Do X-Ray Tracks in Photo Film Suggest Quantum Entanglement?

In summary, Roland Omnes says that hard x-rays can leave straight-line tracks in photographic emulsion and this is strongly reminiscent of a particle trajectory. He goes on to explain that this is because the x-ray beam consists of a number of photons and the wavefunction for the photons collapses when they interact with the liquid in the photograph.
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Swamp Thing
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In Understanding Quantum Mechanics, Ch.1, Sec. 5 Roland Omnes says:
".. hard x-rays can leave straight-line tracks in photographic emulsion and this is strongly reminiscent of a particle trajectory."

How can we describe this in terms of the wavefunction / interaction / measurement paradigm? Is is a series of "position measurments" -- one measurement at each grain of the emulsion? And presumably, a grain of emulsion would have to absorb at most a tiny part of the photon's energy if we are to see many more absorptions further along the track. This seems to fly in the face of "all-or-nothing" annihilation of photons. And what of the expected "collapse" that should occur at each grain?
 
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Swamp Thing said:
In Understanding Quantum Mechanics, Ch.1, Sec. 5 Roland Omnes says:
".. hard x-rays can leave straight-line tracks in photographic emulsion and this is strongly reminiscent of a particle trajectory."

How can we describe this in terms of the wavefunction / interaction / measurement paradigm? Is is a series of "position measurments" -- one measurement at each grain of the emulsion? And presumably, a grain of emulsion would have to absorb at most a tiny part of the photon's energy if we are to see many more absorptions further along the track. This seems to fly in the face of "all-or-nothing" annihilation of photons. And what of the expected "collapse" that should occur at each grain?

I'm not sure I understand your problem here. It appears as if you think "x-ray" beam consists of only ONE photon. It doesn't. There are a gazillion photons in an x-ray beam, the beam has some penetration depth. This means that while there is a fraction of the photons that interact at a certain depth of the material, others pass through unimpeded. And this continues through the thickness of the material until there's no more material, or until there's no more x-ray photons.

Transpose this process to the photographic plate, and that's why you see a track.

Zz.
 
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If the film is exposed long enough, yes there will be "gazillions" of blackened grains / dots (not linear tracks) that will collectively form a dark area on the film. If this is what is meant in the text then it's fine. But I understood it to be talking about a countable number of photons whose individual tracks can be seen, like particle tracks in a cloud chamber.
 
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  • #4
Swamp Thing said:
But I understood it to be talking about a countable number of photons whose individual tracks can be seen, like particle tracks in a cloud chamber.

That problem was solved by Nevill Mott in 1929. You'll find a bunch of threads here and googling for "Mott problem" or "Mott paradox" will find more, including Mott's original paper.

A handwaving qualitative and heuristic explanation is that the initial state of the particle is indeed an expanding spherically symmetric wave. However, that wave function collapses when the particle interacts with one of the droplets of suspended liquid; and Mott showed that the subsequent evolution of that post-interaction wave function leads to a state in which there is a very high probability that the next droplet in the interaction will be a little further away in the same general direction. Of course that's for charged particles in a cloud chamber, but a similar analysis works for photons propagating through a light-sensitive emulsion.
 
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Nugatory said:
That problem was solved by Nevill Mott in 1929. You'll find a bunch of threads here and googling for "Mott problem" or "Mott paradox" will find more, including Mott's original paper.

A handwaving qualitative and heuristic explanation is that the initial state of the particle is indeed an expanding spherically symmetric wave. However, that wave function collapses when the particle interacts with one of the droplets of suspended liquid; and Mott showed that the subsequent evolution of that post-interaction wave function leads to a state in which there is a very high probability that the next droplet in the interaction will be a little further away in the same general direction. Of course that's for charged particles in a cloud chamber, but a similar analysis works for photons propagating through a light-sensitive emulsion.
Thank you.
 
  • #6
Pondering over Nugatory's reply led me to wonder if it makes sense to talk of "entanglement" in this context.

Consider a number of photo grains that happen to lie along a classically possible path (e.g. a radial line going outward from the emitting region). The final state of the grains is significantly correlated -- either you will see a lot of grains on this line that have blackened, or you won't see any blackened grains. On the other hand, if we examine grains that don't lie on the same radial path then there would be no particular correlation among them. So the passage of the x-ray wave has left each radially located set of grains in a correlated (entangled) condition).

So my question again - is it valid to call this an 'entanglement' scenario?
 
  • #7
Swamp Thing said:
So the passage of the x-ray wave has left each radially located set of grains in a correlated (entangled) condition).
Entanglement implies correlation, but correlation does not necessarily imply entanglement - it's easy to find correlations that are not caused by entanglement.

So my question again - is it valid to call this an 'entanglement' scenario?

Only to the extent that any measurement can be thought of as an entanglement of the measuring apparatus with the quantum system being measured... And that's one of the ways into the swamp of never-ending interpretational debate.

A droplet in a cloud chamber or a granule of photosensitive emulsion is not isolated from the environment and quite large enough that decoherence will knock down any superpositions of blackened and not-blackened - and there can be no entanglement without superposition.
 

What are X-Ray tracks in photo film?

X-ray tracks in photo film are patterns of black or grey lines that are created when X-rays pass through the film. These tracks are a result of the interaction between the X-rays and the silver halide crystals in the film.

How are X-Ray tracks produced in photo film?

X-ray tracks are produced when high-energy X-rays pass through the film and interact with the silver halide crystals. The X-rays cause the crystals to change into a form that can be developed into visible tracks on the film. The more X-rays that pass through the film, the more tracks will be produced.

What is the significance of X-Ray tracks in photo film?

X-ray tracks in photo film are important because they can be used to create images of the internal structures of objects. X-rays are able to pass through objects that are opaque to visible light, allowing for the visualization of bones, organs, and other structures inside the body.

How can X-Ray tracks be used in scientific research?

X-ray tracks in photo film have many applications in scientific research. They can be used to study the structure and composition of materials, to detect defects in objects, and to analyze the effects of radiation on different materials. They are also commonly used in medical imaging to diagnose diseases and injuries.

How can X-Ray tracks be detected and measured?

X-ray tracks can be detected and measured using various techniques, such as densitometry, autoradiography, and scanning electron microscopy. These methods involve analyzing the patterns of tracks on the film and converting them into numerical data, which can then be used to quantify the amount of X-rays that passed through the film.

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