Electromagnetic radiation and perturbation

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Discussion Overview

The discussion revolves around the treatment of electromagnetic radiation effects on the Hamiltonian of matter as a perturbation. Participants explore the reasons for this approach, particularly focusing on the relative magnitude of radiation effects compared to other influences in various physical systems.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants suggest that electromagnetic waves contribute very little to the Hamiltonian, often less than 0.1%, justifying their treatment as a perturbation.
  • Others note that each additional photon introduces a factor of e² (approximately 1/137), reinforcing the idea that radiation effects are minimal.
  • A participant questions the assumption that radiation effects are negligible, pointing out that a large number of photons could significantly impact the system.
  • Another participant proposes a simple model relating the electric field of an atom to the charge of the nucleus and distance, suggesting that the amplitude of the electric field from electromagnetic waves could be considered large.
  • It is mentioned that while E₀ can be large, using very powerful, focused lasers may invalidate the perturbative approach.
  • A calculation of energy density in a weak laser setup is suggested, with an emphasis on deriving the average electric field from that energy density.

Areas of Agreement / Disagreement

Participants express differing views on the significance of electromagnetic radiation effects, with some asserting they are negligible while others argue that a large number of photons could lead to significant effects. The discussion remains unresolved regarding the extent to which radiation can be treated as a perturbation.

Contextual Notes

Limitations include assumptions about the strength of electromagnetic fields, the conditions under which perturbation theory is valid, and the specific setups being discussed. The calculations and models referenced may depend on particular definitions and contexts that are not fully explored.

hokhani
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Why do we often treat the electromagnetic radiation effects on Hamiltonian of a matter as a perturbation? In the other words, why the effects of radiation is so little that is treated as a perturbation?
 
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You can calculate the electric field strength in atoms and in electromagnetic waves (both with classical formulas) - in many setups, the waves are a very small contributions (<<0.1%).
 
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Each extra photon brings in a factor e^2, which equals 1/137 so "radiation is so little that is treated as a perturbation."
 
Meir Achuz said:
Each extra photon brings in a factor e^2, which equals 1/137 so "radiation is so little that is treated as a perturbation."
Ok, Thanks. But we have a great number of photons that seem to affect the system significantly. How about that? Am I wrong about that?
 
hokhani said:
Ok, Thanks. But we have a great number of photons that seem to affect the system significantly. How about that? Am I wrong about that?
Did you calculate the values I suggested?
 
mfb said:
Did you calculate the values I suggested?
In a very simple model, we can take the electric field of an atom proportional to [itex] q/r^2[/itex] in which q is the charge of nucleus and r is distance from its center. An electromagnetic wave is [itex] E=E_0 exp(-i\omega t)[/itex].I think we can consider [itex] E_0[/itex] as large as possible; can't we? Could you please guide me If I am wrong?
 
E0 can be very large, but then you need really powerful, focused lasers, and the perturbative approach does not work any more.

The energy density of an electric field in vacuum is ##\frac{\epsilon}{2} E^2##. Take a typical, weak laser with 1mW/mm^2, calculate the energy density, and calculate the average electric field based on that. The value is somewhere at a few V/cm.
 
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