首页> 外文OA文献 >The consistent reduction of the differential calculus on the quantum group $GL_{q}(2,C)$ to the differential calculi on its subgroups and $\sigma$-models on the quantum group manifolds $SL_{q}(2,R)$, $SL_{q}(2,R)/U_{h}(1)$, $C{q}(2|0)$ and infinitesimal transformations
【2h】

The consistent reduction of the differential calculus on the quantum group $GL_{q}(2,C)$ to the differential calculi on its subgroups and $\sigma$-models on the quantum group manifolds $SL_{q}(2,R)$, $SL_{q}(2,R)/U_{h}(1)$, $C{q}(2|0)$ and infinitesimal transformations

机译:量子上微分计算的一致减少   将$ GL_ {q}(2,C)$分组到其子组和的子差分   $ \ sigma $ -models在量子群流上$ sL_ {q}(2,R)$,   $ sL_ {q}(2,R)/ U_ {h}(1)$,$ C {q}(2 | 0)$和无穷小变换

摘要

Explicit construction of the second order left differential calculi on thequantum group and its subgroups are obtained with the property of the naturalreduction: the differential calculus on the quantum group $GL_q(2,C)$ has tocontain the 3-dimensional differential calculi on the quantum subgroup$SL_q(2,C)$, the differential calculi on the Borel subgroups $B_{L}^{(2)}(C)$,$B_{U}^{(2)}(C)$ of the lower and of the upper triangular matrices, on thequantum subgroups $U_{q}(2)$, $SU_{q}(2)$, $Sp_{q}(2,C)$, $Sp_{q}(2)$,$T_{q}(2,C)$, $B_{L}(C)$, $B_{U}(C)$, $U_{q}(1)$, $Z_{-}^{(2)}(C)$,$Z_{+}^{(2)}(C)$ and on the their real forms. The classical limit ($q\to 1$) ofthe left differential calculus is the nondeformed differential calculus. Thedifferential calculi on the Borel subgroups $B_{L}(C)$, $B_{U}(C)$ of the$SL_{q}(2,C)$ coincide with two solutions of Wess-Zumino differential calculuson the quantum plane $C_q(2|0)$. The spontaneous breaking symmetry in the WZNW model with $SL_{q}(2,R)$quantum group symmetry over two-dimensional nondeformed Minkovski space and inthe $\sigma$-models with ${SL_{q}(2,R)/U_{p}(1)}$, $C_{q}(2|0)$ quantum groupsymmetry is considered. The Lagrangian formalism over the quantum groupmanifolds is discussed. The variational calculus on the $SL_{q}(2,R)$ groupmanifold is obtained. The classical solution of $C_{q}(2|0)$ {$\sigma$}-modelis obtained.
机译:利用自然归约的性质,获得了量子群及其子群上二阶左微分计算的明确构造:量子群$ GL_q(2,C)$上的微积分必须包含量子上的三维微分计算。子组$ SL_q(2,C)$,则Borel子组$ B_ {L} ^ {(2)}(C)$,$ B_ {U} ^ {(2)}(C)$的微分计算量子子组$ U_ {q}(2)$,$ SU_ {q}(2)$,$ Sp_ {q}(2,C)$,$ Sp_ {q}(2 )$,$ T_ {q}(2,C)$,$ B_ {L}(C)$,$ B_ {U}(C)$,$ U_ {q}(1)$,$ Z _ {-} ^ {(2)}(C)$,$ Z _ {+} ^ {(2)}(C)$及其真实形式。左微积分的经典极限($ q \到1 $)是非变形微积分。 $ SL_ {q}(2,C)$的Borel子组$ B_ {L}(C)$,$ B_ {U}(C)$的微分计算与量子上Wess-Zumino微积分的两个解一致平面$ C_q(2 | 0)$。在二维非变形Minkovski空间上具有$ SL_ {q}(2,R)$量子组对称的WZNW模型和具有$ {SL_ {q}(2,R)的$ \ sigma $模型中的自发破裂对称性考虑/ U_ {p}(1)} $,$ C_ {q}(2 | 0)$量子组对称性。讨论了量子群流形上的拉格朗日形式主义。获得在$ SL_ {q}(2,R)$子流形上的变分演算。获得了$ C_ {q}(2 | 0)$ {$ \ sigma $}-模型的经典解。

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  • 作者

    Gershun, V. D.;

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  • 年度 1997
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  • 原文格式 PDF
  • 正文语种 {"code":"en","name":"English","id":9}
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