[HN Gopher] Third-polarizing-filter experiment demystified (2004)
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       Third-polarizing-filter experiment demystified (2004)
        
       Author : rahimnathwani
       Score  : 62 points
       Date   : 2022-08-18 19:10 UTC (3 hours ago)
        
 (HTM) web link (alienryderflex.com)
 (TXT) w3m dump (alienryderflex.com)
        
       | adgjlsfhk1 wrote:
       | This only works if you forget that light is quantized. The place
       | the weirdness really comes in is that if you shoot single photons
       | at a time, you observe the same effects.
        
         | avodonosov wrote:
         | Does the sibling comment by phkahler cresolve your doubt?
         | (https://news.ycombinator.com/item?id=32514107)
        
         | yarg wrote:
         | It's not that weird.
         | 
         | You can consider a wave passing through a filter as a sum of
         | two orthogonal waves, rSin(th) + rCos(th), th being the angle
         | between the light-wave and the filtered angle, r being the
         | amplitude of the wave.
         | 
         | One wave gets eliminated, and whatever exits exits at the only
         | angle it can, the angle orthogonal to the filtered angle.
        
       | phkahler wrote:
       | The part that still needs explaining is how the magnitude can be
       | reduced. IIRC single photons can be polarized by these things,
       | and AFAIK their wavelength is not changed so their energy is
       | unchanged as well.
       | 
       | I have always thought (how I got there I don't know) that the
       | polarizer did something weird like rotate the photon to the
       | correct phase angle AND passed it through with probability based
       | on the angle / or didn't let it pass. This would give a similar
       | reduction in intensity for a desktop experiment while having
       | similar but different details when looking at the photon level.
       | Is this correct?
        
         | gorkish wrote:
         | At the single photon level, the photon that goes into the
         | polarizer and the photon that goes out of the polarizer are not
         | the same photon, so it's not right to say that a photon is
         | changed or transformed.
         | 
         | For a photon coming in at 45 degrees to the polarization angle,
         | the probability that another photon will be emitted is
         | sin(45deg) =~ 70% and the probability that it will be absorbed
         | is 1/sin(45deg) =~ 30%.
         | 
         | (This is also a simplification; polarization angle is similarly
         | quantum in nature, and I have assumed it to be collapsed here)
        
         | abdullahkhalids wrote:
         | The explanation given is at the level of classical
         | electromagnetism, and is sufficient to explain and predict
         | experiments with regular light.
         | 
         | If you want an explanation and prediction of what happens at
         | the level of single photons, you need more structure from the
         | theory of quantum optics. But briefly the filter at angle T
         | does a measurement on the photon in the basis {T, T+pi/2}, and
         | you end up seeing the photon on the other side of the filter
         | only with whatever probability the photon has for being in
         | state |T>, as opposed to state |T+pi/2>.
         | 
         | So, filters are inherently destructive and fewer and fewer
         | photons pass through each subsequent filter. And a photon that
         | makes it through a filter at angle T, now has a new state |T>.
        
           | jiggawatts wrote:
           | The thing is that there is no actual evidence that "single
           | photons" exist _in the electromagnetic field_. That last bit
           | is important: photons are a mathematical shorthand for
           | dealing with emission and absorption by atomic orbitals.
           | 
           | They're not an explanation for continuous waves in between,
           | _but the mathematics largely works anyway_ because photons
           | are very similar to how one would do a Monte Carlo numerical
           | simulations of continuous wave phenomena.
           | 
           | This has resulted in an unbelievable amount of confusion...
        
             | oh_my_goodness wrote:
             | There is lots of evidence for photons in the EM field,
             | beginning with Planck's invention of photons. http://hermes
             | .ffn.ub.es/luisnavarro/nuevo_maletin/Planck%20(...
             | 
             | If you make the energy in a mode of the EM field
             | continuous, you get the famous 'ultraviolet catastrophe.'
             | This holds whether the matter involved has a continuous
             | emission spectrum or not.
        
               | renox wrote:
               | I'm not so sure: 'black body' are made of atoms, atoms
               | emits lights only on certain frequency due to the way
               | electrons orbitals are structured, with discrete energy
               | levels, but I don't see how this is related to EM fields
               | themselves..
        
