We represent the real hyperbolic space H" as the rank one homogeneous space Spin (1, n)/ Spin (n) and the spinor bundle S of H as the homogeneous bundle Spin (1, n) x (",V, where V, is the spinor representation space of Spin (n). The representation theoretic decomposition of L2(H, S) combined with t
โฆ LIBER โฆ
Chiral symmetry at finite T, the phase of the Polyakov loop and the spectrum of the Dirac operator
โ Scribed by M.A. Stephanov
- Publisher
- Elsevier Science
- Year
- 1996
- Tongue
- English
- Weight
- 544 KB
- Volume
- 375
- Category
- Article
- ISSN
- 0370-2693
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