How to find effective mass of electron in real semiconductor?
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The effective mass of a semiconductor is obtained by fitting
the actual E-k diagram around the conduction band minimum or the
valence band maximum by a parabola. While this concept is simple
enough the issue turns out to be substancially more complex due to
the multitude and the occasional anisotropy of the minima and maxima. In this section
we first describe the different relevant band minima and maxima, present the
numeric values for germanium, silicon and gallium arsenide and introduce
the effective mass for density of states calculations and the effective mass
for conductivity calculations.
Most semiconductors can be described as having one band minimum at k = 0 as well as several equivalent anisotropic band minima at k ¹ 0. In addition there are three band maxima of interest which are close to the valence band edge.
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