What You will observe in this scenario on the final screen is a diffraction pattern from each of the slits. On the other hand, just by putting the final screen very close after the slits, we are NOT making a which-slit measurement, and You are perfectly right, it is interference, only intercepted very close to the slits.
@@NetAndyCz Except you can, exactly in the way this video proposes. That 25% chance can be made as close to 1 as one wants, and when this happens, you've not modified the state of the system you wanted to observe in any way. Sounds too good? That's because it is: it takes an increasing amount of time/measurements, which diverges to infinity as the probability of a successful "counterfactual measurement" (that's how this kind of thing is called) tends to one. Apart from this particolar class of measurements, you're completely right: to perform any kind of measurement, you need to have an interaction Hamilton with the system you want to observe, i.e. the system is not isolated anymore and its time evolution will change
what's so weird about that? I'm asking seriously, everyday when i get home it tells my wife i did not get killed in an accident (events that did not happen) what's weird about that? it is just simple reasoning... am i missing something crucial here?
@@powerdriller4124 So what is the difference between a "dud" bomb and no bomb at all? Why would a dud bomb be transparent? Of course this is really a test of detecting a "thing in the way of the photon" without it "interacting with a photon", but it seems to me talking about a dud bomb vs a live bomb is then confusing to the average person, hence my comment.
@@GreylanderTV :: Of course it is confusing for the "average person." It is even baffling for the greatest physicists. The photon goes the no-bomb path, but the experiment still manages to detect the bomb state! It is as if a partner photon, a ghost spy photon unseen, undetected by humans and their devices, had gone thru the bomb route and arrive just in time to meet the normal photon to tattletale about the bomb.
@@powerdriller4124 Confusing in different ways for different reasons. Talking about the dud bomb is misleading in a way that has nothing to do with the weird physics involved.
Also quite interestingly, apparently there's a way to keep improving the results further and get closer to probability 1 of truly being able to tell if a bomb is live! 🤯
When I first heard of this, many years ago now, I concluded that you could do something like that to determine the color of unexposed photographic film because you can determine if a photon of a particular wavelength would be reflected without the photon actually needing to hit whatever it is.
@@jonathanguthrie9368 That actually sounds even crazier! Also there was another thing people did recently, which was to communicate using something similar. They managed to communicate and send information, without actually transferring any particles between two regions!
@@factsheet4930 *facepalm* You can do that easily already by tapping Morse code on a wall and having someone on the other side listening. There is no particle transfer, but there is information transfer. You guys really need to stop sensationalizing QM.
@@Elrog3 Nope, you will transfer sound waves. which is to say, movements inside a medium that propagate all the way to the listener... You transfer vibrational energy and also particles.
two questions: 1.) 6:13 its said, that the photon exist in a super position in both paths, but later it matters which path the photon took. what is the missing parameter to explain this better? it sounds like: in the upper path the photon knows that it would have been collapsed with the explosion of the bomb, but only when it actually took the lower path, it tells you for sure. how can the photon know while not collapsing with the bomb? 2.) 6:36 w/o the bomb in between, why is it clear that the path "continues in the same direction as before"? the condition seems to be the same for both directions (up and right), unless the emitter emits the photon with a spin and the spin determines which path to go upon recombination. i.e. the wave remains always directed towards the right, even when it is going up, or is there another parameter which explains this?
The only weird thing about this is the overcomplicated Elitzur-Vaidman problem. The bomb test is a measurement that does not require any interaction. It is not a novel concept to obtain information about an object without interacting with it. For example, there are two boxes, one containing something and the other containing nothing. If you open one box and see nothing, you can be certain that the other one contains something without ever opening it. It's truly weird if you don't understand that basic example.
That's a great point. I think the fact that you open either box, means you have interacted with the system (even if you end up opening the empty box). But I'm not sure. Would love someone more educated on this to comment here.
In counterfactual measurement, or bomb experiment, there is exactly the same weirdness that in the EPR correlations and in the two slits experiment. This weirdness is called quantum mechanics
It's not, just look for pilot wave theory which takes out all the magic. Now I wish that I had a pilot wave based interpretation for this bomb experiment.
I feel like I must be missing something, surely you could create an equivalent of the bomb experiment with nothing but classical mechanics right? so if you replace beams of light with say the flow of water through a canal, for example, and you replace the bomb with a lock that is either open or closed depending on a coin flip, and that also has a 50% chance of having a leak, then wouldn't you end up with the same result at the end, where you could know both whether or not the lock has a leak, and a heads was not flipped?
With classical mechanics there is always a 25% chance to hit B. No matter if there is a Bomb or not. The thing is that the photon interferes with itself at the second splitter if no bomb is in the way which causes a 100% chance to hit A and a 0% chance for B.
If the water went one way ( upwards after hitting the first mirror in the video) in classical mechanics you couldn't learn anything about whether the lock has a leak. If you kept doing the experiment (and having different coin outcomes) you could figure out whether or not the lock had a leak. However in this experiment a single light wave packet can travel two paths at the same time. A single packet cannot go upwards after hitting the first mirror and give information about the lower path at the same time. There are two interesting quantum properties at work. One is similar to the "double slot experiment" the other being a single light packet knowing about a path it didn't take. I am not sure if this answers your question.
Start with a Mach-Zehnder interferometer. It has a lower output branch with constructive interference and an upper output branch with destructive interference. Put a detector on one of the paths. This eliminates the constructive and destructive interference, allowing some photons to reach the upper output branch. Start with another Mach-Zehnder interferometer whose innards are blocked from view. Run one photon through it. If the interference pattern is destroyed as evidenced by the photon being detected on the upper output branch then we can infer that a measuring device is present on one of the paths. The novelty of the bomb scenario is that we call the measuring device a "bomb". In another scenario we call it a "computer".
@@roccraz There is no shortage of people who claim to understand quantum mechanics. The snag is they all have a different explanation, that falls apart when their reasoning is furthered.
@@roccraz the math is easy...grokking the results of experiments by using one's intuition is hard. From the evolutionary point of view, I don't believe that this is all that surprising: We evolved trying to survive macro framework events ...the very idea that small regions of space can be visualized ignores what went into the evolution of our brains
at Richard Jemkins I don't think it's the bomb experiment itself that's weird. It's the entire mechanism of action and results of a Mach-Zehnder interferometer that is mind blowing. I don't get the significance of this experiment because I think the significance is in the photon behavior interfering with itself at the same time. In my opinion the bomb experiment reinforces the wonder behind the famous double slit experiment.
Exactly, it all seemed classically logical and nothing weird was required. Maybe we missed the weird part? I feel like I need a better explanation as to why it's illogical.
You would need to repeat the experiment many times to determine the actual statistical probability of the photon landing at each detector, and if the bomb isn’t a dud it has a 50% probability of exploding each time you run it. So as with every other aspect of entanglement, it’s practically useless.
The experiment does not tell if the bomb is live or a dud. It tells if there has been something interfering with the propagation of the photon through at least one of the paths. The statistics are the same putting a brick in one of the paths and no more informative, meaning they tell nothing on the capacity of that thing to record the passage of a photon, produce a signal, or of the capacity of a hypothetical bomb attached to it to explode. The interesting part is that one click in the detector that should not click if nothing was in the paths indicates the presence of the disturbance at the same time that no determined event occurs between the photon and the obstacle. The bomb is just a dramatization to emphasize a detection that causes no effects in the detected system. You don't need to determine the statistics of the clicks, You need just one click, but it is not certain to occur every time.
9:00 "and that means you know something of the path the photon didn't take" But that's similar to the interference on the double slit. The photon hits the screen, it interferes with its wave from the path it didn't take. The difference is, in the "bomb" case, when it's live, it interacts with the wave function without interacting with the photon.
Sabine is free to use the word "weird" to mean what she wants, but I think there's a consensus among most QM physicists to use the word in a way that makes it appropriate to call QM weird.
@@estranhokonsta : I would not mind Sabine using the word "weird" in a weird way, if she would also try to make her definition clear... why nonlocally collected info about 25% of the live bombs should be called weird, while superposition and entanglement should not be called weird. It should be noted, though, that most words, especially adjectives, are misleading absolutist shorthands that serve (poorly and lazily) as abbreviations for an unstated relative comparison. Relative comparisons such as "bigger than a breadbox" and "bigger than a car" make sense and communicate fairly clearly, whereas the absolutist word "big" is highly ambiguous.
I am not a quantum physicist but find it fascinating, just want to discover more together by throwing some ideas and hypothesis out In the bomb experiment, it says in the “case” that the bomb doesn’t goes off, the photon did not “take the bomb path” I think saying that is mixing deterministic concept (such as there’s a path) when we are talking about probabilistic reality. In probabilistic terms. Even it is a single photon, doesn’t mean there is a “path” isn’t it? The photon could well be “jumping” in between two path if we can make hypothetical observation along the way that doesn’t affecting the wave I understand observations does affect the wave, but just trying to illustrate the concept that the bomb didn’t go off doesn’t have to mean that the photon did not “take the path”. The hypothesis is: the wave function is the photon itself and does interact with the bomb, thus affecting the sensor outcome, us not observing the explosion is just a sampling of reality, that could result in the same experiment outcome isn’t it? Maybe I am missing a lot, I’m just learning.
The path to detector A has one transmission and one reflection by the beam splitters for a photon regardless of which path it took. The path to detector B has 2 reflections travelling the top path or 2 transmissions travelling the lower path. There is a 90 degree phase shift upon reflection thus the path that has 2 reflections is 180 degrees (exactly out of phase) and cancels with the lower path.
I'm glad it's not just me. I feel stupid. 🤣 It seems no weirder than the concept of superposition itself. The experimenter sets up the parameters of the experiment. They provide possible outcomes to be measured. Because of the way it is set up--and I'm guessing here that it has to be done in such a way in order to make an experiment feasible at all, such that a result can be recorded--what the experimenter has established is a limited set of possible outcomes, so while quantum physicists may interpret this as "learning what the particle _hasn't_ done," I just see it as detecting what it _has_ done, within the limited potential outcomes available. 🤷 They can increase or decrease the number of potential paths, but they are always constraining the number themselves, so they know what it is. Therefore, they can calculate what has happened, and what hasn't happened, from the result. They are the ones who choose to impart significance to the fact that this experiment requires a destructive measuring device. But, yeah, quantum stuff is still neat. Edited to fix a missing quotation mark. Dang it.
Hi everyone. As several people have pointed out, the audio doesn't quite sound right. I can't fix this -- I can only take the video down and replace it in the next couple of days. As it seems to at least be clearly understandable I'll let it up. Will make sure that next week we're back to the normal quality. Sorry about that.
It's weird that I didn't notice it until someone pointed out.
@@nomizomichani Ditto
@@nomizomichani Well, neither did I...
I didn't notice a problem at all, even at a second hearing. So the audio track is in a superposition of weird/not weird. But there is nothing spooky about it.
@@SabineHossenfelder Dont worry about the sound Sabine.. When will you physicists finally get real and admit that we're all living inside a super-advanced, hyper-realistic holodeck complex super-structure.. That would explain emergence, fine-tuning and the holographic nature of our reality. The organic big bang theory doesn't explain any of that 😲😲😲
I'm happy that my teacher of quantum physics was Paweł Horodecki, he showed us in 2008 at one of the first lessons this insane topic of Elitzur and Vaidman bomb experiment. I still treat my notes from it like some sacral artifact. I talked to all my friends about it even when they had nothing to do with physics .Great memories
Find someone how whats to talk Physics all the TIME ;)
well, you are not wrong about treating this like that. After all this is the precursor for magical tech
The bomb experiment may not actually be very weird at all. It may just come from the fact we arbitrarily choose to treat photons differently than other states.
As shown with the second beam splitter, beam splitters are sort of like a logic gate with _two_ inputs and _two_ outputs. It is basically equivalent to the Givens logic gate with the angle π/4. If both inputs are 0, it outputs 00, which is the analogue to no light on the beam splitter, then no light comes out. If both inputs are 1, it outputs 11, which is the analogue to light on both angles of the beam splitter just producing light on both angles of the output. If only one of the inputs is 1, meaning you only shine light at it from one angle, then the output is 50% chance 01 or 50% chance 10, meaning it has a 50% chance to redirect the photon to either path.
