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There is this surprising "Asking photons where they have been" PRL 2013 article about experiment where they are able to "ask photons" which mirrors they have visited: by vibrating each mirror with different frequency and performing Fourier transform of the final beam - visited mirrors are marked in the power spectrum.

The problem is that this way they see mirrors we would naively say they shouldn't - mirrors A,B below:

enter image description here

The small inteferometer (with mirrors A,B) is set for destructive interference: such that no photons go through mirror F, what is tested in the lower setting: that if we block beam from mirror C, no light gets to detector.

For explanation, the article uses two-state vector formalism (TSVF): that e.g. $\langle \Phi|\ |\Psi\rangle$ should be undestood that $|\Psi\rangle$ is result of forward propagator from $t=-\infty$ to now, $\langle \Phi|$ of backward propagator from $t=+\infty$ to now, what seems kind of natural e.g. when thinking about Feynman path integral formulation using ensemble of paths from $-\infty$ to $+\infty$.

They explain that we see A, B, C mirrors because only these tree are visited by photons propagating in both time directions.

Is it the proper understanding of this experiment - can it be explained without back-propagation?

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  • $\begingroup$ Wow, that’s very interesting! There better be a forward in time explanation because QM works... $\endgroup$ – knzhou May 24 '18 at 9:13
  • $\begingroup$ QM unitary evolution or path integral formulations are time symmetric. There are many many more experiments with questionable causality, like Wheeler's especially in realization of Aspect's group, delayed choice quantum erasure - especially Walborn's ... Shor's algorithm. $\endgroup$ – Jarek Duda May 24 '18 at 9:19
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    $\begingroup$ Yeah, but we know that the delayed choice experiment and Shor's algorithm do have forward in time explanations, no backward causality required, as I think has been discussed somewhere else on this site. Whether that's the "proper" way to understand it is purely up to personal taste since the results of different formulations of QM is equivalent. $\endgroup$ – knzhou May 24 '18 at 9:25
  • $\begingroup$ There are causal and local explanations of Wheeler's experiment - that photons go one path, but still some pilot/theta wave (of negligible energy) comes the second path. We could analogously say that while photons don't get to F mirror, there is still some pilot/theta wave traveling there ... however, why we don't see E, F mirrors here??? $\endgroup$ – Jarek Duda May 24 '18 at 9:33
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Is it the proper understanding of this experiment - can it be explained without back-propagation?

The answer to this question is definitely yes. Indeed, the authors provide this analysis in the supplementary materials (1) (pdf w/ journal access required).

The field at the detector, for the first setup given above, has this form:

$$\Psi(x,y,t)=\frac{A}{3}\left( e^{-x^2-(y-\delta_C(t))^2}+e^{-x^2-(y-\delta_E(t)-\delta_A(t)-\delta_F(t))^2}-e^{-x^2-(y-\delta_E(t)-\delta_B(t)-\delta_F(t))^2}\right), $$ while in the second setup the first term is removed. The term $\delta_A(t)=\delta_0 \sin {\omega_A t}$ and similarly for the other modulation terms. Note that although I have given this the variable $\Psi$, following the authors, it is actually just a classical electromagnetic amplitude.

It is not very transparent from this form which peaks will result in each situation, and in that regard the TSVF does indeed appear to be useful in this case. However, a few conclusions can be drawn:

  1. The second two amplitudes, which in a path-integral type picture presumably would correspond to the two paths that go through the smaller interferometer, do not in general cancel out. So the statement that the interferometer is in a destructive interference setting does not seem to be entirely true. In effect, the different frequencies $f_A$ and $f_B$ prevent them from cancelling for all times.

  2. As a result, I'm guessing that in principle there should always be some power at $f_A$ and $f_B$, they are just very substantially reduced (it would be interesting to understand by how much exactly) when the beam along mirror C is blocked. If this is not the case, then there must be spectral power elsewhere due to these terms, since they are causing a moving electric field.

