8,744 research outputs found

    Hydrodynamic Simulations of Oscillating Shock Waves in a Sub-Keplerian Accretion Flow Around Black Holes

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    We study the accretion processes on a black hole by numerical simulation. We use a grid based finite difference code for this purpose. We scan the parameter space spanned by the specific energy and the angular momentum and compare the time-dependent solutions with those obtained from theoretical considerations. We found several important results (a) The time dependent flow behaves close to a constant height model flow in the pre-shock region and a flow with vertical equilibrium in the post-shock region. (c) The infall time scale in the post-shock region is several times higher than the free-fall time scale. (b) There are two discontinuities in the flow, one being just outside of the inner sonic point. Turbulence plays a major role in determining the locations of these discontinuities. (d) The two discontinuities oscillate with two different frequencies and behave as a coupled harmonic oscillator. A Fourier analysis of the variation of the outer shock location indicates higher power at the lower frequency and lower power at the higher frequency. The opposite is true when the analysis of the inner shock is made. These behaviours will have implications in the spectral and timing properties of black hole candidates.Comment: 19 pages, 13 figures, 1 Table MNRAS (In press

    Satellite observations of thought experiments close to a black hole

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    Since black holes are `black', methods of their identification must necessarily be indirect. Due to very special boundary condition on the horizon, the advective flow behaves in a particular way, which includes formation of centrifugal pressure dominated boundary layer or CENBOL where much of the infall energy is released and outflows are generated. The observational aspects of black holes must depend on the steady and time-dependent properties of this boundary layer. Several observational results are written down in this review which seem to support the predictions of thought experiments based on this advective accretion/outflow model. In future, when gravitational waves are detected, some other predictions of this model could be tested as well.Comment: Published in Classical and Quantum Gravity, v. 17, No. 12, p. 2427, 200

    A nested sequence of projectors and corresponding braid matrices R^(θ)\hat R(\theta): (1) Odd dimensions

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    A basis of N2N^2 projectors, each an N2×N2{N^2}\times{N^2} matrix with constant elements, is implemented to construct a class of braid matrices R^(θ)\hat{R}(\theta), θ\theta being the spectral parameter. Only odd values of NN are considered here. Our ansatz for the projectors PαP_{\alpha} appearing in the spectral decomposition of R^(θ)\hat{R}(\theta) leads to exponentials exp(mαθ)exp(m_{\alpha}\theta) as the coefficient of PαP_{\alpha}. The sums and differences of such exponentials on the diagonal and the antidiagonal respectively provide the (2N21)(2N^2 -1) nonzero elements of R^(θ)\hat{R}(\theta). One element at the center is normalized to unity. A class of supplementary constraints imposed by the braid equation leaves 1/2(N+3)(N1){1/2}(N+3)(N-1) free parameters mαm_{\alpha}. The diagonalizer of R^(θ)\hat{R}(\theta) is presented for all NN. Transfer matrices t(θ)t(\theta) and L(θ)L(\theta) operators corresponding to our R^(θ)\hat{R}(\theta) are studied. Our diagonalizer signals specific combinations of the components of the operators that lead to a quadratic algebra of N2N^2 constant N×NN\times N matrices. The θ\theta-dependence factors out for such combinations. R^(θ)\hat R(\theta) is developed in a power series in θ\theta. The basic difference arising for even dimensions is made explicit. Some special features of our R^(θ)\hat{R}(\theta) are discussed in a concluding section.Comment: latex file, 32 page

    Generalized boson algebra and its entangled bipartite coherent states

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    Starting with a given generalized boson algebra U_(h(1)) known as the bosonized version of the quantum super-Hopf U_q[osp(1/2)] algebra, we employ the Hopf duality arguments to provide the dually conjugate function algebra Fun_(H(1)). Both the Hopf algebras being finitely generated, we produce a closed form expression of the universal T matrix that caps the duality and generalizes the familiar exponential map relating a Lie algebra with its corresponding group. Subsequently, using an inverse Mellin transform approach, the coherent states of single-node systems subject to the U_(h(1)) symmetry are found to be complete with a positive-definite integration measure. Nonclassical coalgebraic structure of the U_(h(1)) algebra is found to generate naturally entangled coherent states in bipartite composite systems.Comment: 15pages, no figur

    Fluctuation Cumulant Behavior for the Field-Pulse Induced Magnetisation-Reversal Transition in Ising Models

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    The universality class of the dynamic magnetisation-reversal transition, induced by a competing field pulse, in an Ising model on a square lattice, below its static ordering temperature, is studied here using Monte Carlo simulations. Fourth order cumulant of the order parameter distribution is studied for different system sizes around the phase boundary region. The crossing point of the cumulant (for different system sizes) gives the transition point and the value of the cumulant at the transition point indicates the universality class of the transition. The cumulant value at the crossing point for low temperature and pulse width range is observed to be significantly less than that for the static transition in the same two-dimensional Ising model. The finite size scaling behaviour in this range also indicates a higher correlation length exponent value. For higher temperature and pulse width range, the transition seems to fall in a mean-field like universality class.Comment: 5 pages, 8 eps figures, thoroughly revised manuscript with new figures, accepted in Phys. Rev. E (2003
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