Since it is a logic gate and all quantum, logic gates are unitary, applying it twice cancels itself out, so if your input is 10 and you apply it twice, your put is 10. If you apply a phase shifter on one of the paths, basically the Pauli-Z logic gate, then it ends up flipping the final path the photon takes, so if you pass in 10 into the first beam splitter, apply a phase shift on one of the paths, then 01 will come out the second beam splitter. This also replicates what happens if you make a measurement, the state undergoes decoherence after the first beam splitter and becomes either exactly 01 or 10, and thus when it hits the second beam splitter it will have a 50% chance of leaving as a 01 or 10.
If you implemented this circuit into anything _else_ besides photons, all the mystery immediately disappears. For example, if you assign 1 to an electron with spin up and 0 to an electron with spin down, two tangible electrons both take the two paths. There isn't much of a mystery here because both electrons are tangible objects that carry a bit of information as well as some phase related information, so when they recombine on the other end they can interfere based on that information, and making a measurement to the tangible electron causes decoherence. This can be explained in entirely classical terms, you don't even need to resort to quantum mechanics.
The potential fallacious reasoning arises from the fact that we treat photons differently from other quantum states. We assume that a photon in the 0 state does not actually exist and thus cannot carry any information at all. But if we don't treat it differently, if we treat it like any other state, then a photon in the 0 state could indeed carry information and propagate through the system. It would show up on any detector as a 0 because it only carries phase-related information, but it may or may not interact with a detector (depending on whether or not the bomb is a dud), may or may not causing decoherence, and then when it recombines with the other photon, it could alter how they recombine. That would mean it is not an "interaction free measurement," it is an interaction with a photon in the 0 state.
Just food for thought.
I started watching quantum physics a few years ago because I thought it was weird...no what if it's not weird it's no fun
Guess I will go back to the why files and heckelfish to get my daily weird...😊😊
@@amihart9269 I think you are misunderstanding why its weird.
Why its actually weird is because all of this only happens once you add a live bomb, and you can use it to tell if the bomb is live without the photon ever going down the bottom path and activating the bomb. Before you add a bomb, the photon always acts like a wave and goes through both paths which causing it to interfere with itself making it to where it never goes to detector B. But after, and when the bomb is live, the photon starts to act like a particle and only goes through one path. Just the potential interaction with the bomb is enough to collapse the wave function somehow.
I think its pretty amazing that quantum mechanics is both weird and not weird at the same time.
I believe interpretations are that which is weird. In quantum physics particles are NOT in multiple places at once, we just cannot say for certain where a particle is until measured.
Well yes and no. That's the whole idea of the superposition. The particle is located at all of the possible places at the same time before the observation is made. In short - all that is possible, IS possible. It's just about how probable it is. If you were to repeat the measurement over and over again, you would get a probability chart.
Without the observation the particle isn't at any single position, instead the particle is the tautology of "it being" from the sum of all the probabilities (where it could be when observed).
Bomb experiment seems to indicate that we can find out information that COULD be possible without actually it happening, which is really neat.
@@Fex. The idea of it being at all possible places at the same time before the measurement is made..is cool but ultimately bollocks.No different to placing a ping pong ball in a box and shaking it.Would you say the ping pong ball is in superposition?
@@philip851 by your hypothesis, interference pattern should not exist. A single electron can exist at multiple places at the same time and interfere with itself and produce interference pattern.
Well, only until you observe it
"Quantum mechanics isn't weird."
"Oh, that's nice."
"However, quantum mechanics is terribly weird."
"OH NOOOOOOO"
It is weird and not weird or in an undefined state.
It's a superposition.
Hah - Schrodinger's weirdness!
@@Sturzfaktor2 They call the undefined state the superposition? That's like weird.
Let’s ask Douglas Adams about this; he’s still around in a non-Marvel multiverse. 😇
I thought the main weirdness of entanglement was the idea of no hidden variables. That is, it’s not that the two particles have correlated values the whole time that are simply measured at some point for particle A, thus implying what B’s value was all along, but rather that A and B do not in any way have those values, or have them in a non-privileged way along with every other option in superposition, and only when you measure A does B in fact take on the correlated value at that instant, where prior to the measurement it could not have been said to have that value at least not exclusively.
You are absolutely right. Entanglement is incredibly weird, I am always disappointed when people try to "demystify" it. The fact that we have a mathematical model to describe it does not mean that things that it describes are not completely in contrast to our normal understanding and preception of the world.
@@TelekinesisT yeah.. its so misleading because, i can understand that the math is simple enough, but that doesnt mean..i dunno
To be precise, the violation of Bell inequalities breaks local realism, you can keep locality if you throw realism down the drain, that is the idea that it is possible to stitch observers experiences into one global description of the universe.
If all systems are quantum systems, Alice/Bob can't tell that Bob/Alice has chosen a measurement basis before they communicate their results/measure each other, and that can only be done in a way that preserve locality.
That's the idea behind Relational quantum mechanics : en.wikipedia.org/wiki/Relational_quantum_mechanics.
Yeah, the weird thing about entanglement is that if one particle has the value X, and the other -X, you can in fact change the value of one to Y, and when you measure the other it will be -Y... You do not really know what is X or Y either, but you can show with an experiment they are not the same. It is weird.
@@NetAndyCz correct me if I'm wrong but, entangled "particles" must always originate locally. Then, the entangled particles are separated by an arbitrary distance and remain "connected" in so far as their properties must compliment each other. Why is this weird? If particles are really waves in a quantum field(s), then the entangled particles are really just complimentary parts of a wave which remains consistent at any distance. The peak of the wave (particle A) remains a peak, and the trough (particle B) remains a trough, always. If we measure A as a peak, of course B will be the trough, and vice versa. Why is this weird?
7:32 - is this correct, though? There's a 50% chance it gets blocked by the dud, and in the rest of the cases it either goes into detector A or detector B, with 25% chance each. Exactly the same as if the bomb were live.
Unless the wave function somehow magically passes through the dud and recombines with the upper ray to cancel out...?
I looked up the experiment on Wikipedia. The dud does not absorb any light. Protons just pass through.
My thoughts exactly!
You can’t have your cake and eat it…?
The triggers on the dud bombs have no photon sensor, so any light incident on the bomb will not be absorbed and will instead pass straight through.
It was a real experiment, ofc it didn't use a real bomb, but a detector that had the same textbook use as the bomb. The dud (or detector) DID indeed allow the particle to pass through it
@@Christopher-ye6cv Isn't this then only a test about whether there's a photon sensor or not. If you formulate the experiment as "is there a photon-blocking sensor here that does something 50% of the time", it feels pretty trivial, doesn't it? Just shoot a photon through it, if you didn't measure it, it got trapped, but nothing happened.
Quantum mechanics: how I learned to stop worrying and love the bomb.
"how I learned to stop worrying and love the bomb." Finally. Something even I can understand! Thankyou Kimmo.
Haha, good one :)
Lol
ABDULPls
Loved the movie
I had a quantum mechanic once. He was definitely weird. And he was never sure whether he’d actually fixed my car or not.
The car was fixed and not fixed at the same time. But you could never tell where it was and where it was going at the same time.
@@paryanindoeur which wouldn't be so bad if he didn't leave his dead cat inbtge back seat.
That is a joke. But I don't know if a laugh or not.
@@fadiluca , lol
I am both laughing and not laughing but someone is both watching me and not watching me so I am doing neither and both.
By the way, I really appreciate your putting the relevant papers up on the screen. It helps a lot.
Sabine: QM is not weird, just unintuitive.
Me: Ok...
Sabine: But it is weird!
Me: Oh, the plot twist!
And then the villains become the cops and the cops become corrupt. Not surprised to be surprised, it is the plot of all and every American nanar.
Weird and non-intuitive are basically synonyms how most people use them. When they say it's weird, they mean it isn't intuitive...
I got a thought - isn't this just consequence of photon being a wave ? Since wave takes both paths and only collapses after interaction, it travelled a little in the other path that was'nt detected, so it can have some information about it ?
About the "weirdness" of wave functions: I think it's worthwhile to remember that wave functions are NOT the particles themselves, rather they are mathematical models for some aspects of the particles' behavior. It's easy to lose track of the distinction, but it is important. Among other things, it means that there may be aspects of a particle's behavior that the wave function doesn't model very well, and that's fine. It just means we need to understand the limits of our model.
We've been down this road before incidentally. Remember the Bohr model of the atom, and how it was derived with the concept of an electron traveling in a circular path around the nucleus? The model was initially held to be correct, since it proved useful for many purposes. In fact it was based on some faulty assumptions about how electrons function, but it so happens that the math worked out pretty well anyway, and the Bohr model was accepted as the correct model. Until we understood that it wasn't as correct as we thought and discovered its shortcomings.
Wave functions seem to be holding up much much better than that, and they remain a useful model. But it's only a model.
Good comment.
Much of the confusing, so-called "weirdness" of QT comes from making a literal exposition out of the Statistical Interpretation of the Wave-function ("Nature is Uncertain/Indeterministic"). If we regard the Statistical Interpretation as it was first set-out - in Max Born's 1926 letter to Einstein - it is merely a pragmatic, absolute limit on empirical observation, not a statement about the Nature of Reality.
@@donthesitatebegin9283 Well said. And, I suspect that some ideas (like the Many Worlds Interpretation) start with the mistake of confusing the wave function with reality. Maybe there are a billionty jillionty new universes created every nanosecond, or MAYBE it's simply that our model is imperfect. I know which one I'm leaning towards.
Well, wave-particle duality is not weird, it's misleading thinking that only one entity is involved with two roles; one a diffuse and wavy but at the same time compact. The way to see this is to visualize two entities that coexist together, one the wavy quantum package space and the other the compact particle that exists inside the package. This existence changes aleatorily inside the package between valid solutions, on each fluctuation only one eigenstate express. Now, over time the quantum package will have inside a probabilistic distribution of all the particle eigenstates i.e., Psi wavefunction describes space fluctuation but particle physical values depend on a probabilistic distribution of particle existence. So, taking Psi one will conclude that the position will be where it exists, momentum will be where the particle exists, energy will be where the particle is, and so on... all the parameters are developed by an operator over the existence Psi... weirdness has diminished
some people view the wave function as something like a physical wave that pushes the particles around. this interpretation is as valid as any other, unless we find something more fundamental about reality
@@heliusuniverse7460 Yes, but two entities that coexist together solve wave-particle duality, it also explains how communication is achieved in entangled particles, besides, it solves the trajectory problem between eigenstates, explains the collapse situation, and eliminates superposition ideas of simultaneous existence of all the eigenstate with the plausible ultra-high oscillation between them, one at a time idea... many fresh ideas that can be read in a short amazon book "Space, main actor of quantum and relativistic theories."
I don't think the issue is ripping the photo in two and shipping one to New York. The issue would be if you threw one of them in the shredder and the other *instantly* shredded too. That's what Einstein thought was spooky, and he was right.
glad I found this channel
looks like you've misinterpreted the work of the TH-cam's recommendations
So, you glady embrace the religious cannotations of modern science, where guesses and beliefs have become large part? Seems so.
@@josephjohnson3738 What? Mrs. Hossenfelder actively battles against that mentality.
God, I love good experimental design. There is something so satisfying about seeing a complex idea and teasing it apart well enough to test it.
I have the DEFINITIVE solution to the Schrödinger's cat "paradox" I can with significant statistical certainty say that after 10 weeks in a box THE CAT IS DEAD.
This is empirical evidence after a hell of a lot of boxes (and cats)
and you can skip the whole "radioactive" part of the experiment, it makes no differense
@@qinby1182 how do u know that
@@goldenwarrior1186 it starves.
Thank you Sabine. I'm an utter layman and if not for your videos, I very may have fallen into the "quantam woo" trap. You are doing an invaluable service with your videos, it cannot be overstated.
I disagree with her re entanglement. Check it out for yourself. She over simplifies entanglement. I more or less agree re the quantum eraser experiment.
@@deandeann1541 What's wrong with her explanation of entanglement?
A very, very important comment.
Your channel is wonderful, a much needed counter to the Deepak Chopra type folks who keep misusing Feymans's "nobody understands quantum mechanics mechanics" statement. Also- I never had heard of the bomb experiment till this time. You are a true educator in the finest way.
I tried to understand that experiment earlier, but couldn't wrap my head around it.
After your explanation, it is much clearer (but still totally weird). Thank you (again) for being such a great teacher!
This is one of the most intriguing and brilliant videos on quantum mechanics I've ever seen. Brava!
Also completely false. ;-)
@@schmetterling4477 really! In what way?