Therefore, my suspicion (as of yet unconfirmed) is that this experiment can be read as a measurement of a weak modulation either on top of a strong beam or by itself. In the first case you get a field of the form $\epsilon \cos{\omega_{mod} t} + \cos{\omega_c t}$, and in the second case you only have $\epsilon \cos{\omega_{mod} t}$. When you square these to get the power, the modulation by itself has a power of order $\epsilon^2$, but when superimposed on the strong beam you get interference terms of order $\epsilon$. In other words, the effects from a weak modulation can be made arbitrarily larger than the modulation itself by interfering it with a strong beam.

Of course, this doesn't sound nearly as exciting as the language the authors use in the main text to describe what they see. This is a good illustration of a feeling I have about a lot of these types of papers- they claim to demonstrate some new flashy effect, which does explain the data, but then buried in the text or supplemental material they also admit that there is a much more mundane equivalent picture.

(Note added: rereading the paper, I see that they do mention this perspective a bit at the end and say that the "effect is due to a tiny leakage of light in the inner interferometer," supporting the suspicion given above. So I cannot fault the authors' transparency, but still personally find some of the philosophical discussion to be a bit much for classical wave interference.)

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  • $\begingroup$ (sorry this answer is so long and rambling, it took the process of writing it for me to work out what was going on. Maybe I will edit it down later if I get the chance.) $\endgroup$ – Rococo May 25 '18 at 4:17
  • $\begingroup$ Great, thank you. The possibility of choosing forward evolution or TSVF perspective is analogous to using mathematically equivalent: Euler-Lagrange or action optimizing in Lagrangian mechanics. However, there is Shor's algorithm which is natural in TSVF: mounting qubit trajectories in the past (initialization) and future (measurement), but understanding it as just forward evolution could allow for fast simulation on classical computer ... Do you maybe see how it could still work if putting Hadamard gates before measuring values? physics.stackexchange.com/questions/404860 $\endgroup$ – Jarek Duda May 25 '18 at 5:09
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It is very delicate to talk about "the proper understanding" of such an experiment. What is more relevant is how to develop an intuition. The authors here propose that the two-state vector formalism is intuitively more useful that a trajectory-based view.

There is nothing new here in the sense that we know that quantum objects such as elementary particles do not have trajectories. This is often watered down into conceptions implying that "we can/do not know what the actual trajectory is", somewhat implied here by the title of the paper, "asking photons where they have been", which strongly suggests they have been somewhere; but there is no counterfactuality in quantum mechanics: there is no answer to a question that is not asked.

The questions asked in this experiment are not about trajectories. They are about what photons "see" from the overall setup. In this regard it is analogous to the Elitzur-Vaidman bomb tester, or even the Aharonov-Bohm effect. These show that a quantum system has a sort of non-local awareness of the overall setup is it part of.

The two-state vector formalism takes non-locality seriously, in the sense that is does not distinguish past and future boundary conditions. This is the spirit of the path integral, which has an bird-eye, panoramic view of a quantum system that does not attempt to describe its evolution moment by moment, but is only concerned with computing the probabilities for the "observable end points" of its behavior, so to say.

So it makes sense that when the information we are interested in is scattered in distinct parts of a setup (here, the mirrors), we have a better intuition using a framework explicitely giving up on unobserved continuity than with another mental view that assumes there is meaning in trajectories.

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  • $\begingroup$ Indeed, we know e.g. from violation of Bell inequalities, Hardy or GHZ experiments that nature has some kind of nonlocality - the problem is to properly understand its source. My view is that it comes exactly from living in real 4D spacetime, required e.g. in GRT, CPT symmetry, action optimization of Lagrangian mechanics, or that particles should be seen as their trajectories (instead of points) - also because such ensemble leads to Born rules and so Bell violation. So is there anything more in quantum nonlocality? $\endgroup$ – Jarek Duda May 24 '18 at 11:49

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