{"title":"共形组中的自旋自由度引入本征动量算子","authors":"Seiichi Kuwata","doi":"10.21468/scipostphysproc.14.034","DOIUrl":null,"url":null,"abstract":"<jats:p>Considering spin degrees of freedom incorporated in the conformal generators, we introduce an intrinsic momentum operator <jats:inline-formula><jats:alternatives><jats:tex-math>\\pi_\\mu</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msub><mml:mi>π</mml:mi><mml:mi>μ</mml:mi></mml:msub></mml:math></jats:alternatives></jats:inline-formula>, which is feasible for the Bhabha wave equation. If a physical state <jats:inline-formula><jats:alternatives><jats:tex-math>\\psi_{ph}</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msub><mml:mi>ψ</mml:mi><mml:mrow><mml:mi>p</mml:mi><mml:mi>h</mml:mi></mml:mrow></mml:msub></mml:math></jats:alternatives></jats:inline-formula> for spin s is annihilated by the <jats:inline-formula><jats:alternatives><jats:tex-math>\\pi_\\mu</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msub><mml:mi>π</mml:mi><mml:mi>μ</mml:mi></mml:msub></mml:math></jats:alternatives></jats:inline-formula>, the degree of <jats:inline-formula><jats:alternatives><jats:tex-math>\\psi_{ph}</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msub><mml:mi>ψ</mml:mi><mml:mrow><mml:mi>p</mml:mi><mml:mi>h</mml:mi></mml:mrow></mml:msub></mml:math></jats:alternatives></jats:inline-formula>, deg <jats:inline-formula><jats:alternatives><jats:tex-math>\\psi_{ph}</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msub><mml:mi>ψ</mml:mi><mml:mrow><mml:mi>p</mml:mi><mml:mi>h</mml:mi></mml:mrow></mml:msub></mml:math></jats:alternatives></jats:inline-formula>, should equal twice the spin degrees of freedom, <jats:inline-formula><jats:alternatives><jats:tex-math>2 ( 2 s + 1)</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mn>2</mml:mn><mml:mrow><mml:mo stretchy=\"true\" form=\"prefix\">(</mml:mo><mml:mn>2</mml:mn><mml:mi>s</mml:mi><mml:mo>+</mml:mo><mml:mn>1</mml:mn><mml:mo stretchy=\"true\" form=\"postfix\">)</mml:mo></mml:mrow></mml:mrow></mml:math></jats:alternatives></jats:inline-formula> for a massive particle, where the multiplicity <jats:inline-formula><jats:alternatives><jats:tex-math>2</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mn>2</mml:mn></mml:math></jats:alternatives></jats:inline-formula> indicates the chirality. The relation deg <jats:inline-formula><jats:alternatives><jats:tex-math>\\psi_{ph}</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msub><mml:mi>ψ</mml:mi><mml:mrow><mml:mi>p</mml:mi><mml:mi>h</mml:mi></mml:mrow></mml:msub></mml:math></jats:alternatives></jats:inline-formula> = 2(2s+1) holds in the representation <jats:inline-formula><jats:alternatives><jats:tex-math>R_5</jats:tex-math><mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msub><mml:mi>R</mml:mi><mml:mn>5</mml:mn></mml:msub></mml:math></jats:alternatives></jats:inline-formula> (s,s), irreducible representation of the Lorentz group in five dimensions.</jats:p>","PeriodicalId":355998,"journal":{"name":"SciPost Physics Proceedings","volume":"2016 15-16","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2023-11-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Spin degrees of freedom incorporated in conformal group: Introduction of an intrinsic momentum operator\",\"authors\":\"Seiichi Kuwata\",\"doi\":\"10.21468/scipostphysproc.14.034\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<jats:p>Considering spin degrees of freedom incorporated in the conformal generators, we introduce an intrinsic momentum operator <jats:inline-formula><jats:alternatives><jats:tex-math>\\\\pi_\\\\mu</jats:tex-math><mml:math xmlns:mml=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><mml:msub><mml:mi>π</mml:mi><mml:mi>μ</mml:mi></mml:msub></mml:math></jats:alternatives></jats:inline-formula>, which is feasible for the Bhabha wave equation. If a physical state <jats:inline-formula><jats:alternatives><jats:tex-math>\\\\psi_{ph}</jats:tex-math><mml:math