Photon Energy & Wave Amplitude

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    Amplitude Photon Wave
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SUMMARY

The energy of a photon is defined by the equation E=hv, where v represents the frequency, a fundamental wave property. Wave amplitude relates to the expectation value of photon number, indicating that it does not pertain to individual photon properties but rather to the total number of photons present. This discussion clarifies misconceptions regarding the treatment of photons within quantum mechanics, emphasizing the necessity of quantizing the electromagnetic field instead of treating photons as classical particles. The canonical commutation relations and the Fock space framework are essential for understanding photon interactions and energy density.

PREREQUISITES
  • Understanding of quantum mechanics principles, particularly wave-particle duality.
  • Familiarity with the equation E=hv and its implications in photon energy calculations.
  • Knowledge of electromagnetic field quantization and its significance in particle physics.
  • Basic comprehension of Fock space and canonical commutation relations.
NEXT STEPS
  • Study the quantization of electromagnetic fields in detail.
  • Learn about the Fock space representation in quantum mechanics.
  • Research the implications of the Coulomb gauge and radiation gauge in quantum field theory.
  • Explore the concept of photon number eigenstates and their role in energy density calculations.
USEFUL FOR

This discussion is beneficial for physicists, quantum mechanics students, and researchers in particle physics who are exploring the relationship between photon energy, wave amplitude, and the quantization of electromagnetic fields.

jeremyfiennes
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TL;DR
Where does a photon's wave amplitude enter into its energy equation?
A photon's energy is E=hv where v, the frequency, is a wave property. Particles don't have frequencies. But a wave's energy also depends on its amplitude. Where does this come into the energy relation?
 
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jeremyfiennes said:
a wave's energy also depends on its amplitude. Where does this come into the energy relation?

Wave amplitude corresponds to the expectation value of photon number (more precisely, to the square root of it). So in the photon model it has nothing to do with the properties of individual photons; it's just how many photons there are.
 
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This seems to be the typical misconception arising from the misunderstanding that one could treat photons with a wave function as in non-relativistic Schrödinger quantum mechanics. That's not the case. The electromagnetic field is what has to be quantized, because photon number is not conserved but photons can easily be created and destroyed in interactions of charged particles.

The free field, describing asymptotic free states is normalized such as to obey the canonical commutation relations in, say, the Coulomb gauge (or for free fields the "radiation gauge" following from it). Then you can define momentum-eigenmodes of single free photons and build the entire Fock space from the photon-number eigenstates. The total energy density is then given as an expectation value with respect to the states. A single photon in a single-frequency mode always has the energy ##\hbar \omega##, no more no less, and all you can say about this photon is the probability that it's detected by some detector. It's always detected as a whole or nothing.
 

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