         | gnramires wrote:
         | I think that although light is a quantum phenomenon and we can
         | detect single photons, many people overlook that photons still
         | behave similarly to Maxwell's (wave) equations. In particular,
         | the average behavior is that of the electromagnetic wave (up to
         | some extremes like extremely high energies). The 'bullet' model
         | people think of when the word photon (particle) is mentioned is
         | inadequate. This becomes clear in field theory (QED and QFT),
         | where there's a more complete description based of this
         | phenomena solely based on field (wavelike) behavior. It's
         | believe any (small) system follows QFT exactly (there's still
         | uncertainty around gravity).
         | 
         | The exact nature of the relationship of quantumness and fields
         | (i.e. how the single-particle behavior arises from QFT) is
         | still unclear, which is why there are many competing
         | interpretations of quantum mechanics. In the Copenhagen
         | interpretation, which is the most "easy" one, the behavior of
         | photons is just (almost) that of Maxwell's equations, on
         | average, s.t. a single photon will be measured with probability
         | equal to the average light intensity anywhere (they are said to
         | "collapse" at the moment of measurement, which is surely a
         | simplification of a more complete underlying theory).
        
         | roesel wrote:
         | The magnitue drop is reasonably simple to understand in terms
         | of fields. The oscillating optical field might be less
         | effective at exciting material oscillations in the middle
         | filter due to a mismatch in polarization, but it _still does so
         | at the same frequency_. You can think of it as multiple photons
         | (incoming field) collectively exciting the same electron on the
         | same frequency but with reduced efficiency. The electron then
         | re-emits fewer photons (outgoing field) of the same wavelength,
         | leading to a lower light intensity detected after the filter.
        
           | Arwill wrote:
           | I don't think photons are absorbed and re-emitted by
           | electrons. At least that argument does not hold when
           | discussing light slowing down in glass or water. Light is
           | affected by the electromagnetic field of the material it is
           | going trough, is slowed down, or absorbed based on some of
           | its property, but photons that go trough are going trough
           | without collision. Photons that get absorbed and re-emitted
           | are scattered in all directions, and are mostly lost. You
           | would not see a consistent image trough a polarising
           | sunglass, if the photons you were seeing were re-emitted
           | photons.
        
         | Sharlin wrote:
         | The polarization of a single photon is a quantum property, so
         | it's essentially a probability distribution. Passing a photon
         | through a polarizer modifies the probability distribution such
         | that "more perpendicular" polarizations are now less likely and
         | "more parallel" ones more likely. (Polarization is a
         | superposition (ie. a linear combination) of two orthogonal
         | basis vectors, and a polarizer projects a polarization vector
         | onto one of the basis vectors.)
        
       | nh23423fefe wrote:
       | Isn't this backward? Usually polarization is the analogy used to
       | explain stern-gerlach.
       | 
       | I dont get the desire to cast light as something non quantum...
        
         | fsh wrote:
         | The quantum nature of light is extremely difficult to observe.
         | Almost all laboratory experiments can be explained using
         | Maxwell's equations and the quantization of the electric charge
         | (this explains why photodetectors "click"). Photons usually
         | only show up when higher-order correlation functions are
         | analyzed.
        
         | bowsamic wrote:
         | > I dont get the desire to cast light as something non quantum.
         | 
         | Because you can describe it entirely using classical physics in
         | this situation
        
       | yuan43 wrote:
       | Trying to make sure I understand this.
       | 
       | According to the article, the "spookiness" comes from a
       | misunderstanding of what a polarizer does. It doesn't "block" all
       | light polarized on axes different from the polarizer. We know
       | this is true because otherwise sunglasses would transmit much
       | less light than they do. Imagine sunglasses could block any
       | photon within +/- 1 degree of the polarization plane. That means
       | that just 1/180th of the light would get through. But the
       | observed transmission is much higher.
       | 
       | Instead, the polarizer does two things. First, it emits light
       | polarized parallel to its axis. But, and this is the key, _all_
       | incident light gets effectively passed. Along the way the
       | intensity (amplitude, or  "magnitude" in the article) is
       | attenuated based on deviation from the polarizer's plane. The
       | attenuation is 0% for light polarized in parallel and 100% for
       | light polarized perpendicularly.
       | 
       | Now we can understand the experiment with a new mental model.
       | Three filters are placed in series (A, B, and C). However, we can
       | disregard A for the most part and treat this as a two-filter
       | system (B, C), where the light exiting B is attenuated relative
       | to the light entering A and polarized along B's axis. This model
       | explains all of the observations.
        
       | klodolph wrote:
       | > These results can be verified by performing the experiment with
       | an actual light meter -- the meter should show about twice as
       | strong a reading in the Figure 1 arrangement as it does in the
       | Figure 3 arrangement.
       | 
       | Quantum mechanics predicts that the difference is a factor of 4,
       | not a factor of 2.
        
