11 research outputs found

    Jordan-Schwinger map, 3D harmonic oscillator constants of motion, and classical and quantum parameters characterizing electromagnetic wave polarization

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    In this work we introduce a generalization of the Jauch and Rohrlich quantum Stokes operators when the arrival direction from the source is unknown {\it a priori}. We define the generalized Stokes operators as the Jordan-Schwinger map of a triplet of harmonic oscillators with the Gell-Mann and Ne'eman SU(3) symmetry group matrices. We show that the elements of the Jordan-Schwinger map are the constants of motion of the three-dimensional isotropic harmonic oscillator. Also, we show that generalized Stokes Operators together with the Gell-Mann and Ne'eman matrices may be used to expand the polarization density matrix. By taking the expectation value of the Stokes operators in a three-mode coherent state of the electromagnetic field, we obtain the corresponding generalized classical Stokes parameters. Finally, by means of the constants of motion of the classical three-dimensional isotropic harmonic oscillator we describe the geometric properties of the polarization ellips

    A survey of the homotopy properties of inclusion of certain types of configuration spaces into the Cartesian product

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    International audienceLet XX be a topological space. In this survey we consider several types of configuration spaces, namely the classical (usual) configuration spaces Fn(X)F_n(X) and Dn(X)D_n(X), the orbit configuration spaces FnG(X)F_n^G(X) and FnG(X)/SnF_n^G(X)/S_n with respect to a free action of a group GG on XX, and the graph configuration spaces FnΓ(X)F_n^{\Gamma}(X) and FnΓ(X)/HF_n^{\Gamma}(X)/H, where Γ\Gamma is a graph and HH is a suitable subgroup of the symmetric group SnS_n. The ordered configuration spaces Fn(X)F_n(X), FnG(X)F_n^G(X), FnΓ(X)F_n^{\Gamma}(X) are all subsets of the nn-fold Cartesian product 1nX\prod_1^n\, X of XX with itself, and satisfy FnG(X)Fn(X)FnΓ(X)1nXF_n^G(X)\subset F_n(X) \subset F_n^{\Gamma}(X)\subset \prod_1^n\, X. If AA denotes one of these configuration spaces, we analyse the difference between AA and 1nX\prod_1^n\, X from a topological and homotopical point of view. The principal results known in the literature concern the usual configuration spaces. We are particularly interested in the homomorphism on the level of the homotopy groups of the spaces induced by the inclusion ι ⁣:A1nX\iota \colon\thinspace A \longrightarrow \prod_1^n\, X, the homotopy type of the homotopy fibre IιI_{\iota} of the map ι\iota via certain constructions on various spaces that depend on XX, and the long exact sequence in homotopy of the fibration involving IιI_{\iota} and arising from the inclusion ι\iota. In this respect, if XX is either a surface without boundary, in particular if XX is the 22-sphere or the real projective plane, or a space whose universal covering is contractible, or an orbit space Sk/G\mathbb{S}^k/G of the kk-dimensional sphere by a free action of a Lie Group GG, we present some recent results obtained in [23,24] for the first case, and in [18] for the second and third cases. We briefly indicate some older results relative to the homotopy of these spaces that are related to the problems of interest. In order to motivate various questions, for the remaining types of configuration spaces, we describe and prove a few of their basic properties. We finish the paper with a list of open questions and problems
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