@@WeirdMedicine There is no quantum mechanics here. The bombs behave in a perfectly classical way and so does the interferometer. ;-)
@@schmetterling4477 interesting! So the interference would happen with, say, water? I believe this has been debunked, but I’m no expert. Thanks!
@@WeirdMedicine I don't know what you mean by "debunked". This is simply a boring like drying paint physics experiment which doesn't tell us anything about quantum mechanics.
It would sound less weird if you had mentioned what being a dud means, i.e. there is no functioning detector in the "bomb" path. So the weird thing is that the presence of a detector, or anything that can interact with the photon, leads to the change .
Maybe talking about bombs is distracting, but that's the way the original paper described it. For experimental purposes, using a detector that may or not interact with photons works the same.
If I understand the point correctly, what is being described here is essentially the same as the double slit experiment where the attempt to detect which slit the particle went through results in a corruption of the wavefunction such that the interference pattern no longer appears. Which I think is perfectly understandable; introducing "detectors" in the path of the interaction most certainly modifies the wavefunction of the overall physical arrangement.
@@kenlogsdon7095 Sure, but the difference here is that in the double slit, the detector interacts with the particle, or at least could potentially interact with it.
Here, we have it setup in such a way that even if the particle never goes on the path that leads to the detector (and thus shouldn't possibly have the information of its existence) and yet it behaves differently *anyway* simply because it could have interacted with it, even though it didn't. That's what is the crazy thing. The particle somehow knows if it's live or a dud before it interacts with the bomb and changes its behaviour accordingly.
Given that a single particle will exploding the bomb, how does a single particle tell you anything? A detection at B means the bomb went off, which is the same info you get from just trying to set it off directly. A detection at A tells you nothing.
@@zyrain Existing a live bomb, Photons only reach B if they go the "up" path.
My brain can tell me something that didn't happen, which is, understanding this lecture. Whenever I think I'm overly intelligent, I simply watch a video on this channel, and I'm immediately brought back to reality.
yeah i didnt understand so much so i went to the comments for reassurance or a tldr lol i feel so dumb
@@Goldenretriever-k8m LMAO same, by the time I finished the video the inside of my head was just like ?????????????
If you scanned my head right now you wouldn't see a brain, you'd just see an endless question marks filling up an otherwise empty skull
I came to the comments hoping to find an ELI5, or at the very least, reassurance
I found the latter so I'm content.
Don't be afraid of learning. It isn't hard. What is hard is breaking down your own faulty beliefs.
Not necessarily, there are more possibilities than what you think.
Too many incoherent interpretations in QM. Nature doesn't work with probabilities and uncertainty. The only reason we tolerate all those speculations is the fact that they assert to have more or less 5% knowledge of the functioning of the universe; so, not bad for the superior beings of a small planet called Earth.
The average person example is so simplistically brilliant. Thank you for making it understandable.
Things like delayed-choice quantum eraser always bugged me the most in QM. Maybe you could make a video about it?
Even better, I'm writing a paper about it (like, right now). Hopefully also another video in the near future!
@@SabineHossenfelder That sounds interesting, is there a preprint available?
@@taw3e8 Not yet! Working on it, working on it...
@@SabineHossenfelder Waiting in superposition...is it good, is it not?
@@SabineHossenfelder I love you :)
It's a bit weird to say, "it's not weird, it's just counter-intuitive." Counter-intuitive is a plausible definition of 'weird,' and since quantum mechanics also violates long held, informed suppositions about physics, it seems counter to even informed intuitions. To then say you can't even imagine what would satisfy the equations, but it's not weird... I'm having a hard time imagining what 'weird' must mean.
Nothing is intrinsically weird or not weird. Things are what they are. We can put whatever labels onto them that we want but nature doesn't care what we call things.
Yes Bubba, even more... one can say all valid solutions are almost classical (eigenstates). The great difference with classics is that quantum existence is in an oscillatory situation with a frequency depending on its energy. The other great difference is that on each fluctuation, nature doesn't have defined information on which solution is, so it will assume aleatorily a temporary valid solution (one eigenstate per fluctuation). These two quantum realities are the so call weird QM; not just... because we can imagine a world with these two additional conditions over the classical ones. Hope this will reinforce your comment, regards
For me weird is paradoxical, counter-intuitive perhaps less so.
Maybe she thinks of "weird" in physics as something that defy explanation whereas "counterintuitive" would be something that have an explanation that seems illogical to most people. I don´t know, but her language would make more sense if she defined it that way.
Will, I think that some words as weird just express a reaction that gives interest to the reader to continue... the important issue is the reasoning in quantum world, how we must adjust it to the real nature atomic behavior and not only with the classical experience.... the arguments over just a sensational word.
If there is a "bomb" (detector) in the lower path, and it's live but doesn't go boom, do we really know that the photon takes the upper path? Could it not be that photon is still taking both paths with 50% probability, but that the detector, even if it does not go boom, disturbs the anticipated interference pattern, so that the photon has a 25 % chance of being detected at A and a 25 % percent of being detected at B?
Not because the photon "took the upper path" - (in some clear sense as if it was a classical setting), but because the interference pattern is disturbed?
I think the point here is that if the bomb is unable to explode, it will not interfere with the photon at all.
I'm trying to wrap my head around this and I'm struggling.
A - Assuming the bomb is live:
A1 - In 50% of the cases the bomb won't blow up, because the beam takes the upper path. Therefore the beam splits into 2 possible paths in the second beam splitter, with 25% of the cases ending in detector A and the other 25% in detector B.
A2 - In the remaining 50% of the cases the bomb blows up, because the beam takes the lower path. And in this video it isn't made clear what, if anything, is detected in A or in B. Are we assuming that the bomb "absorbs" the beam when it travels to it, therefore blowing up, and ending the beam's path right then and there (both detector A and B will have nothing)? Or is the bomb detecting the beam in such a manner that the beam resumes it's travel in a similar manner as in A1, therefore splitting again into 2 possible paths with 25% ending in A and 25% ending in B? This is Important to know, because it implies how the bomb should influence the beam's behavior in the case where it's a dud, as I will explain below.
B - Assuming the bomb a dud:
B1 - In 50% of the cases the beam takes the upper path. In this case, it should split into 2 possible paths, being detected 25% of the cases in A and 25% of the cases B.
B2 - In the remaining 50% of the cases the beam takes the lower path. Now it's important to know how exactly the bomb is detecting the beam in A2, because the way the bomb detects the beam has to be the same in both cases, or else the experiment doesn't make sense. Again, is the bomb "absorbing" the beam, therefore nothing appears in A and B. Or is it measuring the beam in such a manner that the beam resumes it's travel?
In the way that this video presents it, it leaves me believing that the bomb measures the beam differently depending on it being a dud or live.
If that's not the case, then for this experiment to make any sort of sense to me, the beam alternates between having a fixed path (no recombination) and possible paths (that recombine in the second beam splitter) depending if there is a reactionary element (live bomb) in the midst of one of it's paths. The beam "knows" that there is a live bomb measuring it, and therefore changes the way it travels from the source to the possible destinations. On the case where it's live, it rejects recombination, but when it's a dud, it accepts recombination.
If anyone can help me see what I'm missing here, I would greatly appreciate it.
No one knows, still.
If the bomb is a dud then you can treat it as if it isn't there at all.
"Two paths diverged by a beam splitter, and I took the one without the bomb.... and that has made all the difference." - Robert "Photon" Frost
To get this I think you need to know the phase shift of the photon at beam splitter and why in dud case you can't see detection in both A and B (Hong-Ou-Mandel effect).
What I understand is that the experiment uses single photons. At the first beam splitter this single photon enters superposition. It is going both ways (lower and upper pathway), acts like 2 photons!
Beam splitters cause phase shift to photon and the arrangement is such that destructive interference is detected in direction to B (i.e no detection). Constructive interference is detected at A. So, if there is nothing in lower or upper pathways, then the photon is always detected in A (dud bomb can be counted as nothing).
If there is live bomb in lower pathway, follows 3 different possibilities.
- No detection at all means live bomb detonated and photon "really" went lower pathway. Why no detection in A? Must be because bomb itself acted as an observer and caused the superposition to collapse (i guess)
- Detection at A: Photon "really" went upper path and when in second beam splitter it had 50/50 chance to be observed in A or B. This scenario is indistinguishable from a dud bomb by the way.
- Detection at B: Photon "really" went upper path and again at the second beam splitter it had 50/50 chance to get detected at A or B. Detection at B can only happen can in the absence of interference!
Detection at A means bomb is a dud at 50% probability
Detection at B means bomb is live ad 100% probability
Detection at B means we know that bomb is live even tough we never went to peek there!
Gentleman, you dropped this: 👑
It was a whole lot better explanation than the video.
What would happen when we put the bomb midway when the detector is just about to interpret the result.
Hmm, you mean no bomb at all at start and then putting a bomb midway at lower pathway just before detection is made? I think it's giving result for the original setup. I mean changing "post photon" setup does not affect detection result. Like pouring oil to a racetrack after race car has passed does not affect it. I might be wrong...And thanks for reply!@@Jhakaas_Jai
The thing I don't understand is that why the beam splitter split the photon into two for the dud but doesn't split the beam, instead only create one path for the live.
@@edward3190 Hi! Photon enters superposition when passes 1st beam splitter on both cases (live or dud). After beam splitter the same photon goes both upper and lower path. Dud case is easier to understand. Live bomb case is harder. I understand what you mean (why no explosion always if photon goes both ways as said). In live bomb case we sort of look back what really happened. Detection at B happens only in the absence of interference (no photon lower pathway). Detection at B kind of destroyed photon in lower pathway, so is it influencing backwards in time? There is many world interpretation, but that, I think, makes problems for dud case (we should then see also detection at B 50/50, but we don't, so photon must really go "both ways", not one way in this world and other way in other world). I have not seen good fundamental explanation to this detection at B case. I am a layperson.
Thanks for the video. Brilliant experiment! It illustrates the power of the quantum wave function to describe the real world.
I have spotted a trend in QM: anytime there is a disagreement between the math of the wave function and our intuition (or other ideas), the wave function wins out. In Ψ we trust.
The wave function plus a bit of epistemological autonomy. It's not an easy subject.
Oh boy, I have to re-watch this.
Same here, I am having a very hard time wrapping my brain around this. But as even S abine classifies this as "weird" that was only to be expected...
Danke!
For one thing, you can't say something is in multiple states at once until it is observed because you can't observe it in multiple states.
This is a great example of Sabine thinking like the highly trained physicist and mathematician she is rather than like the ordinary person she is addressing. "Weird" in this context means essentially that we don't know what it means (which Sabine recognizes too), but we ordinary folk can't help but still try to make sense of what it means *in non-mathematical terms* and when we try to do that we fail. Sabine, I suspect, is so at home with the mathematics that she does not need to "make sense" of it in non-mathematical terms. "Weird" is just this tension between the ordinary person's inability to make sense of such things as superposition in concrete terms and their impulse to still try to make concrete sense of it. The fact that such things can be handled perfectly simply (and non-weirdly) in mathematical terms does nothing to take aware that weirdness. When ordinary people try to make sense of superposition they are not thinking of it as the addition of wave functions - they are wondering what that addition of wave functions in the equation represents concretely in the world. "I think I can safely say that no one understands quantum mechanics". - Richard Feynman. That's why it *is* weird.
No. There is definite unnecessary msytifaction of quantum mechanics. But i agree to some extent
The odd thing is not that the we gain knowledge about a path not taken, the odd thing is that the behavior of the photon changes at the splitter depending if there is a bomb and depending on whether it's live or not. If there is no detector, it seems to take both paths, if there is, it takes only one of them. That's the only odd thing here and it may not be really odd if we one day find out what space really is.
Consider this: Space is not empty room, it consists of threads and energy traveling through space must travel along one of the threads. E.g. energy always is a wave on a thread and thus it can only travel along a thread. For simplicity, ignore that threads may join, split up, be bend, or many threads may be knotted together. For a photon arriving at the splitter, there are two threads its energy could take; so it could take one or the other one or it split up and part of its energy could go either way. Nothing odd so far.
But what happens if you put an active detector in its path? How about this: An active detector changes the tension of the thread that it interrupts or forces to "go around it". This change of tension is detectable all the way back to the splitter. If now a photon arrives at the splitter, there are two threads it could take, but unlike before, these threads don't have an equal tension level anymore, their tension level is different and the photon can detect that already at the splitter, long before will hit any detector. This may change things a lot and maybe different tension levels, or let's call them stress levels force a photon to make a decision to take one thread or the other thread, as it will only split up if the stress level of both threads is equal.
