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Fermi integral and density-of-states functions in a parabolic band semiconductor degenerately doped with impurities forming a band tail

机译:费米积分和状态密度函数在简并地掺杂有杂质的抛物线形带半导体中形成带尾

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We provide the energy spectrum of an electron in a degenerately doped semiconductor of parabolic band. Knowing the energy spectrum, the density-of-states (DOS) functions are obtained, considering the Gaussian distribution of the potential energy of the impurity states, showing a band tail in them e.g., energy spectrum and density-of-states. Therefore, Fermi integrals (FIs) of DOS functions, having band tail, are developed by the exact theoretical calculations of the same. It is noticed that with heavy dopings in semiconductors, the total FI demonstrates complex functions, containing both real and imaginary terms of different FI functions. Their moduli possess an oscillatory function of $eta$ (reduced Fermi energy = $E_{f}/k_{B}T, k_{B}$ is the Boltzmann constant and $T$ is the absolute temperature) and $eta e$ (impurity screening potential), having a series solutions of confluent hypergeometric functions, $Phi(a, b; z)$, superimposed with natural cosine functions of angle $heta$. The variation of $heta$ with respect to $eta$ indicated resonance at $eta$ = 1.5. The oscillatory behaviour of FIs show the existence of a??band-gapsa??, both in the real as well as in the forbidden bands as new band gaps in the semiconductor.
机译:我们提供了抛物带的简并掺杂半导体中电子的能谱。知道了能谱,考虑了杂质态势能的高斯分布,获得了状态密度(DOS)函数,并在其中显示了能带尾部,例如,能谱和状态密度。因此,具有带尾的DOS函数的费米积分(FI)是通过精确的理论计算得出的。值得注意的是,在半导体中大量掺杂时,总FI表现出复杂的功能,其中包含不同FI功能的实项和虚项。它们的模量具有$ eta $的振荡函数(费米能量降低= $ E_ {f} / k_ {B} T,k_ {B} $是玻尔兹曼常数,$ T $是绝对温度)和$ eta e $(杂质筛查潜能),具有一系列融合的超几何函数, Phi(a,b; z)$,并与角$ theta的自然余弦函数叠加。 $ theta $相对于$ eta $的变化表示在$ eta $ = 1.5时产生共振。 FI的振荡行为表明在半导体带中的实带和禁带中都存在“带隙”。

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