Copyright by Kirsten Viering 2006 - Raizen Lab - The University of ...
Copyright by Kirsten Viering 2006 - Raizen Lab - The University of ...
Copyright by Kirsten Viering 2006 - Raizen Lab - The University of ...
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Chapter 2<br />
Interaction <strong>of</strong> atoms with<br />
non-resonant light<br />
In this chapter we give a brief introduction into the theory <strong>of</strong> the interaction <strong>of</strong> atoms<br />
with non-resonant light. We restrict the treatment to purely monochromatic light and<br />
use a semi-classical expression for the interaction Hamiltonian.<br />
2.1 Time-dependant Schrödinger equation<br />
A dynamical quantum mechanical system is described <strong>by</strong> the time-dependant Schrödinger-<br />
equation<br />
H|Ψ(r, t)〉 = i ∂<br />
|Ψ(r, t)〉. (2.1)<br />
∂t<br />
For the interaction <strong>of</strong> atoms with light this equation cannot be solved analytically.<br />
Hence we will use perturbation theory and treat the time-dependant electro-magnetic<br />
light field as a perturbation [6]. We separate the total Hamiltonian H(t) into two terms,<br />
H(t) = H0 +H ′ (t), where H0 is time independant; the explicit time dependance is treated<br />
in H ′ (t) as perturbation to the solution <strong>of</strong> the stationary Schrödinger-equation.<br />
<strong>The</strong> solution to the time-independant Schrödinger equation is given <strong>by</strong> the<br />
3