CHIRAL EQUATIONS AND FIBER-BUNDLES

被引:0
作者
MATOS, T
BECERRIL, R
机构
[1] INST POLITECN NACL,CTR INVEST & ESTUDIOS AVANZADOS,DEPT FIS,MEXICO CITY 07000,DF,MEXICO
[2] UNIV AUTONOMA METROPOLITANA AZCAPOTZALCO,FIS,MEXICO CITY 02200,DF,MEXICO
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中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
Using the hypothesis g = g(lambda(i)), the chiral equations(rho-g,(z)g-1),zBAR+(rho-g,zBARg-1),z = 0 are reduced to a Killing equation of a p-dimensional space V(p), being lambda(i) = lambda(i)(z,zBAR) "geodesic" parameters of V(p). Supposing that g belongs to a Lie group G, one writes the corresponding Lie algebra elements (F) in terms of the Killing vectors of V(p) and the generators of the subalgebra of F of dimension d = dimension of the Killing space. The elements of the subalgebras belong to equivalence classes which in the respective group form a principal fiber bundle. This is used to integrate the matrix g in terms of the complex variables z and zBAR.
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页码:69 / 80
页数:12
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共 14 条
[1]   KALUZA-KLEIN THEORIES [J].
BAILIN, D ;
LOVE, A .
REPORTS ON PROGRESS IN PHYSICS, 1987, 50 (09) :1087-&
[2]  
CHAU LL, GEOMETRICAL INTEGRAB
[3]  
CHOQUETBRUHAT, ANAL MANIFOLDS PHYSI, P168
[4]  
Diaz M. C., 1988, Revista Mexicana de Fisica, V34, P1
[5]  
ERNST FJ, 1968, PHYS REV, V167, P1175, DOI 10.1103/PhysRev.167.1175
[6]  
GILMORE R, 1974, LIE GORUPS LIE ALGEB, P213
[7]  
KRAMER D, EXACT SOLUTIONS EINS, P327
[8]  
MATOS T, 1989, ANN PHYS-LEIPZIG, V46, P462, DOI 10.1002/andp.19895010609
[9]  
Matos T., 1989, Revista Mexicana de Fisica, V35, P208
[10]   SL(3,R) REPRESENTATION FOR INVARIANCE-TRANSFORMATIONS IN 5-DIMENSIONAL GRAVITY [J].
MATOS, T .
PHYSICS LETTERS A, 1988, 131 (7-8) :423-426