兴奋剂
价(化学)
接受者
能量(信号处理)
类型(生物学)
物理
结晶学
材料科学
凝聚态物理
化学
量子力学
生态学
生物
作者
Xuefen Cai,Fernando P. Sabino,Anderson Janotti,Su‐Huai Wei
出处
期刊:Physical review
[American Physical Society]
日期:2021-03-22
卷期号:103 (11)
被引量:36
标识
DOI:10.1103/physrevb.103.115205
摘要
$P$-type doping in oxides is usually difficult due to their low valence-band energy. In order to make them $p$ type, the electronic structure of the oxides should be fundamentally changed; that is, the occupied valence band should be raised significantly. Here, using first-principles calculations, we propose that by adding a small amount of ${\mathrm{Bi}}_{2}{\mathrm{O}}_{3}$ into ${\mathrm{Ga}}_{2}{\mathrm{O}}_{3}$ to form dilute ${({\mathrm{Bi}}_{x}{\mathrm{Ga}}_{1--x})}_{2}{\mathrm{O}}_{3}$ alloys and, more importantly, with properly chosen dopants, we can achieve efficient $p$-type doping in a transparent oxide. We show that adding a few percent of Bi to ${\mathrm{Ga}}_{2}{\mathrm{O}}_{3}$ leads to an intermediate valence band that is sufficiently high in energy to facilitate $p$-type doping; however, the commonly expected shallow acceptors, Mg and Zn substitution on the Ga site (${\mathrm{Mg}}_{\mathrm{Ga}}$ and ${\mathrm{Zn}}_{\mathrm{Ga}}$), are still deep acceptors, whereas the expected deep acceptor, ${\mathrm{Cu}}_{\mathrm{Ga}}$, actually creates a relatively shallow level in ${({\mathrm{Bi}}_{x}{\mathrm{Ga}}_{1--x})}_{2}{\mathrm{O}}_{3}$ alloys. This trend is opposite to what is found in pure ${\mathrm{Ga}}_{2}{\mathrm{O}}_{3}$. The puzzling behavior of the acceptor levels in the ${({\mathrm{Bi}}_{x}{\mathrm{Ga}}_{1--x})}_{2}{\mathrm{O}}_{3}$ alloys is attributed to the polaronic character of the holes in the Zn- and Mg-doped cases, and the decoupling of the hole state and the valence-band edge in the Cu-doped case. This understanding provides insights into the realization of $p$-type doping in dilute ${({\mathrm{Bi}}_{x}{\mathrm{Ga}}_{1--x})}_{2}{\mathrm{O}}_{3}$ alloys and paves a way to dope semiconductor materials with a strongly correlated band edge state, i.e., materials with a tendency to form polaronic acceptor or donor states.
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