Mach-Zender-Interferometer with polarizers

In summary, the conversation discusses how polarizing filters can influence interference in a Mach-Zehnder interferometer. The standard MZI configuration with no filters allows 100% of photons to reach D1 and none to reach D2 due to differential phase shifts. When two polarizing filters are added, only every second photon will hit one of the detectors and the rest will be lost. Adding a third filter at 45° in the D1-path destroys the which-path information and results in 25% of photons at D1 and 12.5% at D2. Similarly, adding a filter to the D2-path destroys the which-path information and produces 25% of photons at D1 and none at D2. The
  • #1
Sonderval
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TL;DR Summary
How do different polarizers added in a MZI change the interference pattern?
I have a question on how exactly polarizing filters would influence interference in a Mach-Zehnder interferometer.
To explain, I'll show some configurations and what I would expect to happen - please tell me if I am incorrect anywhere.

Here is the standard MZI configuration with no filters and a single-photon source on the lower left
interfer0.png

In this configuration, 100% of photons will reach D1, none will reach D2, due to the differential phase shifts from the beam splitter. (I assume that both beam splitters are symmetric and shift transmitted and reflected by 90°, as explained here: https://www.physicsforums.com/threa...h-zehnder-interferometer.972867/#post-6188472)
Now I add two polarizing filters, one vertical, one horizontal

interfer1.png


In this configuration (with single photons emitted from the light source on the lower left), on average, only every second photon will hit one of the detectors (for simplicity, assume that the light source emits photons with polarization 45°, i.e. a superposition og horizontal and vertical). Of these 50%reach D1, 50% reach D2 because the polarization adds a "which-path information" to the photon state and thus destroys the interference pattern. So overall I have 25% at D1, 25% at D2, 50% lost.

When I now add a third filter at 45° in the D1-path
interfer2.png

I expect that this destroys the which-path information. However, the which-path information is still available at D2, so I would expect now that I have 25% of the photons at D2, 12,5% at D1 (number is halved due to the loss at the third filter).

And finally, I add a filter to the D2-path:
interfer3.png

Now I've destroyed the which-path information on both paths, so that interference should work again. In this situation I would expect 25% of the photons to end up at D1, none ending up at D2 and the rest being absorbed at one of the filters.

Are all these considerations correct or did I make a mistake somewhere?
 
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  • #2
Are you saying Alice at D1 expects her average click rate to double based on Bob at D2's choice to place the polarizer in a region spacelike separated from her? Is this not a causality violation?
 
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  • #3
@charters
Yupp, that's worrying me as well.
 
  • #4
I've not checked it by a full-fledged calculation, but just adding the relative phase shifts naively I think your presentation is correct.

There's no causality violation here. You can come to that conclusion only if you wrongly think about the photons as localized billiard-ball like bullets. This picture is utterly wrong! Rather think about photons as electromagnetic waves of the lowest possible intensity for the given frequency. Then it's clear that you need to consider the entire setup, because the interference at a point is caused by recombining parts of the waves going along different paths, collecting their phase changes while travelling, at one point.

This is of course not a correct picture either if you work with single-photon states since a photon cannot be "devided" in different wave parts, but this refers to the detection of the photons in a detector, and the waves do not describe the photons themselves but only the probabilities for detection events of a photon at the place of the detector (note that photons do not even have a position observable, i.e., it doesn't make sense to talk about the position of the photon; only the detection events have a position given by the position of the detector).
 
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  • #5
@vanhees71
I now tried to calculate things explicitly and believe my idea above to be incorrect. (Calculation follows below, I'd be very grateful for someone to check it.)
However, I do see a problem with causality if my idea were correct:
Image we set up the light source to send one photon per second. In scenario 3, Alice at D1 would then expect to find 12.5% of them, so on average one every 8 seconds. When Bob inserts a filter in front of D2, Alice would then find an increased probability of 1/4. With sufficient distance between D1 and D2, I think that this would actually allow to send a message, wouldn't it?

But I think my calculation is incorrect anyway because I did not account for the correct superposition of horizontal and vertical states on the path to D1. I use the following labels for the paths:
interferlabel.png


The first beam splitter creates
$$|0\rangle \rightarrow \frac{1}{\sqrt{2}} (i|1\rangle + |2\rangle)$$
(as I said, I assume a symmetric BS with 90° phase shift)
The second beam splitter then changes this to
$$\rightarrow \frac{1}{2} (i (i|4\rangle + | 3\rangle) + |4\rangle + i|3\rangle)$$
so the two ##|4\rangle##-terms cancel each other and the full signal ends up in D1.

Adding the polarization state, the final state can be written as
$$\rightarrow \frac{1}{2} (i (i|4 H\rangle + | 3 H\rangle) + |4 V \rangle + i|3 V\rangle)$$
and with this all four terms are orthogonal to each other and I get 50% probability for D1 (25% with H, 25% with V) and the same for D2.

So this seems to be correct (i hope!).

