1,975 research outputs found

    Avatars of Margulis invariants and proper actions

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    In this article, we interpret affine Anosov representations of any word hyperbolic group in SO0(n−1,n)⋉R2n−1\mathsf{SO}_0(n-1,n)\ltimes\mathbb{R}^{2n-1} as infinitesimal versions of representations of word hyperbolic groups in SO0(n,n)\mathsf{SO}_0(n,n) which are both Anosov in SO0(n,n)\mathsf{SO}_0(n,n) with respect to the stabilizer of an oriented (n−1)(n-1)-dimensional isotropic plane and Anosov in SL(2n,R)\mathsf{SL}(2n,\mathbb{R}) with respect to the stabilizer of an oriented nn-dimensional plane. Moreover, we show that representations of word hyperbolic groups in SO0(n,n)\mathsf{SO}_0(n,n) which are Anosov in SO0(n,n)\mathsf{SO}_0(n,n) with respect to the stabilizer of an oriented (n−1)(n-1)-dimensional isotropic plane, are Anosov in SL(2n,R)\mathsf{SL}(2n,\mathbb{R}) with respect to the stabilizer of an oriented nn-dimensional plane if and only if its action on SO0(n,n)/SO0(n−1,n)\mathsf{SO}_0(n,n)/\mathsf{SO}_0(n-1,n) is proper. In the process, we also provide various different interpretations of the Margulis invariant.Comment: 40 page

    Analysis of ω\omega self-energy at finite temperature and density in the real-time formalism

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    Using the real time formalism of field theory at finite temperature and density we have evaluated the in-medium ω\omega self-energy from baryon and meson loops. We have analyzed in detail the discontinuities across the branch cuts of the self-energy function and obtained the imaginary part from the non-vanishing contributions in the cut regions. An extensive set of resonances have been considered in the baryon loops. Adding the meson loop contribution we obtain the full modified spectral function of ω\omega in a thermal gas of mesons, baryons and anti-baryons in equilibrium for several values of temperature and baryon chemical potential
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