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Pauli–Lubanski pseudovector : ウィキペディア英語版
Pauli–Lubanski pseudovector

In physics, specifically in relativistic quantum mechanics and quantum field theory, the Pauli–Lubanski pseudovector named after Wolfgang Pauli and Józef Lubański〔;
〕 is an operator defined from the momentum and angular momentum, used in the quantum-relativistic description of angular momentum.
It describes the spin states of moving particles.〔 pp 180-181.〕 It is the generator of the
little group of the Lorentz group, that is the maximal subgroup (with four generators) leaving the eigenvalues of the four-momentum vector invariant.
==Definition==

It is usually denoted by (or less often by ) and defined by:
~ \tfrac\varepsilon_ J^ P^\sigma ,
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where
:
*\varepsilon_ is the four-dimensional totally antisymmetric Levi-Civita symbol
:
*J^ is the relativistic angular momentum tensor operator
:
*P^ is the four-momentum.
In the language of exterior algebra, it can be written as the Hodge dual of a trivector,
:\mathbf = \star(\mathbf\wedge\mathbf).
evidently satisfies
:P^W_=0,
as well as the following commutator relations,
:\left()=0,
:\left()=-i \epsilon_ W^ P^.
The scalar is a Lorentz-invariant operator, and commutes with the four-momentum, and can thus serve as a label for irreducible representations of the Lorentz group. That is, it can serve as the label for the spin, a feature of the spacetime structure of the representation, over and above the relativistically invariant label for the mass of all states in a representation.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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