How Rabi frequency scales with laser intensity?

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SUMMARY

The Rabi frequency in a semiclassical model of a two-level atom interacting with a monochromatic field scales with laser intensity according to the relationship V² ∝ I, where intensity is proportional to the square modulus of the electric field amplitude E₀. Key approximations include the two-level approximation, which simplifies the wavefunction to a linear combination of two eigenstates, and the dipole approximation, which assumes the size of the wavefunctions is much smaller than the wavelength of the light. To achieve a Rabi frequency of Ω₁/2π = 1 MHz, the required laser intensity is calculated to be approximately 0.896 Js⁻¹m⁻², taking into account the time-averaged intensity in a medium with refractive index n.

PREREQUISITES
  • Understanding of semiclassical models in quantum mechanics
  • Familiarity with Rabi frequency and its derivation
  • Knowledge of electric field amplitude and intensity relationships
  • Basic concepts of two-level systems and dipole approximations
NEXT STEPS
  • Study the derivation of Rabi frequency in quantum mechanics
  • Learn about the dipole approximation in light-matter interactions
  • Explore the effects of damping in quantum systems
  • Investigate the time-averaged intensity calculations in different media
USEFUL FOR

Students and researchers in quantum mechanics, particularly those focusing on light-matter interactions, atomic physics, and laser applications. This discussion is beneficial for anyone studying Rabi oscillations and their dependence on laser intensity.

Mark Mendl
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Homework Statement


It's not a homework, I'm just studying for the exam, but one question that I'm not sure of the answer is:
"In the semiclassical model of a two-level atom interacting with a monochromatic field, how does the Rabi frequency scale with the laser intensity"

Homework Equations


rabi.png

Also, V=d*E0 (I'm not sure how to put formulas here, sorry)

The Attempt at a Solution


Do I assume no damping? Still, I think something is missing...
 
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Mark Mendl said:
In the semiclassical model of a two-level atom interacting with a monochromatic field, how does the Rabi frequency scale with the laser intensity
Well you can say ##V^2 \propto I## since intensity is proportional to the square modulus of the electric field amplitude ##E_0##. Several approximations assumed in arriving in that expression of Rabi frequency are:
1) Two participating levels approximation: Generally in tackling problems of time-dependent Hamiltonian, one uses the eigenstates of the time-independent part of the Hamiltonian as the bases into which the true wavefunction of the system is expanded, clearly there will be an infinite number of terms. However it can be simplified in the case where the frequency of the interacting light is close to the frequency difference of certain pair of eigenstates, and we can approximate the true wavefunction as a linear combination of only those two coupled eigenstates of the time-independent part of the Hamiltonian.
2) Dipole approximation: the "size" of the participating wavefunctions from point 1) be much smaller than the wavelength of the light the atom in question is interacting with.
 
Last edited:
Thank you for the answer, but for exemple in a more specific question in this model :
"We place a two-level atom with transition energy ħ*ω0 in a monochromatic laser field with
frequency ω. The transition dipole moment is d = 3ea0. a0= 5.29 x1011 m.
(a) Calculate the laser intensity needed to achieve a Rabi frequency Ω1/2π = 1MHz.
So, can I just use the formula above for Rabi frequency (ignoring damping) and the relation between the field and intensity? This would give me something like I=0.896 Js-1m-2
 
As far as I know, the Rabi oscillation frequency was originally derived in the quantum picture of light-matter interaction where only the atom is treated quantum mechanically, I have never known people incorporated the damping term in the Hamiltonian. May be you confused it with the purely classical Lorentz model.
ALso, you have to calculate the 'real' intensity, not just the square of E field. For plane wave in a medium of refractive index ##n##, the time averaged intensity is ##\frac{1}{2} \epsilon_0 nc |E_0|^2##.
 

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