10 research outputs found

    Maximally Symmetric Spin-Two Bitensors on S3S^3 and H3H^3

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    The transverse traceless spin-two tensor harmonics on S3S^3 and H3H^3 may be denoted by T(kl)abT^{(kl)}{}_{ab}. The index kk labels the (degenerate) eigenvalues of the Laplacian □\square and ll the other indices. We compute the bitensor ∑lT(kl)ab(x)T(kl)aâ€Čbâ€Č(xâ€Č)∗\sum_l T^{(kl)}{}_{ab}(x) T^{(kl)}{}_{a'b'}(x')^* where x,xâ€Čx,x' are distinct points on a sphere or hyperboloid of unit radius. These quantities may be used to find the correlation function of a stochastic background of gravitational waves in spatially open or closed Friedman-Robertson-Walker cosmologies.Comment: 12 pages, RevTeX, uuencoded compressed .tex file, minor typos correcte

    Field on Poincare group and quantum description of orientable objects

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    We propose an approach to the quantum-mechanical description of relativistic orientable objects. It generalizes Wigner's ideas concerning the treatment of nonrelativistic orientable objects (in particular, a nonrelativistic rotator) with the help of two reference frames (space-fixed and body-fixed). A technical realization of this generalization (for instance, in 3+1 dimensions) amounts to introducing wave functions that depend on elements of the Poincare group GG. A complete set of transformations that test the symmetries of an orientable object and of the embedding space belongs to the group Π=G×G\Pi =G\times G. All such transformations can be studied by considering a generalized regular representation of GG in the space of scalar functions on the group, f(x,z)f(x,z), that depend on the Minkowski space points x∈G/Spin(3,1)x\in G/Spin(3,1) as well as on the orientation variables given by the elements zz of a matrix Z∈Spin(3,1)Z\in Spin(3,1). In particular, the field f(x,z)f(x,z) is a generating function of usual spin-tensor multicomponent fields. In the theory under consideration, there are four different types of spinors, and an orientable object is characterized by ten quantum numbers. We study the corresponding relativistic wave equations and their symmetry properties.Comment: 46 page

    Representations of Lie Groups and Special Functions

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    An elementary approach to 6j-symbols (classical, quantum, rational, trigonometric, and elliptic)

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    Elliptic 6j-symbols first appeared in connection with solvable models of statistical mechanics. They include many interesting limit cases, such as quantum 6j-symbols (or q-Racah polynomials) and Wilson’s biorthogonal 10W9 functions. We give an elementary construction of elliptic 6j-symbols, which immediately implies several of their main properties. As a consequence, we obtain a new algebraic interpretation of elliptic 6j-symbols in terms of Sklyanin algebra representations
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