Qiurun Wang, Ting Wu, F. Han, B. Peng, Wanli Zhang, Wenxu Zhang
{"title":"方法获得坡莫合金/正常金属双分子层的反自旋霍尔效应电压","authors":"Qiurun Wang, Ting Wu, F. Han, B. Peng, Wanli Zhang, Wenxu Zhang","doi":"10.1109/INEC.2016.7589376","DOIUrl":null,"url":null,"abstract":"In this work, the inverse spin Hall effect was separated from the spin rectification effect by two methods. One is originated from that the inverse spin Hall effect which is an odd function of the spin injection direction while the spin rectification effect is independent on it. The second method is based on the relation between the direction of static magnetic field and the symmetric and anti-symmetric components of voltage.","PeriodicalId":416565,"journal":{"name":"2016 IEEE International Nanoelectronics Conference (INEC)","volume":"134 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2016-05-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Methods to obtain the inverse spin hall effect voltage in permalloy/normal metal bilayer\",\"authors\":\"Qiurun Wang, Ting Wu, F. Han, B. Peng, Wanli Zhang, Wenxu Zhang\",\"doi\":\"10.1109/INEC.2016.7589376\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"In this work, the inverse spin Hall effect was separated from the spin rectification effect by two methods. One is originated from that the inverse spin Hall effect which is an odd function of the spin injection direction while the spin rectification effect is independent on it. The second method is based on the relation between the direction of static magnetic field and the symmetric and anti-symmetric components of voltage.\",\"PeriodicalId\":416565,\"journal\":{\"name\":\"2016 IEEE International Nanoelectronics Conference (INEC)\",\"volume\":\"134 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2016-05-09\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2016 IEEE International Nanoelectronics Conference (INEC)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/INEC.2016.7589376\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2016 IEEE International Nanoelectronics Conference (INEC)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/INEC.2016.7589376","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Methods to obtain the inverse spin hall effect voltage in permalloy/normal metal bilayer
In this work, the inverse spin Hall effect was separated from the spin rectification effect by two methods. One is originated from that the inverse spin Hall effect which is an odd function of the spin injection direction while the spin rectification effect is independent on it. The second method is based on the relation between the direction of static magnetic field and the symmetric and anti-symmetric components of voltage.