14,162 research outputs found

    The Happer's puzzle degeneracies and Yangian

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    We find operators distinguishing the degenerate states for the Hamiltonian H=x(K+1/2)Sz+K⋅SH= x(K+{1/2})S_z +{\bf K}\cdot {\bf S} at x=±1x=\pm 1 that was given by Happer et al[1,2]^{[1,2]} to interpret the curious degeneracies of the Zeeman effect for condensed vapor of 87^{87}Rb. The operators obey Yangian commutation relations. We show that the curious degeneracies seem to verify the Yangian algebraic structure for quantum tensor space and are consistent with the representation theory of Y(sl(2))Y(sl(2)).Comment: 8 pages, Latex fil

    Thermoelectric DC conductivities with momentum dissipation from higher derivative gravity

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    We present a mechanism of momentum relaxation in higher derivative gravity by adding linear scalar fields to the Gauss-Bonnet theory. We analytically computed all of the DC thermoelectric conductivities in this theory by adopting the method given by Donos and Gauntlett in [arXiv:1406.4742]. The results show that the DC electric conductivity is not a monotonic function of the effective impurity parameter β\beta: in the small β\beta limit, the DC conductivity is dominated by the coherent phase, while for larger β\beta, pair creation contribution to the conductivity becomes dominant, signaling an incoherent phase. In addition, the DC heat conductivity is found independent of the Gauss-Bonnet coupling constant.Comment: 1+19 pages, 2 figures,typos in Eq.(40) correcte

    Anisotropic plasma with a chemical potential and scheme-independent instabilities

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    Generically, the black brane solution with planar horizons is thermodynamically stable. We find a counter-example to this statement by demonstrating that an anisotropic black brane is unstable. We present a charged black brane solution dual to a spatially anisotropic finite temperature N=4\mathcal{N}=4 super Yang-Mills plasma at finite U(1)U(1) chemical potential. This static and regular solution is obtained both numerically and analytically. We uncover rich thermodynamic phase structures for this system by considering the cases when the anisotropy constant "a" takes real and imaginary values, respectively. In the case a2>0a^2>0, the phase structure of this anisotropic black brane is similar to that of Schwarzschild-AdS black hole with S3S^3 horizon topology, yielding a thermodynamical instability at smaller horizon radii. For the condition a2≤0a^2\leq 0, the thermodynamics is dominated by the black brane phase for all temperatures.Comment: 14pages,14figures, minor changes, PLB in pres
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