- #36
DParlevliet
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In case 1, supposing only a layer of atoms, does it leave a record, does it change frequency (you told it did change phase)
DParlevliet said:In case 1, supposing only a layer of atoms, does it leave a record, does it change frequency (you told it did change phase)
DParlevliet said:Does "leaving a record" not always change frequency and/or phase?
DParlevliet said:Is the loss of interference not basicly caused by the loss of coherence of the photon, regardless if it leaves a record or not?
DParlevliet said:That is better. Now we have only physical properties. I don't like the impression (also in above topic) that the pattern disappers just because nature want to prevent us knowing what is happening.
But if the photon leaves the detector it is distibuted again (when you place a new 2-slit after that, it again gives a interference pattern). In a mirror also the photon is absorbed and emitted by one atom and becomes distributed again. Unless you suppose there is a relation between the distrubuted before and after the mirror. That looks not QM.
DParlevliet said:That's right (and you pass nicely the remark about distribution :)
Back to case 1: now I understand what effect you mean. But X-ray diffraction is based on coherent scattering of photons by atoms according the Thomson effect. It radiates in all directions, so also forward. So I think case 1 could be made to have an interference pattern. For the discussion it does not matter.
which is bound to an atom. I did mean everything what happens in a atom. It differs if with Thomson (it was called "effect" in my very very old learning book) the photon is not absorbed by the atom/free charged particle, but only sacttered.craigi said:Regarding your case 1, Thomson scattering isn't a photon interaction with an atom. It occurs when a photon interacts with a free charged particle.
DParlevliet said:which is bound to an atom. I did mean everything what happens in a atom. It differs if with Thomson (it was called "effect" in my very very old learning book) the photon is not absorbed by the atom/free charged particle, but only sacttered.
A mirror is that also based on the Thomson effect?
DParlevliet said:Perhaps it was Handbook of X-rays from Kaeble (1967). So:
on what principle is X-ray differaction based?
on what principle is a mirror based?
Then I can search furthre on that.
X-ray diffraction is based on Rayleigh scattering. But in articles of both never the physical background is explained. So this leaves open the possibility that it is not based on absorption-emisioncraigi said:Just search for specular reflection and x-ray diffraction.
DParlevliet said:X-ray diffraction is based on Rayleigh scattering. But in articles of both never the physical background is explained. So this leaves open the possibility that it is not based on absorption-emision
After some thinking I am less satisfied with this.craigi said:Coherent superposition is required for the interference pattern to emerge, which requires the particle to maintain a coherent phase and frequency and have a distributed position. If you take one of these away then, the photon can't contribute to an interference pattern.
DParlevliet said:After some thinking I am less satisfied with this.
- Phase is right (when uncorrellated, not fixed). With one photon there will be interference (there are positions on the detector where the photon will never arrive). But with multiple photons it is not possible to build up a measurable pattern.
- Frequency: Suppose a detector exists which emits a new photon with lower frequency but fixed phase. Then according classical wave still interference would be possible. But transferring higher to lower frequency with fixed phase is essential not possible. So the basic reason here is also uncorrellated phase.
- Distributed position: as mentioned before, after leaving the detector the photon is a wave again, so a distributed position. There is no difference with the photon before the detector.