Wave propagation, resonance and collapse

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SUMMARY

The discussion centers on wave propagation, specifically regarding the behavior of photons and their interaction with atoms. It is established that the wavefunction, denoted as ψ(x, t), represents the probability amplitude for locating a particle at a specific point in space and time. The interaction between a photon and an atom can occur at any point where the wavefunction is nonzero, indicating that wave collapse does not strictly depend on the wavefront meeting an absorber but can happen within the traversed volume of the field. This understanding challenges classical interpretations of energy transfer in wave phenomena.

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  • Understanding of quantum mechanics and wavefunctions
  • Familiarity with the concept of probability amplitudes
  • Knowledge of photon behavior and atomic interactions
  • Basic principles of wave propagation in physics
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This discussion is beneficial for physicists, quantum mechanics students, and anyone interested in the intricacies of wave-particle interactions and the foundational concepts of quantum theory.

yeshi
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Hello,

there is a subject of wave propagation and collapse that has plagued me for some time, and although i must have heard about it, my memories are probably skewed ( i studied EE and had high frequency, physics of materials and nuclear/quantum physics sometime in 1970s :) as subjects). In the online textbooks i was unable to find an answer. My views are somewhat of an EE, that holds fast to antenna and fields, etc. :-p

Question:
When the wave propagates - let's say a single photon - it is my understanding that it will discharge when a resonant candidate (absorber) is reached in space(time) and will ionise an atom by changing an electron in some of its orbitals.

If we look at a wave as a propagating phenomenon traveling from the emitter at speed c (media dependent) then it has a wavefront, maybe an expanding sphere in vacuum or some other form.

Does it mean that the wave can collapse only if the wavefront meets a potential recipient (atom) on its expansion, or can the discharge happen WITHIN the already transversed volume of the field? In other words, is the wave collapse always happening when the absorber is reached along the wavefront expansion?

thank you in advance
 
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yeshi, The wavefunction that we talk about, ψ(x, t), is the probability amplitude for finding the particle at point x at time t. An interaction may take place anywhere that ψ(x, t) is nonzero. The other terms you use, discharge and resonant absorber, make the process sound way too continuous and way too classical. It is not like a wave gradually transferring energy to a receiving antenna. The interaction, if it occurs, occurs at a single point at a single instant.
 
Bill_K said:
yeshi, The wavefunction that we talk about, ψ(x, t), is the probability amplitude for finding the particle at point x at time t. An interaction may take place anywhere that ψ(x, t) is nonzero. The other terms you use, discharge and resonant absorber, make the process sound way too continuous and way too classical. It is not like a wave gradually transferring energy to a receiving antenna. The interaction, if it occurs, occurs at a single point at a single instant.

excellent,

so the interaction can occur at a point within the volume already traversed (as the wavefuncion is nonzero within all of the field (aka volume)). Thank you :)

OTOH, there is an emitter and absorber atom for each photon out there, and it does propagate in real time...
 

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