14,215 research outputs found

    Semi-analytical approach for the Vaidya metric in double-null coordinates

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    We reexamine here a problem considered in detail before by Waugh and Lake: the solutions of spherically symmetric Einstein's equations with a radial flow of unpolarized radiation (the Vaidya metric) in double-null coordinates. This problem is known to be not analytically solvable, the only known explicit solutions correspond to the constant mass case (Schwarzschild solution in Kruskal-Szekeres form) and the linear and exponential mass functions originally discovered by Waugh and Lake. We present here a semi-analytical approach that can be used to discuss some qualitative and quantitative aspects of the Vaidya metric in double-null coordinates for generic mass functions. We present also a new analytical solution corresponding to (1/v)(1/v)-mass function.Comment: 5 pages, 6 figure

    A possible disk mechanism for the 23d QPO in Mkn~501

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    Optically thin two-temperature accretion flows may be thermally and viscously stable, but acoustically unstable. Here we propose that the O-mode instability of a cooling-dominated optically thin two-temperature inner disk may explain the 23-day quasi-periodic oscillation (QPO) period observed in the TeV and X-ray light curves of Mkn~501 during its 1997 high state. In our model the relativistic jet electrons Compton upscatter the disk soft X-ray photons to TeV energies, so that the instability-driven X-ray periodicity will lead to a corresponding quasi-periodicity in the TeV light curve and produce correlated variability. We analyse the dependence of the instability-driven quasi-periodicity on the mass (M) of the central black hole, the accretion rate (M˙\rm{\dot{M}}) and the viscous parameter (α\alpha) of the inner disk. We show that in the case of Mkn~501 the first two parameters are constrained by various observational results, so that for the instability occurring within a two-temperature disk where α=0.05−1.0\alpha=0.05-1.0, the quasi-period is expected to lie within the range of 8 to 100 days, as indeed the case. In particular, for the observed 23-day QPO period our model implies a viscosity coefficient α≤0.28\alpha \leq 0.28, a sub-Eddington accretion rate M˙≃0.02M˙Edd\dot{M} \simeq 0.02 \dot{M}_{\rm Edd} and a transition radius to the outer standard disk of r0∼60rgr_0 \sim 60 r_g, and predicts a period variation δP/P∼0.23\delta P/P \sim 0.23 due to the motion of the instability region.Comment: 18 pages, 1 figure, accepted by AP

    A Characterization of Discrete Time Soliton Equations

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    We propose a method to characterize discrete time evolution equations, which generalize discrete time soliton equations, including the qq-difference Painlev\'e IV equations discussed recently by Kajiwara, Noumi and Yamada.Comment: 13 page

    Magnetic properties of an SU(4) spin-orbital chain

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    In this paper, we study the magnetic properties of the one-dimensional SU(4) spin-orbital model by solving its Bethe ansatz solution numerically. It is found that the magnetic properties of the system for the case of gt=1.0g_t=1.0 differs from that for the case of gt=0.0g_t=0.0. The magnetization curve and susceptibility are obtained for a system of 200 sites. For 0<gt<gs0<g_t<g_s, the phase diagram depending on the magnetic field and the ratio of Land\'e factors, gt/gsg_t/g_s, is obtained. Four phases with distinct magnetic properties are found.Comment: 4 pages, 2 figure
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