It's like an electron in an electric circle getting to a point where it can either pass through a 100 or a 200 kOhm resistor. It will have to make a decision which way to go as both paths will be used, even though the 100 kOhm one will be used a lot more. How it makes that decision? Sure, that would still be a mystery. I'm talking about the photon here, we know it for the electron. And an electron will also not split up if both paths are 100 kOhm, so the photon behavior is different here but adding those threads (or paths or whatever you want to call them) to the mix and giving them a stress level, it's less spooky that the photon changes behavior at the splitter depending on whether there is an active detector or not if only an active detector changes the stress level.
How is an active detector different from an inactive one? How about that: An active detector forces energy, at least certain kind of it, passing by to interact with it, while an inactive one would energy just allow to pass by. Maybe anything that is reactive to at least some form of energy changes the stress level of a path and as path may not be limited in length and could spawn from one end to the other one of the universe, assuming for a second there is such a thing as an end, this could influence the behavior of energy that could take this path and is million of light years away from us.
In reality these threads would rather by a super complex asymmetric 3D grid, you could also say a field and this brings us back to quantum field theory. If our universe is made up out of fields then an active detector would just change these fields in some way and this will change how energy is traveling through these fields, wouldn't it? And from that perspective, I don't think this experiment is weird at all. It's not intuitive to us as the world we live in is full of detectors. E.g. there is matter all around us pretty much all the time that will interact with photons and thus behave like a detector. The stress level of all possible paths is pretty much always different and that's why we see particles only taking distinct paths in our world. Yet that is like if someone who was born on an island completely covered by forest and who also staid there his entry life would believe the entire world must be covered by forest which isn't the case but that's how the only world he knows and has ever seen.
I didn't understand the bomb allegory until realized that the "dud" bomb does not detect anything IE it does not exist. And the live bomb is detecting the electron. Thus decohering the system. So all the thought experiment is doing is detecting the presence of a detector in one of the possible paths without triggering the detector....25% of a time.
Exactly. It's a fake paradox. If the the 'Dud' were REAL then it would ALSO collapse the wavefunction (just like its 'Live' twin).
@@adamjondo The dud could simply take the signal and reemit it and the entangled photon would be retarded. Depending on the inherent delay in that scheme, it would not be measurable and so 'nothing happens'. Thinks... a Fresnel rhomb would pass the electric field and absorb the magnetic component, such that the emission is colinear with the source. Such a system existing in the path of one of two entangled beams would retard the phase of both of them due to inductance at the source (not magical or instantaneity (which still introduces a phase shift, a problem for single photon interference), simply inductance). Failing that a Fresnel rhomb could be introduced into both paths. It would take a long age explain just how rigged it is in the favour of generating the paradox, but you have to give them credit for putting in the work.
Then why does the live bomb collapse the wavefunction? it doesn't explode. So 'nothing happens'. It can superposition. All the jack-in-the-boxes have been defused and can only be sprung by a trainee.
Thank you! I first learned of this a couple years ago, and I have periodically read the wikipedia page on it multiple times since then, but I was never able to properly wrap my head around what actually is happening in this experiment. Seeing the process built up step by step finally made it click for me!
If you understand QM, it is easy. If you do not know QM, it is genuinely weird. It represents a kind of non-locality different from EPR, which is not really that weird. It is based on correlations. Interestingly, EPR shows that QM does not obey the ordinary rules of probability as Bells Theorem showed (amongst other things).
@@bhobba Why then conceive and perform such an experiment by those who obviously understand QM? What did they want to explore?
@@nikoszaronakis1862 Many, many people understand QM. But there are many different interpretations of what it means, largely IMHO because we do not have direct experience with the Quantum World, so do not have an intuition to guide us. It is to emphasise this non-intuitive nature that some come up with such thought experiments - they understand very well how QM explains it. Remember, QM is a model of the QM world, a map if you want to use that sort of language, but as the saying goes - the map is not the territory.
@@bhobba Thank you! So they understand how it works (which I don't fully) but they don't understand why it works that unintuitive way (so there comes interpretation). But it seems like this experiment doesn't add to what we already know about how QM works. To me all these experiments sound like "what would be the analogue of QM behaviour in the macroscopic world and are there really any interactions/ impact on it".
@@nikoszaronakis1862 The way I look at them is to hammer home you can understand something and know why it works, but it still is weird. That occurs not just in QM but in many other areas as well. Take 1+2+3+4...... Any ninny can see it is infinity - but believe it or not, it is -1/12. I know why (it boils down to something in complex analysis called analytic continuation without going into the details), but it is still counterintuitive and weird. The root cause of the problem here is we make an unwarranted assumption the integers are just part of the real numbers - in fact, they are also part of the complex numbers, and powerful theorems from that area of math can be used. So one reason for these 'experiments' is to flesh out the unwarranted assumptions you are making.
This is second part of Entropy, which includes entropy in terms of arrangement and probability.
Suppose there are three color balls, r(red), g(green), b(blue) arranged in three places available for them. So they arranged like; rgb, rbg, bgr, brg, grb, gbr. There are six ways in which they can arranged this is permutation. If one more different color ball or place is added, pernutation or number of arrangement increases to twenty four, that is four multiply to six previous arrangements.
Now as there is no preference of any arrangement and all are equally likelihood, so probability of any one selection is 1/6. Thus we see that probability of any selection decreases with increase in permutation or arrangements, and which is related to number of particles or participants which is ball in this case. Decrease in probability is increase in uncertainity or randomness or chaos.
Now if in above case if two of ball are of same color, suppose there are three balls of two colors r(red) and b(blue). Then above six arrangements reduces to three; rbb, brb, bbr. So when particles becomes indistinguishable, permutation or arrangements decreases and thus probability of any one arrangement is increase. This type of permutation is equivalent to combination of choosing two balls from three balls of different colors.
Probability distribution function of maxwellian particles which are considered as distinguishable is given by suppose, 1/X. Where X is permutation of particles. Similarly permutations of fermions and boson are X+1 and X-1. Both fermions and bosons are considered as indistinguishable particles but their probability distribution function is higher than maxwellian for boson is okay but lower than maxwellian for fermions shows that fermions are distinguishable particles and that is indicated by their spin half property which is basis for exclusion principle.
Does there are three kind of particles, two of them are governed by quantum statics or there is one kind of particle given as classical one and there are three kind of distribution density states.
Suppose permutation of particles having given higher energy is X, then its probability density function is given by, 1/X. This is known as Maxwell-Boltzmann distribution function where it gives probability of a particle having given energy at temperature. On increasing temperature, probability of particle having given energy increased.
Probability of a particle having given energy is 1/X and probability of a particle to not have given energy is,
1 - 1/X or (X - 1)/X. Now ration of a particle having given energy to a particle not having energy is, 1/(X - 1). This is known as Bose-Einstein distribution function and it tells about probability of a particle to have given energy if there is no particle have that given energy before or say ratio of probability of a particle to have given energy to go higher energy level to release given energy to come back to lower energy level. In textbooks it is interpreted entirely different.
Again probability of a particle having given energy is 1/X, and probability of another particle to have that same given energy is, 1 + 1/X or (X + 1)/ X. Now ratio of a particle having given energy and another particle to have same energy is given by, 1/(X + 1). Thus the probability of a particle having same energy as by another particle is decreased to if that energy is not occupied. This is known as Fermi-Dirac distribution.
So we see that there are no more two other kinds of particles obeying quantum statics but conditional probability distribution of same kind of particles.
I was following for a while but the grammar got me confused at the end >< are you saying that the particles have to be distinguishable, because if they weren’t, you could lower the probability distribution by having particles change into different particles?
Neil you are clearly very intelligent and your point seems good but the detail is lost because of grammar twists and turns.. if you could rework it … well I’d love to try to understand cause i think i know what your saying but its just not so clear for me to really get it…. Appreciate.
@@5ty717 May be my words stumble because I want to write in brief and second thing, to write against established conception is difficult due to people misunderstand that I lack understanding. Also this topic is tedious.
"If the bomb is a dud, nothing happens. The photon splits, takes both paths..." But surely the bomb (or its detector) would still block the photon even if it's a dud?
In the scenario of the article, with a 100%-efficient 100%-absorbing detector in one of the arms, the odds are: 25% D1 clicks (let's say D1 is the detector that always clicks when there is nothing in the paths), 25% D2 clicks, 50% neither D1 or D2 clicks and the photon is absorbed in the bomb's detector.
Forget the bomb, the scenario is about what happens along the photon paths and tells us nothing about the quality of bombs eventually wired to a detector along the photon paths.
In fact, the "detector" itself might be damaged and it doesn't register anything. We have no information about this by the click in D2. What we know is that the state of the photon has been altered by the presence of something along the paths, at least one of them. Could be the lab assistant's elbow.
@@ThePinkus Yes, I realise it's not about the bomb. But the detector would still block the photon no matter if the detector works or not. Why does she say "If the bomb's a dud, nothing happens"? 07:27 I guess she should have said "if the bomb is not there..."
@@Tom_Quixote I rechecked the article to see if I was missing something before answering.
Btw, You can find it on arXive, though I am not posting the link since the last time I did YT deleted my comment, or at least that was the correlation between link and deletion...why!?!?
The authors specify the sense in which the bomb is a dud at page 8 of their article.
A bomb is a dud when it doesn't have the detector that would absorb or scatter (prevent it to go on through the interferometer) the photon, so, they mean "dud" = "no obstacle".
When "dud" means just that, then the reasoning goes on as described.
Ok, in this way it makes sense.
You made quite the right question.
No other type of "dudness" can be detected by the apparatus, so it is very important to make this clear.
Thank You for asking!
@@ThePinkus That is not what a dud means in English.
@@yecril71pl I am of course well aware of it. ;)
That is why the authors of the article take care to explicitly state that by "dud" they mean just that, so that they can make the subsequent reasoning. They also are explicit on the fact that all of the bomb narration is just a dramatization of their reasoning, and I would add, so that it is not relevant.
It is totally obvious that the apparatus does not divine the quality of things in the common sense of parlance, but it only detects an obstacle along one of the paths.
So, given that the article is written in that manner, if we don't specify that by "dud", in this case, we have to intend nothing else than "no obstacle" we cannot follow their reasoning.
IIRC the success chance of detection without going boom can also be boosted quite a bit with more elaborate setups, right? (Though the chance that the bomb blows up in your face can't be brought to 0)
Adding more beam splitters after the bomb part should do it. Each time the photon splits and moves the direction or A or B2. Put a bunch of beam splitters (n) and the chance for the photon to always move to A is (0,5)^n. I could be wrong.
@@leolafortune1255 I think once you do the split, the particle will always take the same path in subsequent splinters. It's like a particle can have a probability less than 100% to be in a certain location, but after you measured it there, you can be certain that is where it is and it's not going to jump to one of the other probabilities in a later measurement.
What you want to bias the setup for is a situation where the probability of the photon to go to the bomb is near zero and the probability of going to the detector B when a bomb is live to be near 1. This requires more beam splitters in series before the bomb to increase the probability of the photon not blowing up the bomb. Then, when we go to where the beams recombine, we can sum all wave functions and get something converging on 25% and 75% for B and A respectively. To further increase the accuracy would require increasing the number of times you sum "the path not taken" - and I don't think there is a way to do this. You simply reduce the odds the path taken is the one that blows up the bomb and allow for multiple sample cycles - if you shoot 100 cycles and don't get a response from B or an explosion, then you have whatever the probability of flipping a coin with a 75% chance to be heads is 100 times and getting only heads. Or... 74.999x - or whatever the probability has been reduced to.
I think ... It may converge on 50/50, but I don't think so.
Bear in mind I have had no formal education or experience with this; I am well beyond my math.
@@Aim54Delta en.wikipedia.org/wiki/Elitzur%E2%80%93Vaidman_bomb_tester#Improving_probabilities_via_repetition
Of course, if we take the suggestive scenario too seriously, the better strategy is to detach any explosive or otherwise dangerous part from the apparatus, since the experiment doesn't really tell us anything about their quality.
I thought "entanglement" was different from a ripped photo because the particles don't decide which property they have until they are measured. IIRC there was an experiment where you measure spin axis direction which shows a result different to the expected result for a "ripped photo" example.
The quantitative results are different because we aren't dealing with objects, but the basic idea about entangled pairs, be they classical or quantum mechanical, is fairly similar.
