7,205 research outputs found

    A perturbative analysis of tachyon condensation

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    Tachyon condensation in the open bosonic string is analyzed using a perturbative expansion of the tachyon potential around the unstable D25-brane vacuum. Using the leading terms in the tachyon potential, Pad\'e approximants can apparently give the energy of the stable vacuum to arbitrarily good accuracy. Level-truncation approximations up to level 10 for the coefficients in the tachyon potential are extrapolated to higher levels and used to find approximants for the full potential. At level 14 and above, the resulting approximants give an energy less than -1 in units of the D25-brane tension, in agreement with recent level-truncation results by Gaiotto and Rastelli. The extrapolated energy continues to decrease below -1 until reaching a minimum near level 26, after which the energy turns around and begins to approach -1 from below. Within the accuracy of this method, these results are completely consistent with an energy which approaches -1 as the level of truncation is taken to be arbitrarily large.Comment: 8 pages, 3 eps figures, Latex; v2: typo correcte

    Planck Fluctuations, Measurement Uncertainties and the Holographic Principle

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    Starting from a critical analysis of recently reported surprisingly large uncertainties in length and position measurements deduced within the framework of quantum gravity, we embark on an investigation both of the correlation structure of Planck scale fluctuations and the role the holographic hypothesis is possibly playing in this context. While we prove the logical independence of the fluctuation results and the holographic hypothesis (in contrast to some recent statements in that direction) we show that by combining these two topics one can draw quite strong and interesting conclusions about the fluctuation structure and the microscopic dynamics on the Planck scale. We further argue that these findings point to a possibly new and generalized form of quantum statistical mechanics of strongly (anti)correlated systems of degrees of freedom in this fundamental regime.Comment: 19 pages, Latex, no figures, some new references, to appear ModPhysLett

    Energy Momentum Tensor and Marginal Deformations in Open String Field Theory

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    Marginal boundary deformations in a two dimensional conformal field theory correspond to a family of classical solutions of the equations of motion of open string field theory. In this paper we develop a systematic method for relating the parameter labelling the marginal boundary deformation in the conformal field theory to the parameter labelling the classical solution in open string field theory. This is done by first constructing the energy-momentum tensor associated with the classical solution in open string field theory using Noether method, and then comparing this to the answer obtained in the conformal field theory by analysing the boundary state. We also use this method to demonstrate that in open string field theory the tachyon lump solution on a circle of radius larger than one has vanishing pressure along the circle direction, as is expected for a codimension one D-brane.Comment: LaTeX file, 25 pages; v2: minor addition

    The Evolution of Universe with th B-I Type Phantom Scalar Field

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    We considered the phantom cosmology with a lagrangian L=1η[1−1+ηgΌΜϕ,Όϕ,Îœ]−u(ϕ)\displaystyle L=\frac{1}{\eta}[1-\sqrt{1+\eta g^{\mu\nu}\phi_{, \mu}\phi_{, \nu}}]-u(\phi), which is original from the nonlinear Born-Infeld type scalar field with the lagrangian L=1η[1−1−ηgΌΜϕ,Όϕ,Îœ]−u(ϕ)\displaystyle L=\frac{1}{\eta}[1-\sqrt{1-\eta g^{\mu\nu}\phi_{, \mu}\phi_{, \nu}}]-u(\phi). This cosmological model can explain the accelerated expansion of the universe with the equation of state parameter w≀−1w\leq-1. We get a sufficient condition for a arbitrary potential to admit a late time attractor solution: the value of potential u(Xc)u(X_c) at the critical point (Xc,0)(X_c,0) should be maximum and large than zero. We study a specific potential with the form of u(ϕ)=V0(1+ϕϕ0)e(−ϕϕ0)u(\phi)=V_0(1+\frac{\phi}{\phi_0})e^{(-\frac{\phi}{\phi_0})} via phase plane analysis and compute the cosmological evolution by numerical analysis in detail. The result shows that the phantom field survive till today (to account for the observed late time accelerated expansion) without interfering with the nucleosynthesis of the standard model(the density parameter Ωϕ≃10−12\Omega_{\phi}\simeq10^{-12} at the equipartition epoch), and also avoid the future collapse of the universe.Comment: 17 pages, 10 figures,typos corrected, references added,figures added and enriched, title changed, main result remaine

    Deformed two center shell model

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    A highly specialized two-center shell model has been developed accounting for the splitting of a deformed parent nucleus into two ellipsoidaly deformed fragments. The potential is based on deformed oscillator wells in direct correspondance with the shape change of the nuclear system. For the first time a potential responsible for the necking part between the fragments is introduced on potential theory basis. As a direct consequence, spin-orbit {\bf ls} and {\bf l2^2} operators are calculated as shape dependent. Level scheme evolution along the fission path for pairs of ellipsoidaly deformed fragments is calculated. The Strutinsky method yields the shell corrections for different mass asymmetries from the superheavy nucleus 306^{306}122 and 252^{252}Cf all along the splitting process.Comment: 32 pages, 8 figure

    D0-brane tension in string field theory

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    We compute the D0-brane tension in string field theory by representing it as a tachyon lump of the D1-brane compactified on a circle of radius RR. To this aim, we calculate the lump solution in level truncation up to level L=8. The normalized D0-brane tension is independent on RR. The compactification radius is therefore chosen in order to cancel the subleading correction 1/L21/L^2. We show that an optimal radius R∗R^* indeed exists and that at R∗R^* the theoretical prediction for the tension is reproduced at the level of 10−510^{-5}. As a byproduct of our calculation we also discuss the determination of the marginal tachyon field at R→1R\to 1.Comment: 13 pages, 3 Eps figure
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