{"title":"CoCl2.6H2O反铁磁共振;极化,频率和温度的影响","authors":"H. Benoit, W. Ghidalia","doi":"10.1016/0031-8914(74)90067-6","DOIUrl":null,"url":null,"abstract":"<div><p>The experimental study of the coupling between the magnetizations and the high-frequency field <em>h</em> allows us to observe four resonances <em>R</em><sub>1</sub>, <em>R</em><sub>2</sub>, <em>R</em><sub>3</sub>, <em>R</em><sub>4</sub> (at increasing resonance fields) with various polarizations. At hyperfrequencies, <em>R</em><sub>1</sub> and <em>R</em><sub>4</sub> are elliptically polarized in a plane normal to the cristallographic plane <em>bc</em>; the intersection of these two planes depends of the orientation of the d.c. field <em>H</em>. The polarization of the lines <em>R</em><sub>2</sub> and <em>R</em><sub>3</sub> is linear along <em>c</em>. This direction is independent of the orientation of <em>H</em>, within the experimental errors. At radio frequencies, the elliptical polarization of <em>RR</em><sub>1</sub> and <em>RR</em><sub>4</sub> is reduced to linear polarization in <em>bc</em> along the major axis of the ellipse. The resonances <em>R</em><sub>2</sub> and <em>R</em><sub>3</sub> remain polarized along <em>c</em>. The behaviour of these four resonances is studied as a function of the temperature and the frequency. At 1.91 K and at radio frequencies, the line shape depends strongly of the frequency.</p></div>","PeriodicalId":55605,"journal":{"name":"Physica","volume":"78 2","pages":"Pages 233-244"},"PeriodicalIF":0.0000,"publicationDate":"1974-12-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0031-8914(74)90067-6","citationCount":"2","resultStr":"{\"title\":\"Résonances antiferromagnétiques de CoCl2.6H2O; polarisation, influence de la fréquence et de la température\",\"authors\":\"H. Benoit, W. Ghidalia\",\"doi\":\"10.1016/0031-8914(74)90067-6\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>The experimental study of the coupling between the magnetizations and the high-frequency field <em>h</em> allows us to observe four resonances <em>R</em><sub>1</sub>, <em>R</em><sub>2</sub>, <em>R</em><sub>3</sub>, <em>R</em><sub>4</sub> (at increasing resonance fields) with various polarizations. At hyperfrequencies, <em>R</em><sub>1</sub> and <em>R</em><sub>4</sub> are elliptically polarized in a plane normal to the cristallographic plane <em>bc</em>; the intersection of these two planes depends of the orientation of the d.c. field <em>H</em>. The polarization of the lines <em>R</em><sub>2</sub> and <em>R</em><sub>3</sub> is linear along <em>c</em>. This direction is independent of the orientation of <em>H</em>, within the experimental errors. At radio frequencies, the elliptical polarization of <em>RR</em><sub>1</sub> and <em>RR</em><sub>4</sub> is reduced to linear polarization in <em>bc</em> along the major axis of the ellipse. The resonances <em>R</em><sub>2</sub> and <em>R</em><sub>3</sub> remain polarized along <em>c</em>. The behaviour of these four resonances is studied as a function of the temperature and the frequency. At 1.91 K and at radio frequencies, the line shape depends strongly of the frequency.</p></div>\",\"PeriodicalId\":55605,\"journal\":{\"name\":\"Physica\",\"volume\":\"78 2\",\"pages\":\"Pages 233-244\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1974-12-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://sci-hub-pdf.com/10.1016/0031-8914(74)90067-6\",\"citationCount\":\"2\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Physica\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/0031891474900676\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Physica","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/0031891474900676","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Résonances antiferromagnétiques de CoCl2.6H2O; polarisation, influence de la fréquence et de la température
The experimental study of the coupling between the magnetizations and the high-frequency field h allows us to observe four resonances R1, R2, R3, R4 (at increasing resonance fields) with various polarizations. At hyperfrequencies, R1 and R4 are elliptically polarized in a plane normal to the cristallographic plane bc; the intersection of these two planes depends of the orientation of the d.c. field H. The polarization of the lines R2 and R3 is linear along c. This direction is independent of the orientation of H, within the experimental errors. At radio frequencies, the elliptical polarization of RR1 and RR4 is reduced to linear polarization in bc along the major axis of the ellipse. The resonances R2 and R3 remain polarized along c. The behaviour of these four resonances is studied as a function of the temperature and the frequency. At 1.91 K and at radio frequencies, the line shape depends strongly of the frequency.