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

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6.3. Results and Discussion 85<br />

distribution function. Thus we again divided the spectra by the FD function (convoluted<br />

with a Gaussian corresponding to the energy resolution) as shown in the lower<br />

panel <strong>of</strong> the figure. The spectral DOS thus obtained is found to increase with increasing<br />

temperature in a rather wide energy region between EF and ∼−100 meV.<br />

Intensity<br />

DOS<br />

LuB 12<br />

hν = 21.2 eV<br />

300 K<br />

225 K<br />

150 K<br />

75 K<br />

7 K<br />

300 K<br />

225 K<br />

150 K<br />

75 K<br />

7 K<br />

LuB 12<br />

-150 -100 -50 0 50 100<br />

Energy relative to E F (meV)<br />

Figure 6.6: Temperature-dependent He I photoemission spectra <strong>of</strong> LuB12 (upper panel)<br />

and those divided by the FD function convoluted with the instrumental resolution<br />

(lower panel).<br />

We note again that the intensity at EF in the spectra divided by the convoluted<br />

FD function does not depend on uncertainties in the temperature nor the Gaussian<br />

width, because the FD function is 0.5 at EF at any temperature even if that FD<br />

function is convoluted with any Gaussian. However, an error in the temperature or the<br />

Gaussian width might cause a spurious temperature dependence near EF in the FDfunction-divided<br />

spectra. The fact that temperature dependence is more remarkable

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