I write the 45-degree polarized state as $$|45\rangle = \frac{1}{\sqrt{2}} (|V\rangle + |H\rangle)$$ or
$$|V\rangle = \frac{1}{\sqrt{2}} (|+45\rangle + |-45\rangle)$$
$$|H\rangle = \frac{1}{\sqrt{2}} (|+45\rangle - |-45\rangle)$$

I can now just write the V- and H- states in the 3-path and get

$$\rightarrow \frac{1}{2} (-|4 H\rangle + |4 V \rangle
+ \frac{i}{\sqrt{2}} (| 3, +45\rangle - | 3, -45\rangle )
+ \frac{i}{\sqrt{2}} (| 3, +45\rangle + | 3, -45\rangle ) )$$

With this, what i now see is that the two states in path 3 actually combine to form a +45°-polarized wave, so no photon should be absorbed at the filter at +45°. Corresponsingly, if I have a +45°-filter on path 4, it will absorb all photons whereas a -45° filter will absorb none.

So the correct probabilities should be that in my situation 3 above, the overall probability at D1 is still 25% since the photons from the two paths actually linearly combine to a +45°-polarization state.

I'm not totally sure if this is the right way to calculate things, though, so if you (or someone else) could check this, I'd be very grateful.
 
  • #6
I assumed that the beam splitters don't change the polarization. If you have polarizing beam splitters, of course, the results change. To see this one would have to write down the complete transfer matrices for each of the setup.

Nevertheless, there's no FTL communication possible. Say the message is encoded as "0" and "1", encoded by Bob as having no polarizer (0) vs. having a polarizer (1) in front of his detector, D2. All Alice can measure is however the probability for her detector to click. She needs many photons to get the probability and this takes time. The signals do not propagate faster than light to A and B. Also for the setup to work the photons need to be sufficiently coherent, i.e., they should have a pretty well determined energy. That means the uncertainty of their emission time gets pretty large (through the energy-time uncertainty relation). In order to be able to get enough statistics the photons need to come however well separated in time, i.e., you have to wait sufficiently long between sending the photons, and, because the time uncertainty of the single photons is pretty large, this time is pretty long.
 
  • #7
@vanhees71
I'm not sure I understand. The beam splitters do not change polarization here, polarization comes into it only in situation 3 and 4 where I explicitly added the filters. That is why i simply added the appropriate H and V to the states in the 3rd equation.
I totally agree that there is no FTL communication, but I think if my first (incorrect) assumption on the probabilities were correct, then there would be (because Alice would be able to distinguish a probability of 1/8 from 1/4). I'm not sure the argument that photons need to be well separated in time would prevent this in principle, nothing would prevent me from building 1000 interferometers next to each other (with very long arms between the second beam splitter and the detector), firing all 1000 light sources at the same time and Bob inserting the filter into all of the light paths. But, as I said, it is totally irrelevant because I am quite sure now that my first understanding was simply wrong.
 
  • #8
Ah! I misunderstood you. You are "adding the polarization" for the other cases with the polarizers in the various configurations at place. Then it makes sense.
 
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  • #9
Sonderval said:
... And finally, I add a filter to the D2-path:
View attachment 249932
Now I've destroyed the which-path information on both paths, so that interference should work again. In this situation I would expect 25% of the photons to end up at D1, none ending up at D2 and the rest being absorbed at one of the filters.

Are all these considerations correct or did I make a mistake somewhere?

I don't believe the polarizers you added cause anything to be "erased". You'll get 12.5% at both D1 and D2.
 

Related to Mach-Zender-Interferometer with polarizers

1. What is a Mach-Zender-Interferometer with polarizers?

A Mach-Zender-Interferometer with polarizers is an optical instrument used to measure the phase difference between two beams of light. It consists of two polarizing beam splitters and two mirrors, which split a single beam of light into two paths and then recombine them to produce an interference pattern. The polarizers are used to control the polarization of the light in each path, allowing for precise measurement of the phase difference between the two beams.

2. How does a Mach-Zender-Interferometer with polarizers work?

A Mach-Zender-Interferometer with polarizers works by splitting a single beam of light into two paths using a beam splitter. The two paths then travel through polarizers, which control the polarization of the light. The two paths are then recombined using another beam splitter, and the resulting interference pattern is measured. The phase difference between the two beams can be calculated from the interference pattern, providing information about the sample being measured.

3. What are the applications of a Mach-Zender-Interferometer with polarizers?

A Mach-Zender-Interferometer with polarizers has many applications in optics and photonics research. It is commonly used in interferometry, which is the measurement of small changes in distance or refractive index. It is also used in optical coherence tomography, which is a non-invasive imaging technique used in medical and biological research. Additionally, it is used in the development of optical devices such as lasers and fiber optics.

4. What are the benefits of using polarizers in a Mach-Zender-Interferometer?

The use of polarizers in a Mach-Zender-Interferometer provides several benefits. First, it allows for precise control of the polarization of the light, which is essential for accurate measurement of the phase difference between the two beams. Additionally, polarizers can filter out unwanted light, reducing noise and improving the quality of the interference pattern. Finally, polarizers can be used to compensate for any polarization changes in the light source, ensuring consistent and reliable measurements.

5. What are the limitations of a Mach-Zender-Interferometer with polarizers?

One limitation of a Mach-Zender-Interferometer with polarizers is that it is sensitive to external vibrations and movements, which can disrupt the interference pattern and affect the accuracy of the measurements. Additionally, the setup and alignment of the instrument can be complex and time-consuming. Another limitation is that the instrument is only sensitive to changes in the phase difference between the two beams, and other factors such as temperature and pressure may not be measured. Finally, the use of polarizers can reduce the intensity of the light, which may limit the sensitivity of the instrument in some applications.

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