xmlns:mml=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><mml:msub><mml:mi>ψ</mml:mi><mml:mrow><mml:mi>p</mml:mi><mml:mi>h</mml:mi></mml:mrow></mml:msub></mml:math></jats:alternatives></jats:inline-formula> for spin s is annihilated by the <jats:inline-formula><jats:alternatives><jats:tex-math>\\\\pi_\\\\mu</jats:tex-math><mml:math xmlns:mml=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><mml:msub><mml:mi>π</mml:mi><mml:mi>μ</mml:mi></mml:msub></mml:math></jats:alternatives></jats:inline-formula>, the degree of <jats:inline-formula><jats:alternatives><jats:tex-math>\\\\psi_{ph}</jats:tex-math><mml:math xmlns:mml=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><mml:msub><mml:mi>ψ</mml:mi><mml:mrow><mml:mi>p</mml:mi><mml:mi>h</mml:mi></mml:mrow></mml:msub></mml:math></jats:alternatives></jats:inline-formula>, deg <jats:inline-formula><jats:alternatives><jats:tex-math>\\\\psi_{ph}</jats:tex-math><mml:math xmlns:mml=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><mml:msub><mml:mi>ψ</mml:mi><mml:mrow><mml:mi>p</mml:mi><mml:mi>h</mml:mi></mml:mrow></mml:msub></mml:math></jats:alternatives></jats:inline-formula>, should equal twice the spin degrees of freedom, <jats:inline-formula><jats:alternatives><jats:tex-math>2 ( 2 s + 1)</jats:tex-math><mml:math xmlns:mml=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><mml:mrow><mml:mn>2</mml:mn><mml:mrow><mml:mo stretchy=\\\"true\\\" form=\\\"prefix\\\">(</mml:mo><mml:mn>2</mml:mn><mml:mi>s</mml:mi><mml:mo>+</mml:mo><mml:mn>1</mml:mn><mml:mo stretchy=\\\"true\\\" form=\\\"postfix\\\">)</mml:mo></mml:mrow></mml:mrow></mml:math></jats:alternatives></jats:inline-formula> for a massive particle, where the multiplicity <jats:inline-formula><jats:alternatives><jats:tex-math>2</jats:tex-math><mml:math xmlns:mml=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><mml:mn>2</mml:mn></mml:math></jats:alternatives></jats:inline-formula> indicates the chirality. The relation deg <jats:inline-formula><jats:alternatives><jats:tex-math>\\\\psi_{ph}</jats:tex-math><mml:math xmlns:mml=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><mml:msub><mml:mi>ψ</mml:mi><mml:mrow><mml:mi>p</mml:mi><mml:mi>h</mml:mi></mml:mrow></mml:msub></mml:math></jats:alternatives></jats:inline-formula> = 2(2s+1) holds in the representation <jats:inline-formula><jats:alternatives><jats:tex-math>R_5</jats:tex-math><mml:math xmlns:mml=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><mml:msub><mml:mi>R</mml:mi><mml:mn>5</mml:mn></mml:msub></mml:math></jats:alternatives></jats:inline-formula> (s,s), irreducible representation of the Lorentz group in five dimensions.</jats:p>\",\"PeriodicalId\":355998,\"journal\":{\"name\":\"SciPost Physics Proceedings\",\"volume\":\"2016 15-16\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2023-11-24\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"SciPost Physics Proceedings\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.21468/scipostphysproc.14.034\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"SciPost Physics Proceedings","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.21468/scipostphysproc.14.034","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Spin degrees of freedom incorporated in conformal group: Introduction of an intrinsic momentum operator
Considering spin degrees of freedom incorporated in the conformal generators, we introduce an intrinsic momentum operator \pi_\muπμ, which is feasible for the Bhabha wave equation. If a physical state \psi_{ph}ψph for spin s is annihilated by the \pi_\muπμ, the degree of \psi_{ph}ψph, deg \psi_{ph}ψph, should equal twice the spin degrees of freedom, 2 ( 2 s + 1)2(2s+1) for a massive particle, where the multiplicity 22 indicates the chirality. The relation deg \psi_{ph}ψph = 2(2s+1) holds in the representation R_5R5 (s,s), irreducible representation of the Lorentz group in five dimensions.