{"title":"费曼积分之间的二次关系","authors":"D. Broadhurst","doi":"10.22323/1.303.0053","DOIUrl":null,"url":null,"abstract":"Feynman integrals come in two varieties: polylogarithmic, or \nnot. They are used in two ways: as contributions to an \namplitude that is squared, or as contributions to an \nobservable matrix element. In the former case, products of \nintegrals occur, in the latter they do not. We report on \nproducts of non-polylogarithmic Feynman integrals related to \nthe magnetic moment of the electron, giving details of an \ninfinite set of quadratic relations between these integrals \nat all loops $L>2$.","PeriodicalId":140132,"journal":{"name":"Proceedings of Loops and Legs in Quantum Field Theory — PoS(LL2018)","volume":"32 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2018-10-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"17","resultStr":"{\"title\":\"Quadratic relations between Feynman integrals\",\"authors\":\"D. Broadhurst\",\"doi\":\"10.22323/1.303.0053\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Feynman integrals come in two varieties: polylogarithmic, or \\nnot. They are used in two ways: as contributions to an \\namplitude that is squared, or as contributions to an \\nobservable matrix element. In the former case, products of \\nintegrals occur, in the latter they do not. We report on \\nproducts of non-polylogarithmic Feynman integrals related to \\nthe magnetic moment of the electron, giving details of an \\ninfinite set of quadratic relations between these integrals \\nat all loops $L>2$.\",\"PeriodicalId\":140132,\"journal\":{\"name\":\"Proceedings of Loops and Legs in Quantum Field Theory — PoS(LL2018)\",\"volume\":\"32 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2018-10-02\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"17\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Proceedings of Loops and Legs in Quantum Field Theory — PoS(LL2018)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.22323/1.303.0053\",\"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 Loops and Legs in Quantum Field Theory — PoS(LL2018)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.22323/1.303.0053","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Feynman integrals come in two varieties: polylogarithmic, or
not. They are used in two ways: as contributions to an
amplitude that is squared, or as contributions to an
observable matrix element. In the former case, products of
integrals occur, in the latter they do not. We report on
products of non-polylogarithmic Feynman integrals related to
the magnetic moment of the electron, giving details of an
infinite set of quadratic relations between these integrals
at all loops $L>2$.