@@schmetterling4477I thought the Bell experiment indeed showed there are no hidden variables, so the picture analogy seems to be wrong.
@@daanschone1548 There were already no hidden variables before Bell. The entire idea of hidden variables is just one big intellectual mistake. The point is that entanglement is the consequence of conservation laws and those are the same for both classical and quantum mechanical systems.
@@schmetterling4477 sounds logical. The entangled particle has the opposite state of the other and conservates energy etc. But do you think the outcome of measuring an entangled particle in quantum state is pre determined? Because that is what the photo analogy suggests. And that differs from what I understand of quantum states.
@@daanschone1548 A quantum mechanical measurement outcome is not fully pre-determined. We don't need entanglement to see that. When an individual unstable nucleus decays is not predictable but the average decay energy is. In case of a pure spin (1/2 or 1) state the spin projection statistics depends on the orientation of the measurement device, but there are angles at which all outcomes are either up or down. So, no, the quantum system does not carry all the necessary information about the measurement outcome, but it carries some. This is all fully expressed in Copenhagen, already.
Quantum mechanics has only a fraction of the weirdness of the people who dislike these great videos.
I'm suspecting that Michio Kaku creates fake accounts to dislike Sabine's videos 😂
Sabine Hossenfelder: Her science is up-to-the-minute up-to-date---and her clothes are from the future.
I thought it was a Star Trek uniform from the 1990s
@@fillemptytummy :)
@gustavo champoski You could be right or you could be wrong. You are in a superposition of right/wrong.
I hope I can find stuff like she wears in Sydney, some serious outfit shopping is in my future.
Isn't this equivalent to putting a wall between the first splitter and one of the mirrors? It also deletes one of the paths and prevents destructive interference.
Also, are we experimentally sure about the premise to the experiment, aka that it would only activate detector A without the bomb?
That's what i have a problem with. if superposition is a sum of two possible outcomes then even without a bomb, the same possibilities should exist.
Yes, this is exactly the same result as the classic double slit experiment except the output is binary not a distribution. The weird part is that with the entanglement apparatus described by Sabine you can perform stuff like nondestructive testing on a sample. Using Sabine's example and assuming 50/50 live vs dud population of bombs, you can separate 25% of the live bombs from a mixed population on each pass (meanwhile 50% will blow up and 25% will remain in the mixed population, which can be sampled again). This could have major implications in many areas of science,.medicine, computing, etc.
@@everfree2532 Superposition is a sum in the sense that two entangled states are combined to represent the entire system. Consider a simple oscillation (as a.proxy for the wave function); a superposition would mean the single oscillation is divided into two (or more) oscillations that can be added back together to derive the initial oscillation. Without a "live bomb", they are always added back together. But the presence of the live bomb sometimes "collapses" the wave function whereby the divided oscillation cannot be recombined, and this fundamentally changes the observable behavoir of the quantum object that the oscillation defines (in this case, a photon).
if i understand correctly, the dud is like empty space and does nothing. the bomb is like a detector and a wall and collapses the wave function and destroys the entanglement. this seems similar to the interference pattern disappearing when you introduce a measurement into the double slit experiment.
i think you could do something similar rig a bomb/detector or a dud-nothing to the double slit apparatus. if you detected a photon in the "dark" region of the interference pattern you would have a much better than 50% confidence that there was a bomb/detector attached to the apparatus. if it was in the "bright" region of the interference pattern, you might get into a monty-hall style debate about whether there was a still 50% chance the thing was a dud.
A common confusion with quantum mechanics is people are taught to view particles as a point like object, which there is no evidence for. Hence wave duality "paradoxes". In reality they are more like fuzzy balls that can spread, which explains why an electron can form superposition bond with two protons symmetrically apart, as it spreads. We cannot assume every mathematical description has a realistic counterpart.
Elementary particles are point-like in a certain sense. The probability function is not the same as the particle being spread out. You can actually tell the difference. There is something called a form factor in particle physics which accounts for extended structures of particles. The electron has a charge, and when a particle interacts, the way it is deflected depends on whether the charge is spread out, or located at an infintessimal point in space. It's mathematics, so I can't really explain it any better than that. It is one of the reasons we know that electrons are point-like, but protons are not.
@@alienzenx There is absolutely no evidence that it is located at an infinitessimal point in space and it's not necessary to interpret it that way from the mathematics, please refer to "No Evidence for Particles" by Casey Blood to see the myths answered surrounding the conception of particle.
That's not true. Experiments in colliders have given an upper bound of the size of the electron, and it is much smaller than a proton, _a fortiori_ of an atom. The corpuscular aspect of a particle is that if it is observed (as a point say) at a position, it can't be observed at another position. When the position or the momentum of an electron in an atom is measured with a good enough precision, the atom ceases to exist.
@@clmasse I know that. The point is that the spread of the wavefunction is not the same as the particle itself being spread out, which we can measure.
@@JL-fh4qw We can never measure with infinite accuracy and there are fundamental physical limits to what can even be theoretically measured. Never-the-less, the electron is as far as we can tell point-like, and the spread of the wavefunction is not the same as the particle itself being spread out. The wavefunction has a finite value at every point in space, so you would have to consider particles to be of infinite size.
I'm not a physicist but I've watched a video talking about some scientists proving Einstein wrong in that there are no hidden variables in entangled particles, so wouldn't that mean that even if the correlation between the entangled pairs was locally created, their future states should not be dependent on each other (but they are)?
It is attributed to Einstein that he thought quantum mechanics is not complete, and a more complete description would entail further variables. But we don't exactly what he meant since his famous paper was written by one of his students, and of course he has a more subtle take. He saw what nobody then saw, and in addition he was essential in the discovery of quantum mechanics. Since then there have been the theorem of Bell and the experience of Aspect that showed quantum mechanics is complete. But that doesn't mean it is right. Actually it is weird and doesn't fulfill the criteria of a scientific theory.
That’s correct, the Bell theorem experimental results prove (independent of any possible theory) that there can not be any local hidden variables that would reproduce the correlations predicted by quantum mechanics. Sabine’s analogy of tearing a photo and sending them off, is not in accord with QM,… which is to say, it is invalid to presume that the measured attribute/results exists before a measurement is made. [The act of measurement supplies the conceptual form, as a condition for observability,…. so the attribute is created at observation]
@@clmasse : QM fulfills a non-naive criteria of a scientific theory perfectly well.
@@clmasse *
@@noumenon6923 A scientific theory must be consistent and predictive, quantum mechanics is neither.
It took me ages to get my head around this. You did say ‘when the bomb is live and it doesn’t explode then you know the beam is in the upper portion only. I couldn’t see how this extrapolation would in its self collapse the wave function and I had previously thought that detection and collapse of the wave function only worked positively ie when you observe you see a distinct discrete position. I didn’t realise that a negative observation (nothing observed) also collapsed the wave function to an alternate discrete location.
I was thinking about it the other way around, like, it is the (theorical) collapse of the wave fuction through one path that results in a negative observation.
"The photon goes through one path, so the results tells you something about the path it didnt take"... i think it is the change in the wave fuction that actually causes the result, so i would say it is the wave fuction that tells you something about the possible path it could've taken
If you're still having trouble figuring out why this is better than a coinflip (after all it still explodes 50% of the time), think about the problem this way: we want to test if the bomb is live so that we can store it for use later. In classical physics this is impossible, there is no way to ensure that the bomb is live without blowing it up. But in quantum mechanics, using the method shown in the video, there is a 25% chance it will NOT blow up but we WILL know that it's live.
Thank you
this is a far better explanation than in the video, thanks!
But I still don’t understand even from the video why we know it’s live. It seems like she is saying that the beam splitter in some cases directs the photon in one direction vs the other and in other cases it splits it into two (half photons? Different type of of photons?) and half a photon won’t blow it up?
@@JayMutzafi Yes, this is confusing in the video because of some of the words she uses (splits/beam splitter/recombines). If I understand it correctly, it's not a beam "splitter", instead it causes the photon to choose a direction with a 50% probability. The superposition property allows the photon to interfere with itself at the second "splitter" so if the bomb isn't detected the probabilities of travel (+50/-50) add back up to direction of travel to A. If detected by the bomb being triggered, the superposition property of the photon is removed and the photon is then forced to choose a path at the second splitter with 50% probability once again. In my mind, this still doesn't explain the superposition property.
Yeah it took me 2 hours to figure this out because half of the key terminology Sabine used in this video were misnomers. While beam splitters tend to be used in the context of splitting up a photon, in the video it is used to indicate a split in the photon’s decision tree. At least per my understanding.
This material is still too advanced for my head to wrap around properly at the moment 😅
Concluding that an event didn't happen doesn't sound that weird to me.
Yeah I really don't understand what's weird here
Wow...you are rather good at giving intuitive explanations for this
Some high 🍞
What is she on about? The weird thing about entanglement is that the particles seem to interact with each other instantly faster than the speed of light. Isn't that what they mean by non-locality?
Yeah, i havent checked this distant entangled particles topic too deeply, but wasnt it weird all about interaction/ controll during measurment?
After watching the 'bomb' experiment several times, it appears to be an equivalent of the double slit experiment if having two clear paths makes detection at 'B' never happen, even with a single photon. Definitely goes against how I always thought a beam-splitter worked; one path or the other with a probability (50-50 in the example shown). If equivalent to the 'double-slit experiment', then any detector (bomb or otherwise) placed in the lower path will cause detection at 'B'. It would seem that the experiment is only telling you that you are attempting to determine the path.
This is an under rated comment.
@symo Besides, it seems to me like you could also do this with soundwaves. Really you are just using the properties of interference. Am I right?
@@larswillems9886 no you cannot do this with sound waves.
@@dennylane2010 alright. Why is that? If you don't mind me asking.
@@larswillems9886 there is no classical counterpart to a detector. There is no way to destroy the coherence of a classical wave in a two-slit experiment without closing one of the slit. In the video, both “slits” are open (it is just one of the slit has a detector) but still the coherence is totally destroyed.
If the wave who goes trought the uper path hits the second beam-splitter a long time before the wave who goes trough the bottom path hits it, then should we expected the detector B lights up (with 25% chance of happen) regardless what happens in the bottom path?
What you described was classical superposition; it would be disingenuous to call quantum superposition just 'simple addition and not weird when it has extra properties due to the matrix math involved which makes the 'simple addition' non commutative.
I don't remember addition of wave functions being non-commutative. I only remember that the product, which is what expresses successive measurements, is non-commutative. That is also the case for generic (square) matrix math.
@@histreeonics7770 And you would be right 😉
The strangest thing about QM, are the physicists that act like their interpretation is the correct one.
No interpretation is perfect. They fail to see all the implications, and consider only the ones that fulfill their expectations.
Ah ha…. The nuance of being “correct “ (certainty) and the probability that you are correct
In science, any interpretation is only an analogy and nothing more than that, as long at it is trying to communicate more than the experimental facts. And interpretation will, more often than not, bring much more to the table than just that.
Yes, this is a good example of how mathematical physicists interpret the world. Unfortunately, when they do this, they give us incredibly bad ideas, like Quantum Computers, based on the mathematical idea of the superposition of "Quantum States." Math should be applied to physical reality, instead of creating new fantasies about nature and then using propaganda to get people to believe in these fantasies.
But only in a non local way.
Thanks!
Can someone tell me how the 2nd beam splitter results in constructive interference to detector A, but destructive interference toward detector B?
What is happening at this beam splitter to cause the light to not come out the top?
Phase shifts occur when light is reflected on the front side of a mirror. This is described by the Fresnel equations. See the Wikipedia article on the Mach-Zehnder interferometer, for instance.
yh she didn't explain that part well at all
@@MrCrystalm8yeah, and because of thst i asked why a hundred times, than i tried to explain why could that be, i think it's because if the photon reflects at the beam splitter nothing happens but instead if it goes through the splitter some properties of the photons change
Normally, particle fields are continuous waves and are nonlocal. Only the interactions between two fields are discrete and local (particle).
*This* is really weird
Sabine says: “There’s nothing intrinsically weird about (quantum measurement), people just think there’s something weird about it because they have beliefs about how nature should be.”
I say, "Maybe, Sabine, but the greatest physicists of all time would not have agreed with you: They would say that there’s really something weird about it.
Niels Bohr: “If quantum mechanics hasn’t profoundly shocked you, you haven’t understood it yet. Everything we call real is made of things that cannot be regarded as real.”
