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1.
We describe a new approach to the general theory of unitary representations of Lie groups which makes use of the Gelfand-Segal construction directly on the universal enveloping algebra of any Lie algebra. The crucial observation is that Nelson's theory of analytic vectors allows the characterisation of certain states on the universal enveloping algebra such that the corresponding representations of the universal enveloping algebra are the infinitesimal part of unitary representations of the associated simply connected Lie group. In the first section of the paper we show that with the aid of Choquet's theory of representing measures one can derive a simple new approach to integral decomposition theory along these lines.In the second section of the paper we use these methods to study the irreducible unitary representations of general semi-simple Lie groups. We give a simple proof that theK-finite vectors studied by Harish-Chandra [5] are all analytic vectors. We also give new proofs of some of Godement's results [2] characterising spherical functions of height one, at least for unitary representations. Compared with [2] our method has the possible advantage of obtaining the characterisations by infinitesimal methods instead of using an indirect argument involving functions on the group. We point out that while being purely algebraic in nature, this approach makes almost no use of the deep and difficult theorems of Harish-Chandra concerning the universal enveloping algebra [5].Our work is done in very much the same spirit as that of Power's recent paper [8]. The main difference is that by concentrating on a more special class of positive states we are able to carry the analysis very much further without difficulty.  相似文献   

2.
The irreducibility of a class of unitary representations of certain central extensions of current algebras in two dimensions, constructed in a previous paper, is announced. The techniques are extended and supplemented with new elements in order to construct representations of the central extension of Etingof and Frenkel. Irreducibility of the latter is announced.  相似文献   

3.
In this paper we investigate Leibniz algebras whose quotient Lie algebra is a naturally graded filiform Lie algebra nn,1. We introduce a Fock module for the algebra nn,1 and provide classification of Leibniz algebras L whose corresponding Lie algebra L/I is the algebra nn,1 with condition that the ideal I is a Fock nn,1-module, where I is the ideal generated by squares of elements from L.We also consider Leibniz algebras with corresponding Lie algebra nn,1 and such that the action I×nn,1I gives rise to a minimal faithful representation of nn,1. The classification up to isomorphism of such Leibniz algebras is given for the case of n=4.  相似文献   

4.
It is shown that every finitely generated continuous group has a subgroup generated by its infinitesimal transformations. This subgroup has a group algebra which is the Lie algebra of the group. By obtaining complete systems in the Lie algebra and complete rectangular arrays, it is shown that these can yield matrix representations of the continuous group. Illustrative examples are given for the rotation groups and for the full linear groups. It would seem that all the finite motion representations can be obtained by these methods, including spin representations of rotation groups. But the completeness of the method is not here demonstrated.  相似文献   

5.
For relative classical mechanics we construct a quasi-hamiltonian formalism associated to special representations of Lie algebras. This formalism is natural. For the case of the adjoint representation, this construction reduces to the usual absolute hamiltonian formalism on the dual spaces to Lie algebras.  相似文献   

6.
In paper [*] (P. Moylan: Czech. J. Phys., Vol. 47 (1997), p. 1251) we gave an explicit embedding of the three dimensional Euclidean algebra (2) into a quantum structure associated with U q(so(2, 1)). We used this embedding to construct skew symmetric representations of (2) out of skew symmetric representations of U q(so(2, 1)). Here we consider generalizations of the results in [*] to a more complicated quantum group, which is of importance to physics. We consider U q(so(3, 2)), and we show that, for a particular representation, namely the Rac representation, many of the results in [*] carry over to this case. In particular, we construct representations of so(3, 2), P(2, 2), the Poincaré algebra in 2+2 dimensions, and the Poincaré algebra out of the Rac representation of U q(so(3, 2)). These results may be of interest to those working on exploiting representations of U q(so(3, 2)), like the Rac, as an example of kinematical confinement for particle constituents such as the quarks.  相似文献   

7.
We give an integrability criterion for Lie algebra representations in a reflexive Banach space. Applications are given to skewsymmetric Lie algebra representations in Hilbert spaces and to essential skewadjointness of a sum of two skewadjoint operators.  相似文献   

8.
Let U be a unitary irreducible locally faithful representation of a nilpotent Lie group G, U the universal enveloping algebra of G, M a simple module on U with kernel Ker dU, then there exists an automorphism of U keeping ker dU invariant such that, after transport of structure, M is isomorphic to a submodule of the space of analytic vectors for U.  相似文献   

