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1.
Cyclic representations of maximal dimension of the quantum algebra U
q
L associated with any finite-dimensional simple Lie algebra L are studied from its regular representation at q
p
=1, which is proved to be a quotient module of itself as a left module with respect to some submodules. The general theory is given after an instructive example U
q
sl(2) is studied. Another explicit example U
q
sl(3) is also presented.This work is supported in part by the National Natural Science Foundation of China. Author Fu is also supported by the Jilin Provincial Science and Technology Foundation of China 相似文献
2.
We characterize the finite-dimensional representations of the quantum affine algebra U
q
(
n+1) (whereq × is not a root of unity) which are irreducible as representations of U
q
(sl
n+1). We call such representations small. In 1986, Jimbo defined a family of homomorphismsev
a
from U
q
(sl
n+1) to (an enlargement of) U
q
(sl,n+1), depending on a parametera ·. A second family,ev
a
can be obtained by a small modification of Jimbo's formulas. We show that every small representation of U
q
(
n+1) is obtained by pulling back an irreducible representation of U
q
(sl
n+1) byev
a
orev
a
for somea ·. 相似文献
3.
We propose a general scheme of constructing braided differential algebras via algebras of “quantum exponentiated vector fields” and those of “quantum functions”. We treat a reflection equation algebra as a quantum analog of the algebra of vector fields. The role of a quantum function algebra is played by a general quantum matrix algebra. As an example we mention the so-called RTT algebra of quantized functions on the linear matrix group GL(m). In this case our construction essentially coincides with the quantum differential algebra introduced by S. Woronowicz. If the role of a quantum function algebra is played by another copy of the reflection equation algebra we get two different braided differential algebras. One of them is defined via a quantum analog of (co)adjoint vector fields, the other algebra is defined via a quantum analog of right-invariant vector fields. We show that the former algebra can be identified with a subalgebra of the latter one. Also, we show that “quantum adjoint vector fields” can be restricted to the so-called “braided orbits” which are counterparts of generic GL(m)-orbits in gl∗(m). Such braided orbits endowed with these restricted vector fields constitute a new class of braided differential algebras. 相似文献
4.
5.
Jouko Mickelsson 《Letters in Mathematical Physics》1993,28(2):97-106
It is proposed that instead of normal representations, one should look at cocycles of group extensions valued in certain groups of unitary operators acting in a Hilbert space (e.g. the Fock space of chiral fermions), when dealing with groups associated to current algebras in gauge theories in 3 + 1 spacetime dimensions. The appropriate cocycle is evaluated in the case of the group of smooth maps from the physical three-space to a compact Lie group.The cocyclic representation of a componentX of the current is obtained through two regularizations, (1) a conjugation by a background potential dependent unitary operatorh
A, (2) by a subtraction-h
A
-1
xhA, where
x
is a derivative along a gauge orbit. It is only the total operatorh
A
-1
Xh
A -h
A
-1
xhA which is quantizable in the Fock space using the usual normal ordering subtraction.Supported by the Alexander von Humboldt Foundation 相似文献
6.
To every finite-dimensional irreducible representation V of the quantum group U(g) where is a primitive lth root of unity (l odd) and g is a finite-dimensional complex simple Lie algebra, de Concini, Kac and Procesi have associated a conjugacy class C
V
in the adjoint group G of g. We describe explicitly, when g is of type A
n
, B
n
, C
n
, or D
n
, the representations associated to the conjugacy classes of minimal positive dimension. We call such representations fundamental and prove that, for any conjugacy class, there is an associated representation which is contained in a tensor product of fundamental representations. 相似文献
7.
The generators ofq-boson algebra are expressed in terms of those of boson algebra, and the relations among the representations of a quantum algebra onq-Fock space, on Fock space, and on coherent state space are discussed in a general way. Two examples are also given to present concrete physical spaces with quantum algebra symmetry. Finally, a new homomorphic mapping from a Lie algebra to boson algebra is presented.This work is supported by the National Foundation of Natural Science of China. 相似文献
8.
Let
be a finite-dimensional complex simple Lie algebra and Uq(
) the associated quantum group (q is a nonzero complex number which we assume is transcendental). IfV is a finitedimensional irreducible representation of Uq(
), an affinization ofV is an irreducible representationVV of the quantum affine algebra Uq(
) which containsV with multiplicity one and is such that all other irreducible Uq(
)-components ofV have highest weight strictly smaller than the highest weight ofV. There is a natural partial order on the set of Uq(
) classes of affinizations, and we look for the minimal one(s). In earlier papers, we showed that (i) if
is of typeA, B, C, F orG, the minimal affinization is unique up to Uq(
)-isomorphism; (ii) if
is of typeD orE and is not orthogonal to the triple node of the Dynkin diagram of
, there are either one or three minimal affinizations (depending on ). In this paper, we show, in contrast to the regular case, that if Uq(
) is of typeD
4 and is orthogonal to the triple node, the number of minimal affinizations has no upper bound independent of .As a by-product of our methods, we disprove a conjecture according to which, if
is of typeA
n,every affinization is isomorphic to a tensor product of representations of Uq(
) which are irreducible under Uq(
) (in an earlier paper, we proved this conjecture whenn=1).Both authors were partially supported by the NSF, DMS-9207701. 相似文献
9.