Richard Feynman
"I think I can safely say that nobody understands quantum mechanics." (Statement made the year he won the Noble Prize for work in quantum mechanics)
Wojciech Zurech - one of the theoriticians of decoherence
“Reality is what we agree on. In that sense, it’s what’s invariant. But that invariance-and hence quantum reality--is not fundamental. It’s emergent and approximate.”
Roger Penrose: “Somehow, our consciousness is the reason the universe is here.”
Bernard d'Espagnat - French physicist and philosopher and researcher into the philosophical foundations of quantum physics .
"The doctrine that the world is made up of objects whose existence is independent of human consciousness turns out to be in conflict with quantum mechanics and with facts established by experiment."
Werner Heisenger (German theoretical physicist and director of the Max Planck Institute for Physics and Astrophysics from 1960 to 1970): "The idea of an objective real world whose smallest parts exist objectively in the same sense as stones or trees exist, independently of whether or not we observe them ... is impossible."
David Albert and Rivka Galchen:
“We believe that everything there is to say about the world can in principle be put into the form of a narrative sequence of propositions about spatial configurations of the world at specific times. But entanglement and special relativity together imply that the physical history of the world is far too rich for that.”
Hi Sabine, I am confused about something from your video. When you first start the bomb experiment, you imply that the photon has a 50% chance of going to the top path and the bottom path, but then you only show the results of the photon taking both paths at the same time. In the case where the photon takes both paths at the same time, the split photon will either interfere with itself destructively (nothing detected) or it will interfere with itself constructively (detected only at A). My first question arises here. Why is it that it is only ever going to detector A when it constructively interferes, yet later you imply that if the photon makes it through only the top path, there is an equal chance that it is detected at A or B? Next, you show the bomb scenarios where if it is a dud and the photons go through both the top and bottom paths, the bomb doesn't explode and therefore we should get a detection at A, same as if there was no bomb. When you add the live bomb, somehow the photon is allowed to take only the top path, which makes it possible for the detection at B. As far as I can tell, this has absolutely nothing to do with the bomb being live or a dud. It has everything to do with the inconsistency between two variables. First, whether or not the photon is allowed to take only one path, or if it has to take both paths. If it is allowed to take only one path in any scenario, then if it takes the top path only, you will get the same result whether the bomb is live or a dud, since there is no photon at the lower path to determine if the bomb would explode, and no lower photon energy to interfere with the upper photon energy prior to detection. Second, it makes no sense that the energy making it through the final splitter only has a chance of going to detector B when it only takes the upper path. If energy going through has a 50/50 chance to go to detector A and B, then the entire nature of the experiment changes, and it should have a 50/50 chance of being detected at B when it is constructively interfered with after taking both paths. If the energy going through the final splitter doesn't have a chance of being detected at B when it is taking both paths and is constructively interfered with, it shouldn't have a chance of being detected at B when it only takes one path. If detector A only detects energy that was constructively interfered with, then it wouldn't detect the photon taking only one path, because that energy wouldn't be constructively interfered with. Either way I look at it, the results aren't based on whether the bomb was live or a dud, the results are based on when you do or do not permit the beam to take both paths vs a single path, and when the detectors do and do not have an equal chance of detecting energy that makes it through the final splitter. Can you please help me understand?
A live bomb acts as a measuring device, and takes a measurement of the photon after the beam is split. When you measure the photon, then it can only have taken a single path. But when you don't measure the photon, then the photon takes both paths and interferes with itself at the second beam splitter.
Also, when the photon interferes with itself at the second beam splitter, it's always detected at A. It's not either interfering with itself destructively or constructively. It's at the same time interfering with itself destructively in the direction of B, and therefore nothing is detected at B; and interfering with itself constructively in the direction of A, therefore leading to a detection at A.
Hope this clears things up.
@@Fred-gs1ur It clears up the fact that it's a poor analogy. The live bomb is being treated as a measuring device, but the dud bomb is essentially being treated as if it doesn't exist at all. Why bother including the dud bomb, then? It only muddies the water. Just give the analogy with the live bomb only. In reality, the photon could care less whether you hear the bomb go off. That would be like saying if a detector had an alarm attached to it to let you know when it detected a photon, but the alarm broke, that the photon would completely ignore the detector. The photon is detected because it's interacting with a system that changes the nature of the photon, not because you hear the alarm go off. It's silly to assume that a dud bomb wouldn't cause the exact same result as the live bomb, but it doesn't matter, I get what was intended. Thank you for your time.
@@adorableinsect unless dud bomb not only can't explode, but it dosen't even measure the foton at all
A + for effort from me even though I didn't fully read your question due to you not adding linebreaks and me not understanding the explanation anyways.
you say “it’s silly to assume a dud bomb wouldn’t create exactly the same result as a live bomb”…it doesn’t create the same result. In the live bomb scenario, the photon cannot interfere with itself, and is then capable of being detected at B.
Another great video Sabine! Just one correction - @ 8:51 the bomb can’t go to Detector B, it’s the photon that can.
That's not the only glitch does anyone remotely understand where A and B are and what oath is destructive and which is constructive??
@@leif1075 This is essentially a double slit experiment. If the photon really took both paths, it will combine with itself and create an interference pattern. You place one detector in the bright band of this pattern, and the other detector in the dark band. 50% of the time it will be constructive interference and land in a bright band, and 50% of the time it will be destructive and NOT land in the dark band. If the photon only takes one path, there will be no interference pattern, and 50% of the time it'll land where the bright band would have been, and 50% of the time it lands where the dark band would have been, making it bright. Therefore, if you ever actually detect a photon in the dark band area (and that will happen 25% of the time), that means the photon could only take one path, and the bomb is real and didn't go off. If you detect it in the bright band area (50%) or don't detect it at all (25%) then you don't know if the bomb is real or not, except in the 25% of cases where the bomb does go off.
If this isn't clear, imagine a regular double slit experiment, and you're placing the bomb in front of one of the slits. If the bomb is a dud, the light passes through the bomb (she didn't actually mention this, and I had to go look at the paper to understand that bit) and both slits forming an interference pattern. If the bomb is real, it intercepts the photon, thus blocking one slit, and you get a regular single peak distribution instead of an interference pattern. Though since you're doing this one photon at a time, you can only tell the difference in the patterns if the photon happens to land where normally there'd be darkness in case of interference.
@@stargazer7644 see she did NOT explain it that way in the video..sidnt thr video confuse you too..and you don't mean the photon can literally take both paths at the same time right..since it's not possible for a photon to be in 2 places at once so why did you say that?
@@leif1075 The photon can be in two places at once - it takes both paths at the same time - actually it takes all paths and interferes with itself. That's fundamental to Quantum Mechanics. That's why you get an interference pattern in the double slit experiment instead of just a band of light behind each slit. Look for some videos on the double slit experiment.
@@stargazer7644 but isn't I just the PROBABILITY that the photon cam be in one or the other path right? Think about it a photon is a tiny particle it is not large enough to be in both places at once? It's just the probabikity..the double slit interference can be due to multiple photons interfering with each other
This seems misleading. The difference between "live bomb" and "dud bomb" isn't just the explosion, but the fact that the "dud bomb" lets the photon pass through unaffected. The "live bomb" does not let the photon pass through.
The results (i.e detector A&B probabilities) for the live bomb are the same as if you stick your hand in the chamber (at the same location as the bomb) to block one of the paths. In other words, by observing a photon in detector B, you know interference didn't happen because a path has been blocked.
Does "information that a path has been blocked" really translate to "information about the bomb"? I'd call that misleading - the real hidden assumption is that we engineered a bomb that only obstructs the path when it's live.
Please answer this. Without an answer to this, this video just translates to "quantum mechanics allows you to tell if a path is blocked". What's weird? You can already tell if a path is blocked without quantum mechanics!
This brings to mind something that I’ve wondered about.
Regarding photon emitters: Is it really possible to just emit 1-photon at a time?
I believe that I read somewhere that those photon-emitters actually emit a very small quantity of them, but that technology isn’t good enough yet to emit just one.
They often use sources that actually emit a bunch of them and then filter them until there's only one left.
@@SabineHossenfelder Wow! Thanks for clearing that up.
@@SabineHossenfelder Thanks, but that phrasing needs a little correction. "... until there's only one left according to the accepted theories (in particular QM)".
Is there any way to prove that there only one photon at the end without using all of our theoretical framework? Using just an intuitive experiment? That is where one can see the distance and possibly "weirdness" from our 'normal average' human experience (which are in them selves just as much assumptions).
As an aside i will add that I personally do mainly agree with your demonstrated pragmatic attitude in this video. That is more like what i think as science.
As for my earlier case, it is not that it is wrong to assume anything, but it is wrong to forget that it is an assumption. That is how basic logic works after all. It is just that we must work with some axioms, but that doesn't mean that they automatically apply outside our argumentation.
Here the outside could be some kind of 'reality' vs our theories.
@Sabine Hossenfelder the problem is scientis made assumptions from their beliefs of how things should work and use experiments to proof their assumptins
the experimets dont proof at all, actualy the experiments brings more problems, but they continue with their ideas making other teoris to try to explain the results of the experimets
so when new experiments can prove those teories them think the initial assumption was rigth
if I assume that
1- universe is filled with minuscle particles that are slightly repeled by electrons, the think that qe call vacuum
2- the movement of the electron produce a wave in this particles, the phenomenon that we call light
3- those waves interfer in the movement of the electrons
so a lot of problems in qunatum mecanics will be solved an experiments will prove this assumptions. it will bring a lot of other problems too
what it means? nothing
i just think that scientists shouldnt trust so much in the outcome of experiments and the matematics.
@@estranhokonsta There are actual sources called single-photon emitters, name self-explanatory, and there are single photon detectors or SPD sometimes called single photon counters. The SPDs are different from basic light detectors which measure the flux density of light and are DESIGNED to detect one photon. The construction and theory into building SPDs goes back decades and are sold ubiquitously. Nothing tricky about detecting light. Solar panels do it. The only difference is scale. If you measure the electrical pulse you've detected the photon using whatever math to balance equation when going from what your input is "light" to what that should yield at the output: the electrical which represents a detection.
Some things to note, your eye is sensitive enough to detect a single photon. Also if you're thinking of the Young Double Slit experiment just know that the same quantum results has been done with not just photons but with molecules. Last I read it was with the "bucky-ball" molecule: fullerene so I wouldn't get too caught up with dissecting the peculiarities of quantum physics with light.
Entanglement is said to be weird not because the entangled particles are simply like a left shoe and the matching right shoe each inside a sealed box and we just don’t know which is which, rather the weird part is that we have a method and choice to change one shoe to either left or right and the other shoe will always be instantaneously opposite, so reality is not grounded until observed and when observed, that information seems to propagate instantaneously (faster than light).
I am not an expert. But no "we have a method and choice to change one shoe to either left or right", we don't have a way to change one shoe to either left or right. It's just that if one shoe, when observed, turns out to be right, then other will turn out to be left.
@@abhay8437 Not true. You can flip the spin of one particle (without knowing what it was to begin with), and the two particles will still have opposite spins when observed. That is one aspect of entanglement that makes the universe not “locally real” and is pretty weird.
If it helps, there is no way to check that the entangled flip actually happened until an observer physically travels to and confirms the observation on the other distant particle, so speed of light limits verification, but the flip still happens instantaneously. We have done lab experiments where we sometimes flip one particle and other times don’t flip it, and confirmed that the entangled particle instantaneously flipped to the opposite with the same probability distribution as in the setting without any flips and did so before light could have had time to travel the distance between the two particles.
The above can’t be used to transmit information faster than light because you don’t know what the spin was to begin with and flipping it immediately collapses the wave function, so for information transmission purposes, the left shoe and right shoe analogy holds, but it’s an inaccurate analogy otherwise.
@@abhay8437 yeah, and what's so weird about that? I thought they were able to change the entangled particles or move them around and teleport them etc. didn't they do that with quantum mechanics? What about that?
This is not true. We cannot change the spin of one entangled particle and instantaneously change the spin of the other entangled particle.
I love you show! Binge watching after watching the last video you posted, You are a true scientist!
6:44 - Why would the 2nd beam splitter always Just Reverse the effect of the first beam splitter? Wouldn't it create another 50%/50%? It doesn't know what the first beam splitter does. You are shooting a single photon, so it will go one way or the other. You are not splitting a photon into 2 photons.
@@veryrarecommenter5196 I'm totally confused by this also.
