419 research outputs found

    Semi-regular masas of transfinite length

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    In 1965 Tauer produced a countably infinite family of semi-regular masas in the hyperfinite II1\mathrm{II}_1 factor, no pair of which are conjugate by an automorphism. This was achieved by iterating the process of passing to the algebra generated by the normalisers and, for each n∈Nn\in\mathbb N, finding masas for which this procedure terminates at the nn-th stage. Such masas are said to have length nn. In this paper we consider a transfinite version of this idea, giving rise to a notion of ordinal valued length. We show that all countable ordinals arise as lengths of semi-regular masas in the hyperfinite II1\mathrm{II}_1 factor. Furthermore, building on work of Jones and Popa, we obtain all possible combinations of regular inclusions of irreducible subfactors in the normalising tower.Comment: 14 page

    Algebraic methods in the theory of generalized Harish-Chandra modules

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    This paper is a review of results on generalized Harish-Chandra modules in the framework of cohomological induction. The main results, obtained during the last 10 years, concern the structure of the fundamental series of (g,k)−(\mathfrak{g},\mathfrak{k})-modules, where g\mathfrak{g} is a semisimple Lie algebra and k\mathfrak{k} is an arbitrary algebraic reductive in g\mathfrak{g} subalgebra. These results lead to a classification of simple (g,k)−(\mathfrak{g},\mathfrak{k})-modules of finite type with generic minimal k−\mathfrak{k}-types, which we state. We establish a new result about the Fernando-Kac subalgebra of a fundamental series module. In addition, we pay special attention to the case when k\mathfrak{k} is an eligible r−r-subalgebra (see the definition in section 4) in which we prove stronger versions of our main results. If k\mathfrak{k} is eligible, the fundamental series of (g,k)−(\mathfrak{g},\mathfrak{k})-modules yields a natural algebraic generalization of Harish-Chandra's discrete series modules.Comment: Keywords : generalized Harish-Chandra module, (g,k)-module of finite type, minimal k-type, Fernando-Kac subalgebra, eligible subalgebra; Pages no. : 13; Bibliography : 21 item

    Completely positive maps on modules, instruments, extremality problems, and applications to physics

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    Convex sets of completely positive maps and positive semidefinite kernels are considered in the most general context of modules over C∗C^*-algebras and a complete charaterization of their extreme points is obtained. As a byproduct, we determine extreme quantum instruments, preparations, channels, and extreme autocorrelation functions. Various applications to quantum information and measurement theories are given. The structure of quantum instruments is analyzed thoroughly.Comment: 32 page

    Orthogonal polynomials of discrete variable and Lie algebras of complex size matrices

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    We give a uniform interpretation of the classical continuous Chebyshev's and Hahn's orthogonal polynomials of discrete variable in terms of Feigin's Lie algebra gl(N), where N is any complex number. One can similarly interpret Chebyshev's and Hahn's q-polynomials and introduce orthogonal polynomials corresponding to Lie superlagebras. We also describe the real forms of gl(N), quasi-finite modules over gl(N), and conditions for unitarity of the quasi-finite modules. Analogs of tensors over gl(N) are also introduced.Comment: 25 pages, LaTe

    Superanalogs of the Calogero operators and Jack polynomials

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    A depending on a complex parameter kk superanalog SL{\mathcal S}{\mathcal L} of Calogero operator is constructed; it is related with the root system of the Lie superalgebra gl(n∣m){\mathfrak{gl}}(n|m). For m=0m=0 we obtain the usual Calogero operator; for m=1m=1 we obtain, up to a change of indeterminates and parameter kk the operator constructed by Veselov, Chalykh and Feigin [2,3]. For k=1,12k=1, \frac12 the operator SL{\mathcal S}{\mathcal L} is the radial part of the 2nd order Laplace operator for the symmetric superspaces corresponding to pairs (GL(V)×GL(V),GL(V))(GL(V)\times GL(V), GL(V)) and (GL(V),OSp(V))(GL(V), OSp(V)), respectively. We will show that for the generic mm and nn the superanalogs of the Jack polynomials constructed by Kerov, Okunkov and Olshanskii [5] are eigenfunctions of SL{\mathcal S}{\mathcal L}; for k=1,12k=1, \frac12 they coinside with the spherical functions corresponding to the above mentioned symmetric superspaces. We also study the inner product induced by Berezin's integral on these superspaces

    Extreme Covariant Quantum Observables in the Case of an Abelian Symmetry Group and a Transitive Value Space

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    We represent quantum observables as POVMs (normalized positive operator valued measures) and consider convex sets of observables which are covariant with respect to a unitary representation of a locally compact Abelian symmetry group GG. The value space of such observables is a transitive GG-space. We characterize the extreme points of covariant observables and also determine the covariant extreme points of the larger set of all quantum observables. The results are applied to position, position difference and time observables.Comment: 23 page

    Locally Trivial W*-Bundles

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    We prove that a tracially continuous W∗^*-bundle M\mathcal{M} over a compact Hausdorff space XX with all fibres isomorphic to the hyperfinite II1_1-factor R\mathcal{R} that is locally trivial already has to be globally trivial. The proof uses the contractibility of the automorphism group Aut(R)\mathrm{Aut}({\mathcal{R}}) shown by Popa and Takesaki. There is no restriction on the covering dimension of XX.Comment: 20 pages, this version will be published in the International Journal of Mathematic

    "Massless" vector field in de Sitter Universe

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    In the present work the massless vector field in the de Sitter (dS) space has been quantized. "Massless" is used here by reference to conformal invariance and propagation on the dS light-cone whereas "massive" refers to those dS fields which contract at zero curvature unambiguously to massive fields in Minkowski space. Due to the gauge invariance of the massless vector field, its covariant quantization requires an indecomposable representation of the de Sitter group and an indefinite metric quantization. We will work with a specific gauge fixing which leads to the simplest one among all possible related Gupta-Bleuler structures. The field operator will be defined with the help of coordinate independent de Sitter waves (the modes) which are simple to manipulate and most adapted to group theoretical matters. The physical states characterized by the divergencelessness condition will for instance be easy to identify. The whole construction is based on analyticity requirements in the complexified pseudo-Riemanian manifold for the modes and the two-point function.Comment: 33 pages, 3 figure

    Non-commutative fermion mass matrix and gravity

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    The first part is an introductory description of a small cross-section of the literature on algebraic methods in non-perturbative quantum gravity with a specific focus on viewing algebra as a laboratory in which to deepen understanding of the nature of geometry. This helps to set the context for the second part, in which we describe a new algebraic characterisation of the Dirac operator in non-commutative geometry and then use it in a calculation on the form of the fermion mass matrix. Assimilating and building on the various ideas described in the first part, the final part consists of an outline of a speculative perspective on (non-commutative) quantum spectral gravity. This is the second of a pair of papers so far on this project.Comment: To appear in Int. J. Mod. Phys. A Previous title: An outlook on quantum gravity from an algebraic perspective. 39 pages, 1 xy-pic figure, LaTex Reasons for new version: added references, change of title and some comments more up-to-dat

    Localizations at infinity and essential spectrum of quantum Hamiltonians: I. General theory

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    We isolate a large class of self-adjoint operators H whose essential spectrum is determined by their behavior at large x and we give a canonical representation of their essential spectrum in terms of spectra of limits at infinity of translations of H. The configuration space is an arbitrary abelian locally compact not compact group.Comment: 63 pages. This is the published version with several correction
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