A new method of generating the high-temperature molecule PN is described. Previous results for the decomposition of PN into Pz and N2 as well as for the formation and properties of (PN) 3 are confirmed. The reaction energy ER for the reaction fPz+ iN,\*PN is determined from extended CPF calculations
Decomposition Numbers of SL3(pn) and SU3(pn)
β Scribed by Leonard Chastkofsky
- Publisher
- Elsevier Science
- Year
- 2001
- Tongue
- English
- Weight
- 156 KB
- Volume
- 240
- Category
- Article
- ISSN
- 0021-8693
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β¦ Synopsis
We review the results obtained in 1 , as applied to SL p and 3
Ε½ n . Let β« be either the group SL p or SU p . Let X be the weight n 3 3 lattice for β« . It is isomorphic to β«ήβ¬ q = β«ήβ¬ q . Let X n be the subset of n p p n -restricted weights, consisting of those elements of X whose coordinates in terms of the fundamental dominant weights lie between 0 and p n y 1.
The projective indecomposable characters are indexed by weights in X n . Let β½ be the projective indecomposable character indexed by .
p , n
Let W be the Weyl group. Let W be the affine Weyl group, that is, a, p the semidirect product of W with translations by elements of p times the
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