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Native point defects in CuIn$_{1-x}$Ga$_x$Se$_{2}$: hybrid density functional calculations predict origin of p- and n-type conductivity

机译:CuIn $ _ {1-x} $ Ga $ _x $ se $ _ {2} $:混合密度中的原生点缺陷   功能计算预测p-和n-型电导率的起源

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摘要

We have performed a first-principles study of the p- and n-type conductivityin CuIn$_{1-x}$Ga$_x$Se$_{2}$ due to native point defects, based on the HSE06hybrid functional. Band alignment shows that the band gap becomes larger with$x$ due to the increasing conduction band minimum, rendering it hard toestablish n-type conductivity in CuGaSe$_{2}$. From the defect formationenergies, we find that In/Ga$_{\mathrm{Cu}}$ is a shallow donor, whileV$_{\mathrm{Cu}}$, V$_{\mathrm{In}/\mathrm{Ga}}$ andCu$_{\mathrm{In}/\mathrm{Ga}}$ act as shallow acceptors. Using total chargeneutrality of ionized defects and intrinsic charge carriers to determine theFermi level, we show that under In-rich growth conditions In$_{\mathrm{Cu}}$causes strongly n-type conductivity in CuInSe$_{2}$. Under In-poor growthconditions the conductivity type in CuInSe$_{2}$ alters to p-type andcompensation of the acceptors by In$_{\mathrm{Cu}}$ reduces, as observed inphotoluminescence experiments. In CuGaSe$_{2}$, the native acceptors pin theFermi level far away from the conduction band minimum, thus inhibiting n-typeconductivity. On the other hand, CuGaSe$_{2}$ shows strong p-type conductivityunder a wide range of Ga-poor growth conditions. Maximal p-type conductivity inCuIn$_{1-x}$Ga$_x$Se$_{2}$ is reached under In/Ga-poor growth conditions, inagreement with charge concentration measurements on samples with In/Ga-poorstoichiometry, and is primarily due to the dominant acceptorCu$_{\mathrm{In}/\mathrm{Ga}}$.
机译:基于HSE06混合函数,由于自然点缺陷,我们已经对CuIn $ _ {1-x} $ Ga $ _x $ Se $ _ {{2} $]中的p型和n型电导率进行了第一性原理研究。能带对准显示,由于导带最小值的增加,带隙随着$ x $的增大而变大,使得难以在CuGaSe $ _ {2} $中建立n型电导率。从缺陷形成能中,我们发现In / Ga $ _ {\ mathrm {Cu}} $是浅层供体,而V $ _ {\ mathrm {Cu}} $,V $ _ {\ mathrm {In} / \ mathrm {Ga}} $和Cu $ _ {\ mathrm {In} / \ mathrm {Ga}} $充当浅受体。使用离子化缺陷和内在电荷载流子的总电荷中性来确定费米能级,我们表明在In-In生长条件下,In $ _ {\ mathrm {Cu}} $在CuInSe $ _ {{2} $}中具有很强的n型导电性。如在光致发光实验中所观察到的,在贫乏生长条件下,CuInSe $ _ {2} $中的电导率类型变为p型,并且In $ _ {\ mathrm {Cu}} $中受体的补偿减小。在CuGaSe $ _ {2} $中,天然受体将费米能级固定在远离导带最小值的位置,从而抑制了n型电导率。另一方面,CuGaSe $ _ {2} $在多种Ga贫乏生长条件下均显示出强p型导电性。在In / Ga贫乏的生长条件下,达到CuIn $ _ {1-x} $ Ga $ _x $ Se $ _ {2} $的最大p型电导率,并同意采用In / Ga不足化学计量法对样品进行电荷浓度测量,并且主要归因于主导受体Cu $ _ {\ mathrm {In} / \ mathrm {Ga}} $。

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