- #1
enwa
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Why does an atom emit discrete frequencies of light?
Solving the Schrodinger wave function for the hydrogen atom (that is a single particle representing an electron bound by a spherical potential) we find that it has discrete energy levels. Plotting every possible value of [itex]f[/itex] in [itex]E'-E = \hbar f[/itex] where [itex]E'[/itex] and [itex]E[/itex] are the different energy levels of eigenstates we recover the emission spectra.
What I don't understand is why we only see these discrete energy levels. According to the superposition principle, the wave function could be in a superposition with expected energy [itex]\tfrac{1}{2}(E'+E)[/itex] but differences from these levels don't show up on the emission spectra. The measurement postulate seems relevant, "measurement" collapses a wave function into an eigenstate, this seems to be happening before and after the photon emission, can anyone explain why?
Solving the Schrodinger wave function for the hydrogen atom (that is a single particle representing an electron bound by a spherical potential) we find that it has discrete energy levels. Plotting every possible value of [itex]f[/itex] in [itex]E'-E = \hbar f[/itex] where [itex]E'[/itex] and [itex]E[/itex] are the different energy levels of eigenstates we recover the emission spectra.
What I don't understand is why we only see these discrete energy levels. According to the superposition principle, the wave function could be in a superposition with expected energy [itex]\tfrac{1}{2}(E'+E)[/itex] but differences from these levels don't show up on the emission spectra. The measurement postulate seems relevant, "measurement" collapses a wave function into an eigenstate, this seems to be happening before and after the photon emission, can anyone explain why?