9.
We give a representation–theoretic interpretation of recent discovered coupled soliton equations using vertex operators construction of affinization of not simple but quadratic Lie algebras. In this setup we are able to obtain new integrable hierarchies coupled to each Drinfeld–Sokolov of A, B, C, D hierarchies and to construct their soliton solutions.  相似文献   

10.
It is discussed how boundedness of the quadratic Casimir operator in skew-symmetric representation τ of semisimple Lie algebra can simplify the proof of integrability of τ.  相似文献   

11.
Vertex representations are obtained for toroidal Lie algebras for any number of variables. These representations afford representations of certainn-variable generalizations of the Virasoro algebra that are abelian extensions of the Lie algebra of vector fields on a torus.Work supported in part by the Natural Sciences and Engineering Research Council of Canada.  相似文献   

12.
Letters in Mathematical Physics - In this paper, we study the asymptotics of multiplicities of irreducible representations in large tensor products of finite dimensional representations of simple...  相似文献   

13.
We characterize real Lie algebras carrying a hypersymplectic structure as bicrossproducts of two symplectic Lie algebras endowed with a compatible flat torsion-free connection. In particular, we obtain the classification of all hypersymplectic structures on 4-dimensional Lie algebras, and we describe the associated metrics on the corresponding Lie groups.  相似文献   

14.
《Nuclear Physics B》1999,561(3):413-432
We consider some unitary representations of infinite-dimensional Lie algebras motivated by string theory on AdS3. These include examples of two kinds: the A,D,E type affine Lie algebras and the N=4 superconformal algebra. The first presents a new construction for free field representations of affine Lie algebras. The second is of a particular physical interest because it provides some hints that a hybrid of the NSR and GS formulations for string theory on AdS3 exists.  相似文献   

15.
A procedure for taking the irreducible representations of subperiodic rod groups from tables of irreducible representations of three-periodical space groups is derived. Examples demonstrating the use of this procedure and derivation of selection rules for direct and phonon assisted electrical dipole transitions are presented. The text was submitted by the authors in English.  相似文献   

16.
17.
Sufficient conditions on unbounded, symmetric operatorsA andB which imply that $$\exp (itA)\exp (isB)\exp ( - itA)$$ satisfies the well known “multiple commutator” formula are derived. This formula is then applied to prove new necessary and sufficient conditions for the integrability of representations of Lie algebras and canonical commutation relations and the commutativity of the spectral projections of two commuting, unbounded, self-adjoint operators. A classic theorem of Nelson's is obtained as a corollary. Our results are useful in relativistic quantum field theory.  相似文献   

18.
Infinite-dimensional Lie algebras are introduced, which are only partially graded, and are specified by indices lying on cyclotomic rings. They may be thought of as generalizations of the Onsager algebra, but unlike it, or its sl(n) generalizations, they are not subalgebras of the loop algebras associated with sl(n). In a particular interesting case associated with sl(3), their indices lie on the Eisenstein integer triangular lattice, and these algebras are expected to underlie vertex operator combinations in CFT, brane physics, and graphite monolayers.  相似文献   

19.
A bicovariant calculus of differential operators on a quantum group is constructed in a natural way, using invariant maps from Fun toU q g, given by elements of the pure braid group. These operators—the reflection matrixYL + SL being a special case—generate algebras that linearly close under adjoint actions, i.e. they form generalized Lie algebras. We establish the connection between the Hopf algebra formulation of the calculus and a formulation in compact matrix form which is quite powerful for actual computations and as applications we find the quantum determinant and an orthogonality relation forY inSO q (N).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 PHY90-21139  相似文献   

20.
For each pair (G,K) where G is a complex finite-dimensional Lie algebra and K a semi-simple subalgebra of G, we construct an associative algebra (step algebra) Y (G,K) and a homomorphism i*: Y (G,K)→E(G) is the enveloping algebra of G. Y (G,K) has the following properties: (1) If V is any G-module and x ? V a K-maximal vector, then sx = i* (s)x is K-maximal for any s ? Y (G,K); (2) If V is irreducible and a certain simple criteria is fulfilled, then any K-maximal vector can be written in the form sxm, s ? Y (G,K), where xm is some fixed K-maximal vector. Because of these properties Y (G,K) has great practical value when constructing irreducible representations of Lie algebras in a form which makes the reduction with respect to a semi-simple subalgebra explicit.  相似文献   

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