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Электронный каталог: Golubtsova, A. A. - Continuous Spin Field in the AdS&sub(6) Space
Golubtsova, A. A. - Continuous Spin Field in the AdS&sub(6) Space
Статья
Автор: Golubtsova, A. A.
Nuclear Physics B: Continuous Spin Field in the AdS&sub(6) Space
б.г.
ISBN отсутствует
Автор: Golubtsova, A. A.
Nuclear Physics B: Continuous Spin Field in the AdS&sub(6) Space
б.г.
ISBN отсутствует
На полку
Статья
Golubtsova, A.A.
Continuous Spin Field in the AdS&sub(6) Space / A.A.Golubtsova, M.A.Podoinitsyn. – Text : electronic // Nuclear Physics B. – 2026. – Vol. 1027. – P. 117462. – URL: https://doi.org/10.1016/j.nuclphysb.2026.117462. – Bibliogr.: 78.
A representation of the so(2, 5) algebra corresponding to the continuous spin field in AdS&sub(6) is considered. The algebra is realized using the Lie-Lorentz derivative, which naturally incorporates AdS&sub(6) geometry and spin degrees of freedom. Within this framework, we derive explicit expressions for the Casimir operators in terms of both the covariant derivative and spin invariants. The continuous spin representation under consideration is defined by a system of operator constraints that generalize those known for six-dimensional Minkowski space. We demonstrate that these constraints completely fix all Casimir operators of the so(2, 5) algebra with eigenvalues determined by the dimensional real parameter *m and the positive (half-)integer s.
Спец.(статьи,препринты) = С 323.5в - Спиновые эффекты при высоких энергиях
ОИЯИ = ОИЯИ (JINR)2026
Golubtsova, A.A.
Continuous Spin Field in the AdS&sub(6) Space / A.A.Golubtsova, M.A.Podoinitsyn. – Text : electronic // Nuclear Physics B. – 2026. – Vol. 1027. – P. 117462. – URL: https://doi.org/10.1016/j.nuclphysb.2026.117462. – Bibliogr.: 78.
A representation of the so(2, 5) algebra corresponding to the continuous spin field in AdS&sub(6) is considered. The algebra is realized using the Lie-Lorentz derivative, which naturally incorporates AdS&sub(6) geometry and spin degrees of freedom. Within this framework, we derive explicit expressions for the Casimir operators in terms of both the covariant derivative and spin invariants. The continuous spin representation under consideration is defined by a system of operator constraints that generalize those known for six-dimensional Minkowski space. We demonstrate that these constraints completely fix all Casimir operators of the so(2, 5) algebra with eigenvalues determined by the dimensional real parameter *m and the positive (half-)integer s.
Спец.(статьи,препринты) = С 323.5в - Спиновые эффекты при высоких энергиях
ОИЯИ = ОИЯИ (JINR)2026
