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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

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