Quantum dot Quantum optics Nanocavity
Rabi model9

The Rabi model is a semi-classical model. This means that we use a classical representation of the field

  Equation 3.1 (3.1)

For the atom we use a quantized description, so the atom has two states; the ground state and the excited state

  Equation 3.2 (3.2)

The atom-field interaction is described by the interaction Hamiltonian

  Equation 3.3 (3.3)


  Equation 3.4 (3.4)

The interaction Hamiltonian can be seen as the energy flow between the atom and the field. The total Hamiltonian of a quantum mechanical atom-field interacting system is

  Equation 3.5 (3.5)

The free-atom Hamiltonian is

  Equation 3.6 (3.6)

We choose the energy of the ground state of the atom to be zero, so the free-atom Hamiltonian becomes

  Equation 3.7 (3.7)

Because we do not use a quantum field, there is no free-field Hamiltonian. So the total Hamiltonian becomes

  Equation 3.8 (3.8)

The state vector of the system is

  Equation 3.9 (3.9)

Substituting this expansion in the time-dependent Schrödinger equation

  Equation 3.10 (3.10)


  Equation 3.11 (3.11)

leads to the set of coupled first-order differential equations for the amplitudes

  Equation 3.12 (3.12)

As initial conditions we assume that all the population is in the ground state at t=0, so near t=0

  Equation 3.13 (3.13)

After we have expanded cos(ωt) in exponentials and apply the Rotating Wave Approximation (RWA, retain only the terms oscillating with ωeg) we obtain

  Equation 3.14 (3.14)

At this point we introduce the detuning Δ

  Equation 3.15 (3.15)

By integrating the differential equation 3.14, the solution is

  Equation 3.16 (3.16)


  Equation 3.17 (3.17)

is the Rabi frequency. The probability that the atom is in its excited state is

  Equation 3.18 (3.18)

Equation 3.18 is plotted in figure 9 for various values of the detuning Δ. The smaller the detuning the larger the probability of finding the atom in its excited state. If you want to see Rabi oscillations, you need an atom in its excited state (see figure 8). For the case of exact resonance, Δ = 0, we have at the time

  Equation 3.18 (3.63)

all the atomic population has been transferred to the excited state. This is the ideal situation for Rabi oscillations.

Probability that the atom is in state |e>
Figure 9: Plots of Pe(t) versus t for various detuning Δ 9

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