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Thesis High-Resolution Photoemission Study of Kondo Insulators ...

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Chapter 2<br />

<strong>Photoemission</strong> Spectroscopy<br />

In this Chapter we present general principles and experimental technique <strong>of</strong> photoemission<br />

spectroscopy. In the section <strong>of</strong> the general principles, we express a formulation <strong>of</strong><br />

photoemission spectrum and then show how to deduce spectral density <strong>of</strong> states (DOS)<br />

from measured photoemission spectra. In the section <strong>of</strong> the technique, we give some<br />

remarks on a pumping system for photoemission spectroscopy with a He discharge lamp<br />

and then explain a background correction for the photoemission spectra taken with a<br />

He lamp.<br />

2.1 General Principles<br />

2.1.1 Formulation <strong>of</strong> <strong>Photoemission</strong> Spectrum<br />

First we present the formulation <strong>of</strong> photoemission spectrum following Gunnarsson and<br />

Schönhammer [2.1]. We assume a transition from the initial ground state |E0(N) > to<br />

the final states ψ †<br />

k |En(N − 1) >, where the emitted electron |k >has no interaction<br />

with the remaining (N − 1) electrons1 . The golden rule gives the number <strong>of</strong> emitted<br />

electrons with the energy <strong>of</strong> ɛout as<br />

P < (ɛout) = � �<br />

k<br />

where τ = �<br />

ki<br />

n<br />

| | 2 δ(ɛout−ɛk)δ(ɛout+En(N−1)−hν−E0(N))<br />

(2.1)<br />

τkiψ †<br />

k ψi represents the transition induced by photons with a matrix ele-<br />

ment τki between the one-electron states |i >and |k >. With a further assumption <strong>of</strong><br />

1 This approximation becomes more accurate as the kinetic energy <strong>of</strong> the emitted electron increases.<br />

17

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