共形组中的自旋自由度引入本征动量算子

Seiichi Kuwata
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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. 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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. 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引用次数: 0

摘要

考虑到共形发生器中包含的自旋自由度,我们引入了一个本征动量算子 \pi_\muπμ,它对巴巴波方程是可行的。如果自旋为 s 的物理态 \psi_{ph}ψph 被 \pi_\muπμ 湮灭,\psi_{ph}ψph 的度 deg \psi_{ph}ψph 应该等于自旋自由度的两倍,对于大质量粒子为 2 ( 2 s + 1)2(2s+1) ,其中倍数 22 表示手性。deg \psi_{ph}ψph = 2(2s+1)关系在五维洛伦兹群的不可还原表示 R_5R5 (s,s)中成立。
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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.
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