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
On the numerical solution of hyperbolic PDEs with variable space operator
β Scribed by Allaberen Ashyralyev; Mehmet Emir Koksal
- Publisher
- John Wiley and Sons
- Year
- 2009
- Tongue
- English
- Weight
- 204 KB
- Volume
- 25
- Category
- Article
- ISSN
- 0749-159X
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