       | rahimnathwani wrote:
       | I came across this on Twitter. Someone had posted an image of the
       | same experiment, and said they used it to teach their kid about
       | quantum effects.
       | 
       | Several replies explained how the effect can be explained without
       | quantum mechanics.
       | 
       | This article (linked in one of those comments) is so clear, and
       | I'm amazed I haven't seen it on HN before.
        
         | bowsamic wrote:
         | That thread was a huge mess of confusion and misinformation. I
         | hope I managed to dispel some confusions there
        
       | roesel wrote:
       | While this explanation is very nice, it still does not actually
       | explain what is happening on a material level.
       | 
       | The light does not "pass" through the middle filter, but it
       | excites oscillations in the material, which effectively re-emits
       | the light with different properties. The incoming light polarized
       | at 0deg induces oscillations in electrons which are "bound to a
       | rail" in the material, which allows them to only oscillate in the
       | direction of 45deg (and all oscillations in the direction of
       | -45deg are absorbed). Therefore, a portion of the incoming field
       | essentially gets re-emitted _by_ the middle filter linearly
       | polarized at 45deg.
       | 
       | This representation is much less helpful if you think of the
       | light in terms of individual photons rather than fields of
       | course, but it is not worse than the article in this regard
       | either.
        
         | function_seven wrote:
         | If the material is being excited into oscillations that then
         | re-emit "new" light, how is the color and direction preserved?
         | Polarization filters tend to pass the full spectrum (or nearly
         | so) of visible light, but my understanding of photon absorption
         | and emittance is that the wavelengths are dependent on the
         | electron energy levels. (I'm thinking of the same mechanism
         | that produces lines on a spectrometer, indicating which
         | elements are present in a sample.)
         | 
         | I guarantee I've misused a term or two above. Hopefully you get
         | what I'm asking.
         | 
         | Taking a stab at my own question, the "rails" are field lines
         | within the material, and not electrons themselves that
         | interact. Is that close?
        
           | amluto wrote:
           | It's because the "re-emission" is coherent in the sense that
           | it's in the same phase as the incoming light. As a decent
           | analogy: when you sing a pure note, it "excites" (vibrates)
           | air molecules as it travels, and those air molecules in turn
           | bump into other molecules, all at random, but still all in
           | phase so that whoever is listening hears the original note.
           | Similarly, when light goes through ordinary glass, it wiggles
           | the electrons in the glass, which in turn change the way the
           | light propagates, refracting it while still preserving an
           | image.
           | 
           | Any textbook on electricity and magnetism will cover this in
           | a section called something like "Maxwell's equations in
           | materials".
        
         | moralestapia wrote:
         | Is it photons in -> (new) photons out? Or the same ones
         | reoriented?
        
           | NotYourLawyer wrote:
           | It's new photons being emitted.
        
             | amluto wrote:
             | I disagree. Photons don't have identity - you can't
             | distinguish old from new. This is true of all bosons, and
             | it's quite important to how they behave.
        
               | moralestapia wrote:
               | (Interesting) Could you elaborate?
        
       | avodonosov wrote:
       | The concern that the article presents - that the middle filter
       | influences the light and thus allows it to pass through the third
       | filter - is actually addressed in popular quantum mechanics
       | explanations that use the 3 filter experiment.
       | 
       | They say that if we use two entangled photons and let them fly
       | far apart, then pass one of them through two filters, and the
       | second photon through the middle filter, the first photon will be
       | affected - it will get a chance to pass though the pair of
       | filters.
       | 
       | That they say is "spooky action at distance" - the second photon
       | will influence behaviour of the first photon at the remote site
       | of the experiment and the "influence" is faster then the speed of
       | light.
       | 
       | Example here by MinutePhysics and 3Blue1Brown:
       | https://youtu.be/zcqZHYo7ONs Explanation about entanglement
       | starts at around 8:50.
       | 
       | But even with that addressed, to me personally this video is not
       | satisfying.
       | 
       | If the spooky action at distance can be observed so trivially -
       | choosing a filter at one site site affects what happens at the
       | remote site - we don't need a mathematical inequality (the Bell's
       | inequality), it's already so obviously spooky.
       | 
       | There are also serious problems with clarity of their
       | explanation, as I commented in
       | https://www.youtube.com/watch?v=zcqZHYo7ONs&lc=Ugz3tzpDP_i1N...
       | and
       | https://www.youtube.com/watch?v=zcqZHYo7ONs&lc=Ugz3tzpDP_i1N...
       | 
       | I am not sure the real Bell experiments are really done using 3
       | polarizing filters and will the effect really be observed in
       | experiment with two remote sites.
       | 
       | My conclusion, it's problematic to rely on "pupular science"
       | explanations, even by good channels like MinutePhysics and
       | 3Blue1Brown.
        
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