141 research outputs found

    K-essential Phantom Energy: Doomsday around the Corner? Revisited

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    We generalize some of those results reported by Gonz\'{a}lez-D\'{i}az by further tuning the parameter (β\beta) which is closely related to the canonical kinetic term in kk-essence formalism. The scale factor a(t)a(t) could be negative and decreasing within a specific range of β\beta (1/ω\equiv -1/\omega, ω\omega : the equation-of-state parameter) during the initial evolutional period.Comment: 1 Figure, 6 page

    Electronic population transfer via impulsive stimulated x-ray Raman scattering with attosecond soft-x-ray pulses

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    Artículo escrito por un elevado número de autores, solo se referencian el que aparece en primer lugar, el nombre del grupo de colaboración, si le hubiere, y los autores pertenecientes a la UA

    Regularity of maximal functions on Hardy–Sobolev spaces

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    We prove that maximal operators of convolution type associated to smooth kernels are bounded in the homogeneous Hardy–Sobolev spaces H1,p(Rd) when p > d/(d + 1). This range of exponents is sharp. As a by-product of the proof, we obtain similar results for the local Hardy–Sobolev spaces h1,p(Rd) in the same range of exponents

    A new view of k-essence

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    K-essence models, relying on scalar fields with non-canonical kinetic terms, have been proposed as an alternative to quintessence in explaining the observed acceleration of the Universe. We consider the use of field redefinitions to cast k-essence in a more familiar form. While k-essence models cannot in general be rewritten in the form of quintessence models, we show that in certain dynamical regimes an equivalence can be made, which in particular can shed light on the tracking behaviour of k-essence. In several cases, k-essence cannot be observationally distinguished from quintessence using the homogeneous evolution, though there may be small effects on the perturbation spectrum. We make a detailed analysis of two k-essence models from the literature and comment on the nature of the fine tuning arising in the models.Comment: 7 pages RevTeX4 file with four figures incorporate

    New holographic scalar field models of dark energy in non-flat universe

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    Motivated by the work of Granda and Oliveros [L.N. Granda, A. Oliveros, Phys. Lett. B {\bf 671}, 199 (2009)], we generalize their work to the non-flat case. We study the correspondence between the quintessence, tachyon, K-essence and dilaton scalar field models with the new holographic dark energy model in the non-flat FRW universe. We reconstruct the potentials and the dynamics for these scalar field models, which describe accelerated expansion of the universe. In the limiting case of a flat universe, i.e. k=0k = 0, all results given in [L.N. Granda, A. Oliveros, Phys. Lett. B {\bf 671}, 199 (2009)] are obtained.Comment: 11 page

    Interacting polytropic gas model of phantom dark energy in non-flat universe

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    By introducing the polytropic gas model of interacting dark energy, we obtain the equation of state for the polytropic gas energy density in a non-flat universe. We show that for even polytropic index by choosing K>Ba3nK>Ba^{\frac{3}{n}}, one can obtain ωΛeff<1\omega^{\rm eff}_{\Lambda}<-1, which corresponds to a universe dominated by phantom dark energy.Comment: 7 page

    Infrared cut-off proposal for the Holographic density

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    We propose an infrared cut-off for the holographic the dark-energy, which besides the square of the Hubble scale also contains the time derivative of the Hubble scale. This avoids the problem of causality which appears using the event horizon area as the cut-off, and solves the coincidence problem.Comment: 9 pages, 2 figures, to appear in Phys. Lett.

    K-essence and the coincidence problem

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    K-essence has been proposed as a possible means of explaining the coincidence problem of the Universe beginning to accelerate only at the present epoch. We carry out a comprehensive dynamical systems analysis of the k-essence models given so far in the literature. We numerically study the basin of attraction of the tracker solutions and we highlight the behaviour of the field close to sound speed divergences. We find that, when written in terms of parameters with a simple dynamical interpretation, the basins of attraction represent only a small region of the phase space.Comment: 5 pages RevTeX4 file with two figures incorporated. Minor changes to match PRD accepted versio
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