C. Jayasankar, E. Antic-Fidancev, M. Blaise, P. Porcher
{"title":"Optical Properties of EuF3 and GdF3 and Paramagnetic Susceptibility of EuF3","authors":"C. Jayasankar, E. Antic-Fidancev, M. Blaise, P. Porcher","doi":"10.1002/PSSB.2221330140","DOIUrl":null,"url":null,"abstract":"The optical properties of EuF3 and GdF3 are reinvestigated. Crystal field parameters derived from the data by using the D3h C2v descending symmetry procedure for EuF3 are (in cm−1): B = 465, B = 375, B = −232, B = −96, B = −114, B = −490, B = 83, B = −518, B = −162. The temperature dependent paramagnetic susceptibility of EuF3, is calculated by using the simulated wave functions. The calculated and experimental paramagnetic susceptibilities are in very good agreement. \n \n \n \nLes proprietes optiques de EuF3 et GdF3 ont ete reexaminees. A partir des niveaux observes, les parametres de champ cristallin ont ete determines par la methode de symetrie descendante D3h C2v pour EuF3 les parametres sont: B = 465, B = 375, B = −232, B = −96, B = −114, B = −490, B = 83, B = −518, B = −162 (en cm−1). En outre, l'evolution en fonction de la temperature de la susceptibilite paramagnetique de EuF3 a ete calculee grace aux fonctions d'onde deduites de la simulation. L'accord entre l'experience et le calcul est excellent.","PeriodicalId":11087,"journal":{"name":"Day 1 Tue, January 11, 2022","volume":"50 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"1986-12-31","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"12","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Day 1 Tue, January 11, 2022","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1002/PSSB.2221330140","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 12
Abstract
The optical properties of EuF3 and GdF3 are reinvestigated. Crystal field parameters derived from the data by using the D3h C2v descending symmetry procedure for EuF3 are (in cm−1): B = 465, B = 375, B = −232, B = −96, B = −114, B = −490, B = 83, B = −518, B = −162. The temperature dependent paramagnetic susceptibility of EuF3, is calculated by using the simulated wave functions. The calculated and experimental paramagnetic susceptibilities are in very good agreement.
Les proprietes optiques de EuF3 et GdF3 ont ete reexaminees. A partir des niveaux observes, les parametres de champ cristallin ont ete determines par la methode de symetrie descendante D3h C2v pour EuF3 les parametres sont: B = 465, B = 375, B = −232, B = −96, B = −114, B = −490, B = 83, B = −518, B = −162 (en cm−1). En outre, l'evolution en fonction de la temperature de la susceptibilite paramagnetique de EuF3 a ete calculee grace aux fonctions d'onde deduites de la simulation. L'accord entre l'experience et le calcul est excellent.
重新研究了EuF3和GdF3的光学性质。利用D3h C2v下降对称法得到的EuF3晶体场参数(单位cm−1)为:B = 465, B = 375, B =−232,B =−96,B =−114,B =−490,B = 83, B =−518,B =−162。利用模拟波函数计算了EuF3的温度随顺磁化率。顺磁化率的计算值与实验值吻合较好。EuF3和GdF3的所有权对复试者无效。一组研究人员观察到,在对称的派生方法D3h - C2v - EuF3中,有两个参数:B = 465, B = 375, B = - 232, B = - 96, B = - 114, B = - 490, B = 83, B = - 518, B = - 162 (en cm - 1)。在此基础上,推导出了EuF3的温度演化函数和磁化顺磁性函数,并计算了EuF3的温度演化函数和磁化顺磁性函数。L'accord中心,L 'experience中心,L' compute中心,优秀。