arXiv:1810.02034·v3·High Energy Physics — Phenomenology
Spinor Representation of for
Teruyuki Kitabayashi🇯🇵 · Masaki Yasuè🇯🇵
Abstract
All possible permutations in the discrete group are classified by three rotation angles associated with the orthogonal group . We construct a spinor representation of , which is transformed by three 44 matrices corresponding to three Pauli matrices in . An irreducible decomposition of supplies a vector representation of {\bf 3} of , thereby, of . Our construction is consistent with the mathematical fact that . The parity in the spinorial space is described by a block off-diagonal matrix as the spinorial parity operator, whose eigenvalues are consistent with .
Comments: 11 pages