Radiation from a continually-accelerating electron

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    Electron Radiation
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SUMMARY

The discussion centers on the behavior of electromagnetic (EM) radiation emitted by a continuously-accelerating electron, contrasting it with the discrete energy level transitions in atoms. Participants clarify that the jumps between stationary states in atoms are interpretations rather than direct consequences of Schrödinger's equation. The wave function of an electron changes continuously according to differential equations, influenced by external fields. The outcomes for a specific electron are not strictly defined by quantum theory, allowing for various interpretations such as Brownian motion and Bohm's theory.

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sshai45
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Hi.

I was wondering about this. According to the quantum theory, all EM radiation is made up of discrete units -- photons. So what happens in something like with an electron or other charged particle being accelerated continuously, as opposed to discretely flipping between energy levels like in an atom?
 
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sshai45,

the jumps between the stationary states in atom you mention are not a consequence of Schroedinger's equation; they are just an interpretation of the ( expansion coefficients of the wave function into eigenbasis of H0 ).

What happens mathematically to the wave function is that it changes continuously according to differential equation, with its center most probably accelerating due to external field. The only thing we can do is to look at the function and try to interpret it somehow, usually as probability density in configuration or momentum space.

What happens to one particular electron is not determined by quantum theory; it can jump, it can move erraticaly (Brownian motion), it can move continuously ( Bohm's theory)...
 

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