{"title":"NJL模型中夸克物质张量自能引起的自旋极化","authors":"T. Maruyama, T. Tatsumi","doi":"10.7566/jpscp.26.024020","DOIUrl":null,"url":null,"abstract":"We study the magnetic properties of quark matter in the NJL model including the tensor interaction. There are two kinds of spin-polarized phases: one appears in the chiral-broken phase, and the other in the chiral-restored phase where the quark mass is zero. The latter phase can appear independently of the strength of the tensor interaction.","PeriodicalId":175849,"journal":{"name":"Proceedings of the 8th International Conference on Quarks and Nuclear Physics (QNP2018)","volume":"35 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2019-11-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Spontaneous Spin Polarization due to Tensor Selfenergies in Quark Matter in NJL Model\",\"authors\":\"T. Maruyama, T. Tatsumi\",\"doi\":\"10.7566/jpscp.26.024020\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We study the magnetic properties of quark matter in the NJL model including the tensor interaction. There are two kinds of spin-polarized phases: one appears in the chiral-broken phase, and the other in the chiral-restored phase where the quark mass is zero. The latter phase can appear independently of the strength of the tensor interaction.\",\"PeriodicalId\":175849,\"journal\":{\"name\":\"Proceedings of the 8th International Conference on Quarks and Nuclear Physics (QNP2018)\",\"volume\":\"35 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2019-11-08\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Proceedings of the 8th International Conference on Quarks and Nuclear Physics (QNP2018)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.7566/jpscp.26.024020\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Proceedings of the 8th International Conference on Quarks and Nuclear Physics (QNP2018)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.7566/jpscp.26.024020","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Spontaneous Spin Polarization due to Tensor Selfenergies in Quark Matter in NJL Model
We study the magnetic properties of quark matter in the NJL model including the tensor interaction. There are two kinds of spin-polarized phases: one appears in the chiral-broken phase, and the other in the chiral-restored phase where the quark mass is zero. The latter phase can appear independently of the strength of the tensor interaction.