首页> 外文期刊>Pramana >Electronic structure and band alignments of ${mbox{ZnTe} mathord{left/ {vphantom {mbox{ZnTe} {mbox{CrTe(0 0 1)}}}} right. kern-0em} {mbox{CrTe}}}(0 0 1)$ , ${mbox{CdSe} mathord{left/ {vphantom {mbox{CdSe} {mbox{CrTe(0 0 1)}}}} right. kern-0em} {mbox{CrTe}}}(0 0 1)$ and ${mbox{CdTe} mathord{left/ {vphantom {mbox{CdTe} {mbox{CrTe(0 0 1)}}}} right. kern-0em} {mbox{CrTe}}}(0 0 1)$ interfaces
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Electronic structure and band alignments of ${mbox{ZnTe} mathord{left/ {vphantom {mbox{ZnTe} {mbox{CrTe(0 0 1)}}}} right. kern-0em} {mbox{CrTe}}}(0 0 1)$ , ${mbox{CdSe} mathord{left/ {vphantom {mbox{CdSe} {mbox{CrTe(0 0 1)}}}} right. kern-0em} {mbox{CrTe}}}(0 0 1)$ and ${mbox{CdTe} mathord{left/ {vphantom {mbox{CdTe} {mbox{CrTe(0 0 1)}}}} right. kern-0em} {mbox{CrTe}}}(0 0 1)$ interfaces

机译:$ {mbox {ZnTe} mathord {left / {vphantom {mbox {ZnTe} {mbox {CrTe(0 0 1)}}}}右的电子结构和能带对准。 kern-0em} {mbox {CrTe}}}(0 0 1)$,$ {mbox {CdSe} mathord {left / {vphantom {mbox {CdSe}} {mbox {CrTe(0 0 1)}}}}右。 kern-0em} {mbox {CrTe}}}(0 0 1)$和$ {mbox {CdTe} mathord {left / {vphantom {mbox {CdTe}} {mbox {CrTe(0 0 1)}}}}}右。 kern-0em} {mbox {CrTe}}}(0 0 1)$接口

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摘要

All-electron full potential calculations based on spin density functional theory were performed to study cubic zincblende (ZB) and hexagonal NiAs structures of bulk CrTe and ${mbox{ZnTe} mathord{left/ {vphantom {mbox{ZnTe} {mbox{CrTe(0 0 1)}}}} right. kern-0em} {mbox{CrTe}}}(0 0 1)$ , ${mbox{CdTe} mathord{left/ {vphantom {mbox{CdTe} {mbox{CrTe(0 0 1)}}}} right. kern-0em} {mbox{CrTe}}}(0 0 1)$ and ${mbox{CdSe} mathord{left/ {vphantom {mbox{CdSe} {mbox{CrTe(0 0 1)}}}} right. kern-0em} {mbox{CrTe}}}(0 0 1)$ interfaces. The lattice mismatch effect in ZB CrTe and magnetic properties of CrTe in the ideal ZB CrTe structure were investigated. The band alignment properties of the ${mbox{ZnTe} mathord{left/ {vphantom {mbox{ZnTe} {mbox{CrTe(0 0 1)}}}} right. kern-0em} {mbox{CrTe}}}(0 0 1)$ , ${mbox{CdTe} mathord{left/ {vphantom {mbox{CdTe} {mbox{CrTe(0 0 1)}}}} right. kern-0em} {mbox{CrTe}}}(0 0 1)$ and ${mbox{CdSe} mathord{left/ {vphantom {mbox{CdSe} {mbox{CrTe(0 0 1)}}}} right. kern-0em} {mbox{CrTe}}}(0 0 1)$ interfaces were computed and a rather large minority valence band offset of about 1.09 eV was observed in ${mbox{ZnTe} mathord{left/ {vphantom {mbox{ZnTe} {mbox{CrTe(0 0 1)}}}} right. kern-0em} {mbox{CrTe}}}(0 0 1)$ heterojunction. Also in the ${mbox{CdTe} mathord{left/ {vphantom {mbox{CdTe} {mbox{CrTe(0 0 1)}}}} right. kern-0em} {mbox{CrTe}}}(0 0 1)$ and ${mbox{CdSe} mathord{left/ {vphantom {mbox{CdSe} {mbox{CrTe(0 0 1)}}}} right. kern-0em} {mbox{CrTe}}}(0 0 1)$ interfaces, the conduction band minimum of minority spin in CrTe was above the conduction band minimum of CdTe and CdSe and so the majority spin electrons could be directly injected to both semiconductors, indicating the possibility of highly efficient spin injection into the CdSe and CdTe semiconductors.
机译:进行了基于自旋密度泛函理论的全电子全势计算,以研究块状CrTe和$ {mbox {ZnTe} mathord {left / {vphantom {mbox {ZnTe}} {mbox {CrTe (0 0 1)}}}}对。 kern-0em} {mbox {CrTe}}}(0 0 1)$,$ {mbox {CdTe} mathord {left / {vphantom {mbox {CdTe}} {mbox {CrTe(0 0 1)}}}}右。 kern-0em} {mbox {CrTe}}}(0 0 1)$和$ {mbox {CdSe} mathord {left / {vphantom {mbox {CdSe}} {mbox {CrTe(0 0 1)}}}}}右。 kern-0em} {mbox {CrTe}}}(0 0 1)$接口。研究了理想ZB CrTe结构中ZB CrTe中的晶格失配效应和CrTe的磁性。 $ {mbox {ZnTe} mathord {left / {vphantom {mbox {ZnTe}} {mbox {CrTe(0 0 1)}}}} right的波段对齐属性。 kern-0em} {mbox {CrTe}}}(0 0 1)$,$ {mbox {CdTe} mathord {left / {vphantom {mbox {CdTe}} {mbox {CrTe(0 0 1)}}}}右。 kern-0em} {mbox {CrTe}}}(0 0 1)$和$ {mbox {CdSe} mathord {left / {vphantom {mbox {CdSe}} {mbox {CrTe(0 0 1)}}}}}右。 kern-0em} {mbox {CrTe}}}(0 0 1)$接口被计算,在$ {mbox {ZnTe} mathord {left / {vphantom {mbox { ZnTe} {mbox {CrTe(0 0 1)}}}}。 kern-0em} {mbox {CrTe}}}(0 0 1)$异质结。同样在$ {mbox {CdTe} mathord {left / {vphantom {mbox {CdTe}} {mbox {CrTe(0 0 1)}}}}}右中。 kern-0em} {mbox {CrTe}}}(0 0 1)$和$ {mbox {CdSe} mathord {left / {vphantom {mbox {CdSe}} {mbox {CrTe(0 0 1)}}}}}右。 kern-0em} {mbox {CrTe}}}(0 0 1)$接口,CrTe中少数自旋的导带最小值高于CdTe和CdSe的导带最小值,因此大多数自旋电子可以直接注入到两者半导体,这表明有可能将自旋注入CdSe和CdTe半导体。

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