Borcherds algebras represent a new class of Lie algebras which have almost all the properties that ordinary Kac-Moody algebras have, but the only major difference is that these generalized Kac-Moody algebras are allowed to have imaginary simple roots. The simplest nontrivial examples one can think of are those where one adds by hand one imaginary simple root to an ordinary Kac-Moody algebra. We study the fundamental representation of this class of examples and prove that an irreducible module is given by the full tensor algebra over some integrable highest weight module of the underlying Kac-Moody algebra. We also comment on possible realizations of these Lie algebras in physics as symmetry algebras in quantum field theory.Supported by Konrad-Adenauer-Stiftung e.V.Supported by Deutsche Forschungsgemeinschaft. 相似文献
10.
Jun'Ichi Shiraishi Harunobu Kubo Hidetoshi Awata Satoru Odake 《Letters in Mathematical Physics》1996,38(1):33-51
A quantum deformation of the Virasoro algebra is defined. The Kac determinants at arbitrary levels are conjectured. We construct a bosonic realization of the quantum deformed Virasoro algebra. Singular vectors are expressed by the Macdonald symmetric functions. This is proved by constructing screening currents acting on the bosonic Fock space. 相似文献
11.
Casimir invariants for quantized affine Lie algebras are constructed and their eigenvalues computed in any irreducible highest-weight representation. 相似文献
12.
V. K. Dobrev 《Letters in Mathematical Physics》1991,22(4):251-266
We give explicit formulae for singular vectors of Verma modules over Uq(G), where G is any complex simple Lie algebra. The vectors we present correspond exhaustively to a class of positive roots of G which we call straight roots. In some special cases, we give singular vectors corresponding to arbitrary positive roots. For our vectors we use a special basis of Uq(G
-), where G
- is the negative roots subalgebra of G, which was introducted in our earlier work in the case q=1. This basis seems more economical than the Poincaré-Birkhoff-Witt type of basis used by Malikov, Feigin, and Fuchs for the construction of singular vectors of Verma modules in the case q=1. Furthermore, this basis turns out to be part of a general basis recently introduced for other reasons by Lusztig for Uq(-), where - is a Borel subalgebra of G.A. v. Humboldt-Stiftung fellow, permanent address and after 22 September 1991: Bulgarian Academy of Sciences, Institute of Nuclear Research and Nuclear Energy, 1784 Sofia, Bulgaria. 相似文献
13.
Using the previously obtained universalR-matrix for the quantized nontwisted affine Lie algebras U
q
(A
1
(1)
) and U
q
(A
2
(1)
), we determine the explicitly spectral dependent universalR-matrix for the corresponding quantum Lie algebras U
q
(A
1) and U
q
(A
2). As applications, we reproduce the well known results in the fundamental representations and we also derive an extremely explicit formula of the spectral-dependentR-matrix for the adjoint representation of U
q
(A
2), the simplest nontrivial case when the tensor product decomposition of the representation with itself has nontrivial multiplicity. 相似文献
14.
Let U
q
be a quantized affine Lie algebra. It is proven that the universal R-matrix R of U
q
satisfies the celebrated conjugation relationR
+ =TR withT the usual twist map. As applications, the braid generator is shown to be diagonalizable on arbitrary tensor product modules
of integrable irreducible highest weight U
q
-module and a spectral decomposition formula for the braid generator is obtained which is the generalization of Reshetikhin
and Gould forms to the present affine case. Casimir invariants are constructed and their eigenvalues computed by means of
the spectral decomposition formula. As a by-product, an interesting identity is found. 相似文献
15.
Peter Bryant 《Letters in Mathematical Physics》1990,19(2):97-108
Following the work of Krichever and Novikov, Bonora, Martellini, Rinaldi and Russo defined a superalgebra associated to each compact Riemann surface with spin structure. Noting that this data determines a graded Riemann surface, we find a natural interpretation of the BMRR-algebra in terms of the geometry of graded Riemann surfaces. We also discuss the central extensions of these algebras (correcting the form of the central extension given by Bonoraet al.). It is hoped that this work will be the first step towards defining Krichever-Novikov algebras for (the more general) super-Riemann surfaces; in particular we emphasise the importance ofgraded conformal vectorfields. 相似文献
16.
17.
Explicit formulas of the universalR-matrix are given for all quantized nontwisted rank 3 affine KM algebras U
q
(A
2
(1)
), U
q
(C
2
(1)
) and U
q
(G
2
(1)
). 相似文献
18.
19.
We show that the algebra of the bicovariant differential calculus on a quantum group can be understood as a projection of the cross-product between a braided Hopf algebra and the quantum double of the quantum group. The resulting super-Hopf algebra can be reproduced by extending the exterior derivative to tensor products.This work was supported in part by the Director, Office of Energy Research, Office of High Energy and Nuclear Physics, Division of High Energy Physics of the U.S. Department of Energy under Contract DE-AC03-76SF00098 and in part by the National Science Foundation under grant PHY-90-21139.Supported in part by a Feodor-Lynen Fellowship. 相似文献
20.
We present the eigenvalues of the Casimir invariants for the type I quantum superalgebras on any irreducible highest weight module. 相似文献