Photons and physical interpretation of Fourier transform

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SUMMARY

The discussion centers on the relationship between Fourier transforms and photon energies in electromagnetic waves. It establishes that non-sinusoidal waves can be decomposed into sinusoidal components via Fourier transforms, with the energy of photons related to frequency by the equation E=h·f. However, it questions the assumption that abrupt changes in waveforms, such as switching a radiofrequency wave on and off, introduce higher frequency components in the Fourier transform that correspond to higher energy photons. The consensus is that while Fourier analysis may indicate higher frequencies, the actual photon energies remain unchanged under these conditions.

PREREQUISITES
  • Understanding of Fourier transforms and their application in wave analysis
  • Knowledge of electromagnetic wave theory and photon energy relations
  • Familiarity with the equation E=h·f and its implications
  • Basic concepts of wave modulation and its effects on frequency components
NEXT STEPS
  • Research the implications of Fourier transform in quantum mechanics
  • Study the effects of pulse modulation on electromagnetic waves
  • Explore the relationship between time-domain signals and frequency-domain representations
  • Investigate the principles of wave packet formation and their relation to photon energies
USEFUL FOR

Physicists, electrical engineers, and students studying wave phenomena and quantum mechanics will benefit from this discussion, particularly those interested in the intersection of Fourier analysis and photon energy concepts.

Jarl
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When we study physics at the faculty we are told that any non-sinusoidal wave can be regarded as a combination of sinusoidal waves of different frecuencies, with the ‘weight’ of the different frecuencies given by the Fourier transform. On the other hand, if we have an electromagnetic wave, we know that it is the combined result of many photons of different energies, and it is generally assumed that the interval of the Fourier space where Fourier transform is not zero gives us the energies of the photons in the beam, through the famous relation E=h·f.

However, if we have a radiofrecuency wave (for example), and we switch it on and off abruptly, we introduce much higher frecuencies in the Fourier transform ¿does it mean that we’ll have photons at these high frecuencies?. It is hard to believe so.

A more clear case, a continuous (cuasi)monocromatic wave source, a detector, and a shutter between them. For the source, the radiation have only one frecuency, but after the shutter, the Fourier transform of the wave has also higher frecuencies. The photons, however shouldn’t have more energy.

So ¿in which cases or under which conditions can we relate the ‘matematical’ frecuencies given by Fourier analysis with photons energies?
 
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Switching the beam on and off does not generate higher frequency components, it generates low-frequency components at the rate that you are switching the beam on and off.
 
berkeman said:
Switching the beam on and off does not generate higher frequency components, it generates low-frequency components at the rate that you are switching the beam on and off.

If we allow the wave to pass only during some short time (i.e, only a pulse) we introduce high frecuencies in the Fourier transform.
Anyway, the Fourier transform is modified in some way, while the photon energies shouldn't change.The question is about it.
 

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