{"title":"Aspects of Quark Orbital Angular Momentum","authors":"M. Burkardt","doi":"10.1142/9789811214950_0051","DOIUrl":null,"url":null,"abstract":"The difference between the quark orbital angular momentum (OAM) defined in light-cone gauge (Jaffe-Manohar) compared to defined using a local manifestly gauge invariant operator (Ji) is interpreted in terms of the change in quark OAM as the quark leaves the target in a DIS experiment.","PeriodicalId":215936,"journal":{"name":"Probing Nucleons and Nuclei in High Energy Collisions","volume":"227 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2020-01-11","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Probing Nucleons and Nuclei in High Energy Collisions","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1142/9789811214950_0051","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
The difference between the quark orbital angular momentum (OAM) defined in light-cone gauge (Jaffe-Manohar) compared to defined using a local manifestly gauge invariant operator (Ji) is interpreted in terms of the change in quark OAM as the quark leaves the target in a DIS experiment.