This is how I understood: Those are 2 different kinds of "splitters" the "2nd beam splitter" acts as a mirror while the others are half reflective mirrors (that's why 50% goes to one direction opposed to 100% from the "2nd beam splitters aka mirrors"
This video exploded my supposed understanding of quantum mechanisms.
Sounds like a dangerous version of what I like to call the rectangle experiment, except instead of a bomb you have an ultra-fast LCD "disk." You can set up the same thing and put the LCD in one of the paths. Now, turn the brightness down until you get only one photon at a time going through the apparatus. After the photon leaves the source you can decide whether to make the LCD opaque or transparent. If transparent, you get an interference pattern where the two beams collide. If opaque, you don't. But you can change the state of the LCD _after_ the photon leaves the source. So you can imagine a wave function with the photon going down both arms (actually in a superposition of the two). And while the photon is in transit you turn the LCD opaque. So what happens? One of two things: (1) The photon is now only in the arm with the LCD and gets absorbed. Or, (2) the photon is now _only_ in the other arm -- _after_ you turn the LCD dark. So in case two, the photon starts by being in both arms, but when the LCD goes dark, suddenly it's all in the other arm. The one on its way to the detector suddenly ceases to exist! Now recall this is a superposition of the photon being in either arm or both arms or whatever. So it's like the bomb experiment, but a lot safer!!! It's kind of like the 2-slit experiment, but stretched out to make the weirdness of it quite salient.
So there is a way for a quantum particle (light) to interact with a sensor (bomb) in a way that does not change the particle in any way? How so?
A quantum state describes more than just determined events. E.g., it describes correlations (in the form of entanglement). Since (quantum) mechanics is the evolution of these states, we can have a physically significant (quantum) mechanical evolution of correlations that does not entails the occurrence of any determined event.
In the scenario of the article, the photon's state enters the apparatus "going through both arms", and it always "interacts", in the above sense, with the system placed in one of the paths. This is necessary for the possibility of the second detector to click, it wouldn't if the state went through unaltered.
Yet, when this detector clicks it never happens together with any other determined event occurring between the photon and the system placed in the arm. In this sense, which is entirely different than the previous one, the scenario is narrated as "interaction-free detection".
@@ThePinkus Let me rephrase my question, since it seems to me that you did not adress at all: The sensor (bomb) that (clearly has to) interact with the particle does not change the particle with this interaction?
@@oceanliketeacher The interaction changes the particle state, and one could say that the particle is changed or affected while meaning just that.
The particle going into the EV apparatus with an obstacle ("bomb", for dramatization I guess, but quite irrelevant what it is) is always affected/changed by the presence of the obstacle on one of its path in this sense, whatever the end result.
Formally, this is probably the more correct description -- the state changes, and when we say that a particle changes we just mean that its state changes.
But with this meaning, it is already impossible to give a positive answer to Your question "the sensor that interacts with the particle does not change the particle with this interaction?". By definition, the interaction does change the particle. There is no way to interact without changing the particle, in this sense (a trivial interaction that doesn't affect the particle is the identity operator, eventually multiplied by a complex scalar, but we probably want to call that "no interaction at all").
But! One might want to reserve "interaction", "change", "being affected" (and I am not suggesting that one should, in fact, I'd rather suggest that one shouldn't) for a stricter meaning, such as the particle being absorbed, or scattered from one of its undisturbed paths, or exchange some amount of energy, or some determined occurrence in general (which is vague...). When one says "interaction-free detection", he/she refers to this second meaning. And this meaning is open to a positive answer to Your question.
I'll try the "how is this possible?".
The first thing that the "bomb-detector" does to the particle state is decohering its state in the basis resolving the two paths.
For the first meaning the particle is changed by this, but not for the second (for a very ideal, decoherence-only, effect on the particle state).
If the "bomb-detector" does nothing else than this to the particle, both states along the two paths propagate to the final beam splitter and end up to the interferometer detectors.
The particle has not been absorbed, scattered, it had no exchange of energy, nothing whatsoever (of this sort).
Maybe, according to the second meaning we want to sat that the particle has not changed due to its interaction (which occurred!) with the obstacle?
Maybe. But is its behavior at the end of the apparatus the same? No, its different because its state has changed.
Statistics? No bomb-detector yields odds for clicks in the two detectors that are 100% D1 and 0% for D2. Bomb-detector yields odds that are 50% for D1 and 50% for D2. So the change is physically significant.
Do we want to call this change in behavior a change of the particle or not?
I guess it depends on preferences, context, what one wants to express.
For certain reasons that I have, to me this is already a very dramatic and significant change.
Formally the particle going into the apparatus can be represented as a superposition of the states going through the separate arms of the interferometers.
If it is not disturbed, i.e., there is no "bomb-detector", this choice of basis is just a matter of convenience for the computation of the effects of beam splitters and mirrors. It exits directed toward D1 with 100% probability. In the basis picture, there is a constructive interference toward D1 and a destructive interference toward D2.
If instead there is our ideal decohering "detector" in one of the arms, no matter which or both, the state is changed from a superposition into a mixture of the states going through each path. The mixture (a matrix, not a vector as a pure state) is diagonal in the basis resolving the two paths, by the construction of the scenario. So this basis is no longer just a matter of preference.
You can practically think of this mixture as a classical statistical distribution over alternatives, i.e. that the photon state is travelling in either one of the paths, but not both. Or You can just say that the mixture has the interference terms which prevented the photon to reach the D2 detector suppressed. What we get is that now the photon clicks the two detectors with equal probability.
Note that in the article setup the bomb-detector prevents the photon on its own path to reach the other side of the interferometer.
When it clicks, the click occurs together with a change of the particle in both of the previous meaning.
When it doesn't click, we are back to the question of the two meanings we can intend for a "changed particle".
I don't know if this makes it clearer how I am trying to answer Your question, or if I intended it as You meant it.
This is explained so well in so few words, and with a scheme, that I don't get what is supposed to be weird. It sounds and looks quite intuitive. What I am missing?
the second beamsplitter should let 50% through, but she says it does not, it would reverse the effect of the first. But what is the reason for the second beamsplitter to work totally different all of a sudden.
Its only possible when the photon wave duplicates at the splitter, and then interferes at the second splitter to go back to a non splitted wave.
I think the weird thing is that we still think of light as partickes, though they obviously are a wave, as the inerference pattern of the double slit shows.
I wonder how these experiments change using polarized lighhtwaves
I don't understand the cancellations at time 6:48. I need to keep watching the video.
Update: I coupled this video with another video. I believe that I now have a better understanding about the destructive interference part of this video.
QM doesn't tell you anything about path not taken. All information about it came from the probabilities you gave earlier.
The reasoning is a quite off and unnecessarily confusing : Sabine repeatedly said that there is nothing weird about entanglement or superpositions. However this bomb tester is simply an application of these tools to achieve the bomb test task. If these two tools aren't weird, then there is certainly nothing weird at all in exploiting the tools' unique properties to reveal information about a path even though the particle didn't take that path. Because that's basically what the tools enable: revealing the lower path has a detector while the particle travels via the upper path. Do you find that weird? well that's what's exactly weird about the tool itself, not the logical application of it!
That’s looking at it objectively from the experiments point of view.
What’s interesting is how this is applied to the real world. Your eyes are your detectors, so you only see the end result, you don’t always see the path taken.
The merit in this is to keep an open mind. That nothing is really absolute. Because we don’t know everything about time space we can never say for sure. Calling something a theory doesn’t it’s weak or a challenge to refute it but welcoming of a better understanding that could help us.
"And that's what we'll talk about today"
I love the little smile that goes with this every time.
This makes quantum mechanics sound a lot like being an electrician.
only that the amount of actual knowledge you gained is zero with 100% probability.
Person: "Super positions, unobservable eave functions, and entanglement. Quantum mechanics is so weird".
Sabina: "Hold my beer"
Nobody:
Will it fit in my Honda?
Hold my beer
Am I a joke to you?
Asking for a friend
Everybody gangsta
End this man’s whole career
He protecc, he attacc …
Sexual/genitalia innuendo/big balls
Scatological/flatulence /potty joke
Question of quantity answered yes
Plot twist
Left/entered the chat
Gaming reference
Dislikes are from
I’m a simple man
Not gonna lie
No one gonna talk about
Last time I was this early
First
Legend has it
That’ll buff right out
Fun fact
(X) be like
(X) intensifies
(X) wants to know your location
Ha ha (X) go brrrrr
POV: (X)
(X):
Also (X):
Her: I'm home alone
It’s complicated
YT algorithm counting down years
Who’s watching in current year?
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It’s free real estate
So you've chosen death?
Understandable, have a great day
Punch line below read more
😂😂😂😂😂😂😂😂😂😂😂😂😂😂😂😂😂😂😂😂😂😂😂😂!
Idiot.
@@onemoremisfit someone forgot their pills
For people who dont understand this at first, you need to know that if there is no bomb (no measurement between the photon splitters), the photon will ALWAYS be in superposition (both trasectories at the same time), thus always hitting A (100% probability). If you add the bomb (measurement between the splitters) than there will be NO superposition and the photon will follow only 1 path, either top or bottom. If if follows the bottom path the bomb explodes and if it follows the top path there's a 50% chance it'l hit either A or B.
As per the video, the first and second detectors behave differently when hit by a photon from just one path. First detector splits the beam into two paths and the photon travels along both paths. Second detector (when bomb destroys photon on the lower path) sends the photon from the upper path to either detector A or detector B, but not both. WHY? Why is the photon not sent along both paths like for the first detector? Is it because the 1st detector is intentionally designed and created to send the photon along two different paths while the second detector is designed and created to send the photon along just one of the two paths?
@@Sam-ng8lq «First detector splits the beam into two paths» Did you mean to say "beam-splitter" here instead of "detector"?
I heard so much about quantum physics by now, that everything about it seems casual
Casually causal or causally casual? :)
@@CAThompson wait....
In college I never got credit for being 25% right - no one detected my brilliance
You were credited with a -75%. That was brilliant enough that the college still got their money! 👍
It's not easy being a photon after all :)
This is probably because you never 50% detonated.
I bet they didn't, you kept blowing up the school half the time!
In the case where the photon is detected by B with a live bomb that does not go off, this means that the superposition collapses without interacting with the live bomb, what exactly makes it collapse? does the bomb observe the superposition without exploding? Is it possible to create a bomb that explodes if it observes a photon ie breaks the superposition without necessiraly interacting with it?
One thing I've always found weird: videos on the internet says that if you measure the photon in the double slit experiment, you get a particle, and if you don't, you get a wave interference pattern. Isn't both cases interference patterns? Only one is highly focused on the slits because you are measuring close to the slits? Also, is it possible to measure the photon close to the slit and still let it hit the detector far away?
Exactly. Their description needs to be more clear.
The "particle vs wave" narration in 2021 is... anachronistic? I would use other terms for those "explanations" in a private and informal context.
A measurement is first and foremost decoherence.
A possible measurement is distinguishing (resolving) which slit the particle travels through. You don't need to observe the result, and it doesn't need to be recorded in any recoverable way. It only needs to correlate the resolution of the state of the particle through the slit with some state of other systems (e.g. the environment).
This destroys interference from the two slit. What You will observe in this scenario on the final screen is a diffraction pattern from each of the slits.
On the other hand, just by putting the final screen very close after the slits, we are NOT making a which-slit measurement, and You are perfectly right, it is interference, only intercepted very close to the slits.
You cannot really "measure" particle without affecting it. I think it is because of the uncertainty principle.
@@NetAndyCz photones don't exist, it's a concept to faciliate math and measiurment
@@NetAndyCz Except you can, exactly in the way this video proposes. That 25% chance can be made as close to 1 as one wants, and when this happens, you've not modified the state of the system you wanted to observe in any way. Sounds too good? That's because it is: it takes an increasing amount of time/measurements, which diverges to infinity as the probability of a successful "counterfactual measurement" (that's how this kind of thing is called) tends to one.
Apart from this particolar class of measurements, you're completely right: to perform any kind of measurement, you need to have an interaction Hamilton with the system you want to observe, i.e. the system is not isolated anymore and its time evolution will change
Thank you, Professor.
I am a retired chemist.
QM works, but at 74, it still seems strange to me. I am more at home with relativity.
Doc Martin
what's so weird about that? I'm asking seriously, everyday when i get home it tells my wife i did not get killed in an accident (events that did not happen) what's weird about that? it is just simple reasoning... am i missing something crucial here?
