4 ms·

You know that is all happening according to Schroedinger’s equation, right?

by kgwgk 7y ago

scotty79 7y ago
Culling of the the wave function due to absorbtion by the atoms of the barrier that happens or not with some probability is a consequence of Schrodinger equation? I thought it describes evolution of the wave function in spacetime empty or not (like around nucleus) but doesn't cover any kind of decay, absorptions, emmisions and such. --- We reached max thread depth and I can't reply to your response. Not sure if you are going to see this. If you are using electrons instead of photons for double slit experiment barrier still absorbs them. They get caught by atoms of the barrier or exchange virtual photons with electrons of the barrier. Shrodinger doesn't cover that I think.
- kgwgk 7y ago
  Absorption of what? If you’re talking about photons, strictly speaking they are not described by Schroedinger’s equation at all (it applies to massive, non-relativistic particles). The double-slit experiment is often discussed in quantum mechanics in terms of matter waves (having interferences in light is not particularly surprising anyway).
- kgwgk 7y ago
  In principle you can model the interaction between the electrons and the particles in the barrier and the whole system evolves according to Schroedinger’s equation and will be described by a wavefunction. This wavefunction may be a superposition of states where the electron goes through the slits and states where it doesn’t. Until there is a “measurement” - a “detection” which is “amplified” - you cannot say what has happened to the electron: every outcome remains possible and the system remains described by a wavefunction. If the detection happens first at the screen there will be a probability of finding the electron at each position and a probability of not finding it at all. Note that the detection on the screen is done using a scintillator/photomultiplier or something like that to amplifify the detection of a single electron into a measurable electric signal.

You know that is all happening according to Schroedinger’s equation, right?

by kgwgk 7y ago

You know that is all happening according to Schroedinger’s equation, right?

Culling of the the wave function due to absorbtion by the atoms of the barrier that happens or not with some probability is a consequence of Schrodinger equation? I thought it describes evolution of the wave function in spacetime empty or not (like around nucleus) but doesn't cover any kind of decay, absorptions, emmisions and such. --- We reached max thread depth and I can't reply to your response. Not sure if you are going to see this. If you are using electrons instead of photons for double slit experiment barrier still absorbs them. They get caught by atoms of the barrier or exchange virtual photons with electrons of the barrier. Shrodinger doesn't cover that I think.

kgwgk 7y ago
Absorption of what? If you’re talking about photons, strictly speaking they are not described by Schroedinger’s equation at all (it applies to massive, non-relativistic particles). The double-slit experiment is often discussed in quantum mechanics in terms of matter waves (having interferences in light is not particularly surprising anyway).
kgwgk 7y ago
In principle you can model the interaction between the electrons and the particles in the barrier and the whole system evolves according to Schroedinger’s equation and will be described by a wavefunction. This wavefunction may be a superposition of states where the electron goes through the slits and states where it doesn’t. Until there is a “measurement” - a “detection” which is “amplified” - you cannot say what has happened to the electron: every outcome remains possible and the system remains described by a wavefunction. If the detection happens first at the screen there will be a probability of finding the electron at each position and a probability of not finding it at all. Note that the detection on the screen is done using a scintillator/photomultiplier or something like that to amplifify the detection of a single electron into a measurable electric signal.