{"title":"n型和p型CuInTe2的电学和光学性质","authors":"S. Wasim, J. G. Albornóz","doi":"10.1002/PSSA.2211100231","DOIUrl":null,"url":null,"abstract":"The electrical properties between 80 and 300 K and the optical absorption at room temperature of both n- and p-type CuInTe2 are studied. The n-type sample is obtained by annealing p-type CuInTe2 in the presence of indium for a prolonged period of time. The p-type samples are grown by programmed directional freezing technique with slight excess of indium in the stoichiometry. Two defect levels with ED = 58 meV and EA around 15 meV are identified from the analysis of the temperature dependence of the carrier concentration. The origin of these levels, consistent with the covalent bonding model, is attributed to InCu and VTe, respectively. From a theoretical fit to the experimental data, the density of states effective mass of the electrons is found to be m = 0.16me. The estimated values of the conduction and valence-band deformation potentials are in agreement with the general trend observed in other I–III–VI2 compounds. Using the model proposed for the band-gap shrinkage, the energy gap of n-type CuInTe2 in the dilute limit is calculated to be 1.026 eV. On a etudie les proprietes electriques entre 80 et 300 K, et l'absorption optique a temperature ambiante de CuInTe2 type n et type p. L'echantillon type n a ete obtenu par recuit et celuit type p par mise en presence de l'Indium durant une periode de temps prolonge. On a fait croǐtre les echantillons type p par la technique de refroidissement directionnel programme avec un leger exces d'Indium dans la stoechiometrie. Par l'analyse de la dependance de la temperature de concentration des porteurs, on a identifie deux niveaux de defauts avec ED = 58 meV et EA environ 15 meV. L'origine de ces niveaux, compatible avec le modele de liaison covalente, est attribue it a InCu et a VTe, respectivement. Apres un ajustement theorique aux donnees experimentales, la densite des etats de la masse effective des electrons est de m★ = 0,16me. Les valeurs estimees des potentiels de deformation des bandes de conduction et de valence sont en accord avec la tendance generale observee dans les composes I–III–VI2. En utilisant le modele propose pour la contraction de la bande du gap, le resultat de gap d'energie de CuInTe2 type n dans la limite diluee est de 1,026 eV.","PeriodicalId":90917,"journal":{"name":"Machine learning and interpretation in neuroimaging : international workshop, MLINI 2011, held at NIPS 2011, Sierra Nevada, Spain, December 16-17, 2011 : revised selected and invited contributions. MLINI (Workshop) (2011 : Sierra Nevada...","volume":"31 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"1988-12-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"38","resultStr":"{\"title\":\"Electrical and Optical Properties of n- and p-Type CuInTe2\",\"authors\":\"S. Wasim, J. G. Albornóz\",\"doi\":\"10.1002/PSSA.2211100231\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The electrical properties between 80 and 300 K and the optical absorption at room temperature of both n- and p-type CuInTe2 are studied. The n-type sample is obtained by annealing p-type CuInTe2 in the presence of indium for a prolonged period of time. The p-type samples are grown by programmed directional freezing technique with slight excess of indium in the stoichiometry. Two defect levels with ED = 58 meV and EA around 15 meV are identified from the analysis of the temperature dependence of the carrier concentration. The origin of these levels, consistent with the covalent bonding model, is attributed to InCu and VTe, respectively. From a theoretical fit to the experimental data, the density of states effective mass of the electrons is found to be m = 0.16me. The estimated values of the conduction and valence-band deformation potentials are in agreement with the general trend observed in other I–III–VI2 compounds. Using the model proposed for the band-gap shrinkage, the energy gap of n-type CuInTe2 in the dilute limit is calculated to be 1.026 eV. On a etudie les proprietes electriques entre 80 et 300 K, et l'absorption optique a temperature ambiante de CuInTe2 type n et type p. L'echantillon type n a ete obtenu par recuit et celuit type p par mise en presence de