2015
DOI: 10.1063/1.4928923
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Induced representations of tensors and spinors of any rank in the Stueckelberg-Horwitz-Piron theory

Abstract: We show that a modification of Wigner's induced representation for the description of a relativistic particle with spin can be used to construct spinors and tensors of arbitrary rank, with invariant decomposition over angular momentum. In particular, scalar and vector fields, as well as the representations of their transformations, are constructed. The method that is developed here admits the construction of wave packets and states of a many body relativistic system with definite total angular momentum. Furthe… Show more

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Cited by 4 publications
(4 citation statements)
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“…Since the transformation on the wave function (in ξ or π representation) is independent of π, the expectation value of x μ is covariant. In discussing the two body case later, we remark that this formulation may be applied to any spin (constructed with Clebsch-Gordan products in the spin space [25]).…”
Section: Quantum Theorymentioning
confidence: 99%
See 1 more Smart Citation
“…Since the transformation on the wave function (in ξ or π representation) is independent of π, the expectation value of x μ is covariant. In discussing the two body case later, we remark that this formulation may be applied to any spin (constructed with Clebsch-Gordan products in the spin space [25]).…”
Section: Quantum Theorymentioning
confidence: 99%
“…However, the spin representations we construct are entirely within the local infinitesimal algebra, sufficient to define spin as a local intrinsic structure of the particle (with generators satisfying the Pauli spin algebra). Constructing higher representations from direct product with Clebsch-Gordan coefficients (coordinate independent) can also be done in the same small neighborhood, as can the composition of spins of different particles [25], as we shall do in our discussion of entanglement.…”
Section: Spin Of a Particle In Shpgrmentioning
confidence: 99%
“…with L(n) the transformation bringing (1, 0, 0, 0) to n µ . Since the transformatiion on the wave function (in ξ or π representation) is indepedent of π, the expectation value of x µ is covariant.In discussing the two body case later, we remark that this formulation may be applied to any spin (constructed with Clebsch-Gordan products in the spin space [25]).…”
Section: Quantum Theorymentioning
confidence: 99%
“…However, the spin representations we construct are entirely within the local infinitesimal algebra, sufficient to define spin as a local intrinsic structure of the particle (with generators satisfyig the Pauli spin algebra). Constructing higher representations from direct product with Clebsch-Gordan coefficients (coordinate independent) can also be done in the same small neighborhood, as can the composition of spins of different particles [25], as we shall do in our discussion of entanglement.…”
Section: Spin Of a Particle In Shpgrmentioning
confidence: 99%