Something is missing from this explanatin: why does the dud bomb not absorb the photon?
This is tripping me up as well. Would love for someone to explain the physics of the bomb in more detail.
Because it is transparent, but it detects an electromagnetic effect when the photon is passing thru.
@@powerdriller4124 So what is the difference between a "dud" bomb and no bomb at all? Why would a dud bomb be transparent? Of course this is really a test of detecting a "thing in the way of the photon" without it "interacting with a photon", but it seems to me talking about a dud bomb vs a live bomb is then confusing to the average person, hence my comment.
@@GreylanderTV :: Of course it is confusing for the "average person." It is even baffling for the greatest physicists. The photon goes the no-bomb path, but the experiment still manages to detect the bomb state! It is as if a partner photon, a ghost spy photon unseen, undetected by humans and their devices, had gone thru the bomb route and arrive just in time to meet the normal photon to tattletale about the bomb.
@@powerdriller4124 Confusing in different ways for different reasons. Talking about the dud bomb is misleading in a way that has nothing to do with the weird physics involved.
Also quite interestingly, apparently there's a way to keep improving the results further and get closer to probability 1 of truly being able to tell if a bomb is live! 🤯
When I first heard of this, many years ago now, I concluded that you could do something like that to determine the color of unexposed photographic film because you can determine if a photon of a particular wavelength would be reflected without the photon actually needing to hit whatever it is.
@@jonathanguthrie9368 That actually sounds even crazier!
Also there was another thing people did recently, which was to communicate using something similar. They managed to communicate and send information, without actually transferring any particles between two regions!
@@factsheet4930 *facepalm* You can do that easily already by tapping Morse code on a wall and having someone on the other side listening. There is no particle transfer, but there is information transfer. You guys really need to stop sensationalizing QM.
@@Elrog3 Nope, you will transfer sound waves. which is to say, movements inside a medium that propagate all the way to the listener... You transfer vibrational energy and also particles.
@@factsheet4930 Yes, there is energy transfer. There is no particle transfer.
two questions:
1.) 6:13 its said, that the photon exist in a super position in both paths, but later it matters which path the photon took. what is the missing parameter to explain this better?
it sounds like: in the upper path the photon knows that it would have been collapsed with the explosion of the bomb, but only when it actually took the lower path, it tells you for sure.
how can the photon know while not collapsing with the bomb?
2.) 6:36 w/o the bomb in between, why is it clear that the path "continues in the same direction as before"? the condition seems to be the same for both directions (up and right), unless the emitter emits the photon with a spin and the spin determines which path to go upon recombination. i.e. the wave remains always directed towards the right, even when it is going up, or is there another parameter which explains this?
The only weird thing about this is the overcomplicated Elitzur-Vaidman problem.
The bomb test is a measurement that does not require any interaction. It is not a novel concept to obtain information about an object without interacting with it. For example, there are two boxes, one containing something and the other containing nothing. If you open one box and see nothing, you can be certain that the other one contains something without ever opening it.
It's truly weird if you don't understand that basic example.
Yeah that's what I was thinking. Physicists over complicate normal human experience. Probably they aren't or share alien DNA.
That's a great point. I think the fact that you open either box, means you have interacted with the system (even if you end up opening the empty box). But I'm not sure. Would love someone more educated on this to comment here.
In counterfactual measurement, or bomb experiment, there is exactly the same weirdness that in the EPR correlations and in the two slits experiment. This weirdness is called quantum mechanics
I just found this channel. Wow, my answer to the question "what do you find most strange about QM?" has forever changed. Thank you, this is awesome!
The double slit experiment is REALLY weird. That broke my brain and turned my entire perception of reality upside down.
It's not, just look for pilot wave theory which takes out all the magic. Now I wish that I had a pilot wave based interpretation for this bomb experiment.
@@jondo7680 you are correct. Many people dont understand that the observer means hiting a photon over the particle. Which changes its behaviour
Case bomb is live: pilot wave is blocked from going rhrough the bomb route. Case bomb dead: wave can pass through and we get results
I feel like I must be missing something, surely you could create an equivalent of the bomb experiment with nothing but classical mechanics right? so if you replace beams of light with say the flow of water through a canal, for example, and you replace the bomb with a lock that is either open or closed depending on a coin flip, and that also has a 50% chance of having a leak, then wouldn't you end up with the same result at the end, where you could know both whether or not the lock has a leak, and a heads was not flipped?
With classical mechanics there is always a 25% chance to hit B. No matter if there is a Bomb or not. The thing is that the photon interferes with itself at the second splitter if no bomb is in the way which causes a 100% chance to hit A and a 0% chance for B.
And in this experiment it is not a continuous beam of light like a flow of water. It is a package of light (single photon).
If the water went one way ( upwards after hitting the first mirror in the video) in classical mechanics you couldn't learn anything about whether the lock has a leak. If you kept doing the experiment (and having different coin outcomes) you could figure out whether or not the lock had a leak. However in this experiment a single light wave packet can travel two paths at the same time. A single packet cannot go upwards after hitting the first mirror and give information about the lower path at the same time. There are two interesting quantum properties at work. One is similar to the "double slot experiment" the other being a single light packet knowing about a path it didn't take. I am not sure if this answers your question.
Start with a Mach-Zehnder interferometer. It has a lower output branch with constructive interference and an upper output branch with destructive interference. Put a detector on one of the paths. This eliminates the constructive and destructive interference, allowing some photons to reach the upper output branch.
Start with another Mach-Zehnder interferometer whose innards are blocked from view. Run one photon through it. If the interference pattern is destroyed as evidenced by the photon being detected on the upper output branch then we can infer that a measuring device is present on one of the paths.
The novelty of the bomb scenario is that we call the measuring device a "bomb". In another scenario we call it a "computer".
"I think I can safely say that nobody understands quantum mechanics." [Richard Feynman]
No one yet. Don't you think some one might understand quantum mechanics. It is not hard to understand it. I am writing a book on it. 😂😂😂
@@roccraz There is no shortage of people who claim to understand quantum mechanics. The snag is they all have a different explanation, that falls apart when their reasoning is furthered.
At the same time one understands, one also properly dirt sands and also over stands
@@clmasse maybe you should read my book once it comes out.
@@roccraz the math is easy...grokking the results of experiments by using one's intuition is hard. From the evolutionary point of view, I don't believe that this is all that surprising: We evolved trying to survive macro framework events ...the very idea that small regions of space can be visualized ignores what went into the evolution of our brains
Sabine: "Here's how quantum mechanics is actually weird."
Also Sabine: Explains it in a way that makes perfect sense.
I thought the bomb experiment is more or less a variation of the alive and dead cat problem.
at Richard Jemkins I don't think it's the bomb experiment itself that's weird. It's the entire mechanism of action and results of a Mach-Zehnder interferometer that is mind blowing. I don't get the significance of this experiment because I think the significance is in the photon behavior interfering with itself at the same time. In my opinion the bomb experiment reinforces the wonder behind the famous double slit experiment.
@@danielm5161 No
Exactly, it all seemed classically logical and nothing weird was required. Maybe we missed the weird part? I feel like I need a better explanation as to why it's illogical.
@@KittyBoom360 The point is here 9:17. The experiment shows how quantum mechanics can tell us about events that never happened.
A flowery way to talk about sums. Non- local correlation. That truly does make it not weird. Thank you.
I don't need my physics degree to assert þat I love Sabine
You would need to repeat the experiment many times to determine the actual statistical probability of the photon landing at each detector, and if the bomb isn’t a dud it has a 50% probability of exploding each time you run it.
So as with every other aspect of entanglement, it’s practically useless.
You just use the Banach Tarsky construction to make four identical bombs out of the one bomb so you can blow up the cake and eat it. ;-)
@@magicmulder conservation of mass will not be violateeeeeeeeed!
The experiment does not tell if the bomb is live or a dud. It tells if there has been something interfering with the propagation of the photon through at least one of the paths. The statistics are the same putting a brick in one of the paths and no more informative, meaning they tell nothing on the capacity of that thing to record the passage of a photon, produce a signal, or of the capacity of a hypothetical bomb attached to it to explode.
The interesting part is that one click in the detector that should not click if nothing was in the paths indicates the presence of the disturbance at the same time that no determined event occurs between the photon and the obstacle.
The bomb is just a dramatization to emphasize a detection that causes no effects in the detected system.
You don't need to determine the statistics of the clicks, You need just one click, but it is not certain to occur every time.
9:00 "and that means you know something of the path the photon didn't take"
But that's similar to the interference on the double slit. The photon hits the screen, it interferes with its wave from the path it didn't take.
The difference is, in the "bomb" case, when it's live, it interacts with the wave function without interacting with the photon.
Sabine is free to use the word "weird" to mean what she wants, but I think there's a consensus among most QM physicists to use the word in a way that makes it appropriate to call QM weird.
There are many consensus in the fiction communities too.
Sabine seems to think that the metaphysics doesn't matter, that only the things you can calculate matter
I think the nature of reality matters
"Weird" is a term used by science communicators to entertain the audience.
That's true, but what's often called weird about it isn't uniquely weird to QM. It's a kind of weirdness shared by other phenomena.
@@estranhokonsta : I would not mind Sabine using the word "weird" in a weird way, if she would also try to make her definition clear... why nonlocally collected info about 25% of the live bombs should be called weird, while superposition and entanglement should not be called weird.
It should be noted, though, that most words, especially adjectives, are misleading absolutist shorthands that serve (poorly and lazily) as abbreviations for an unstated relative comparison. Relative comparisons such as "bigger than a breadbox" and "bigger than a car" make sense and communicate fairly clearly, whereas the absolutist word "big" is highly ambiguous.
I Quantum Clicked on your Quantum video to Quantum Listen to what you have to Quantum Say about Quantum mechanics.
Why is there no Quantum after you?*
@@ListenToMcMuck I guess there's a 50 / 50 chance of there being a Quantum Me. But is there a Quantum You ?
@@paulfrancis8836 Well, at least I didn't go boom while watching the clip...
I guess there's still a chance for me, too. ^.^ ,
@@ListenToMcMuck You may go Quantum Boom yet, just give it Quantum Infinity.
I am not a quantum physicist but find it fascinating, just want to discover more together by throwing some ideas and hypothesis out
In the bomb experiment, it says in the “case” that the bomb doesn’t goes off, the photon did not “take the bomb path”
I think saying that is mixing deterministic concept (such as there’s a path) when we are talking about probabilistic reality. In probabilistic terms. Even it is a single photon, doesn’t mean there is a “path” isn’t it?
The photon could well be “jumping” in between two path if we can make hypothetical observation along the way that doesn’t affecting the wave
I understand observations does affect the wave, but just trying to illustrate the concept that the bomb didn’t go off doesn’t have to mean that the photon did not “take the path”. The hypothesis is: the wave function is the photon itself and does interact with the bomb, thus affecting the sensor outcome, us not observing the explosion is just a sampling of reality, that could result in the same experiment outcome isn’t it?
Maybe I am missing a lot, I’m just learning.
I somehow totally fail to understand the weirdness of this experiment.
Something is missing for a non-physican
The path to detector A has one transmission and one reflection by the beam splitters for a photon regardless of which path it took. The path to detector B has 2 reflections travelling the top path or 2 transmissions travelling the lower path. There is a 90 degree phase shift upon reflection thus the path that has 2 reflections is 180 degrees (exactly out of phase) and cancels with the lower path.
physican to physicist is like malapropian to malapropist
I'm glad it's not just me. I feel stupid. 🤣 It seems no weirder than the concept of superposition itself. The experimenter sets up the parameters of the experiment. They provide possible outcomes to be measured. Because of the way it is set up--and I'm guessing here that it has to be done in such a way in order to make an experiment feasible at all, such that a result can be recorded--what the experimenter has established is a limited set of possible outcomes, so while quantum physicists may interpret this as "learning what the particle _hasn't_ done," I just see it as detecting what it _has_ done, within the limited potential outcomes available. 🤷
They can increase or decrease the number of potential paths, but they are always constraining the number themselves, so they know what it is. Therefore, they can calculate what has happened, and what hasn't happened, from the result. They are the ones who choose to impart significance to the fact that this experiment requires a destructive measuring device. But, yeah, quantum stuff is still neat.
Edited to fix a missing quotation mark. Dang it.
Technically, Sabine is also a non-physician. She is a physicist and not an MD.
@@ccarson Thanks, this actually helped me to understand.