l'Indium durant une periode de temps prolonge. On a fait croǐtre les echantillons type p par la technique de refroidissement directionnel programme avec un leger exces d'Indium dans la stoechiometrie. Par l'analyse de la dependance de la temperature de concentration des porteurs, on a identifie deux niveaux de defauts avec ED = 58 meV et EA environ 15 meV. L'origine de ces niveaux, compatible avec le modele de liaison covalente, est attribue it a InCu et a VTe, respectivement. Apres un ajustement theorique aux donnees experimentales, la densite des etats de la masse effective des electrons est de m★ = 0,16me. Les valeurs estimees des potentiels de deformation des bandes de conduction et de valence sont en accord avec la tendance generale observee dans les composes I–III–VI2. En utilisant le modele propose pour la contraction de la bande du gap, le resultat de gap d'energie de CuInTe2 type n dans la limite diluee est de 1,026 eV.\",\"PeriodicalId\":90917,\"journal\":{\"name\":\"Machine learning and interpretation in neuroimaging : international workshop, MLINI 2011, held at NIPS 2011, Sierra Nevada, Spain, December 16-17, 2011 : revised selected and invited contributions. 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引用次数: 38
摘要
研究了n型和p型CuInTe2在80 ~ 300 K范围内的电学性能和室温下的光吸收。将p型CuInTe2在铟存在下长时间退火得到n型样品。p型样品采用程序定向冷冻技术生长,化学计量中铟含量略超标。通过分析载流子浓度的温度依赖性,确定了ED = 58 meV和EA约为15 meV的两个缺陷能级。这些水平的起源,与共价键模型一致,分别归因于InCu和VTe。从理论拟合到实验数据,发现电子的态密度有效质量为m = 0.16me。传导电位和价带变形电位的估计值与其他I-III-VI2化合物中观察到的一般趋势一致。利用提出的带隙收缩模型,计算出n型CuInTe2在稀极限下的能隙为1.026 eV。在一个实验中,在80 ~ 300 K的温度范围内,有1种吸收光,温度环境为CuInTe2型和p型。1种吸收光,温度环境为CuInTe2型和p型。事实上,croǐtre les echantilons type p - parla technique de refrodisdisdisdirectnel programme在法律上超过了d'Indium dans和stohi计量学。第二部分分析了在一个确定的双系统默认条件下,温度和浓度的相关性,平均ED = 58 meV, EA环境为15 meV。原始的、兼容的、连接共价的、可分别归属于InCu和VTe的模型。根据实验条件下的调整理论,得到了质量有效电子的密度值= 0.16 μ m。莱斯的值估计的des potentiels de传导的变形des·邦德:不吸烟者价是在协议用拉照顾兴业银行observee在I-III-VI2作曲。在实用模型中,提出了一种压缩带隙的方法,使得闭合带隙的能量达到了CuInTe2型的极限稀释值为1026 eV。
Electrical and Optical Properties of n- and p-Type CuInTe2
The electrical properties between 80 and 300 K and the optical absorption at room temperature of both n- and p-type CuInTe2 are studied. The n-type sample is obtained by annealing p-type CuInTe2 in the presence of indium for a prolonged period of time. The p-type samples are grown by programmed directional freezing technique with slight excess of indium in the stoichiometry. Two defect levels with ED = 58 meV and EA around 15 meV are identified from the analysis of the temperature dependence of the carrier concentration. The origin of these levels, consistent with the covalent bonding model, is attributed to InCu and VTe, respectively. From a theoretical fit to the experimental data, the density of states effective mass of the electrons is found to be m = 0.16me. The estimated values of the conduction and valence-band deformation potentials are in agreement with the general trend observed in other I–III–VI2 compounds. Using the model proposed for the band-gap shrinkage, the energy gap of n-type CuInTe2 in the dilute limit is calculated to be 1.026 eV. On a etudie les proprietes electriques entre 80 et 300 K, et l'absorption optique a temperature ambiante de CuInTe2 type n et type p. L'echantillon type n a ete obtenu par recuit et celuit type p par mise en presence de l'Indium durant une periode de temps prolonge. On a fait croǐtre les echantillons type p par la technique de refroidissement directionnel programme avec un leger exces d'Indium dans la stoechiometrie. Par l'analyse de la dependance de la temperature de concentration des porteurs, on a identifie deux niveaux de defauts avec ED = 58 meV et EA environ 15 meV. L'origine de ces niveaux, compatible avec le modele de liaison covalente, est attribue it a InCu et a VTe, respectivement. Apres un ajustement theorique aux donnees experimentales, la densite des etats de la masse effective des electrons est de m★ = 0,16me. Les valeurs estimees des potentiels de deformation des bandes de conduction et de valence sont en accord avec la tendance generale observee dans les composes I–III–VI2. En utilisant le modele propose pour la contraction de la bande du gap, le resultat de gap d'energie de CuInTe2 type n dans la limite diluee est de 1,026 eV.