4,854 research outputs found

    Pure geometric thick f(R)f(R)-branes: stability and localization of gravity

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    We study two exactly solvable five-dimensional thick brane world models in pure metric f(R)f(R) gravity. Working in the Einstein frame, we show that these solutions are stable against small linear perturbations, including the tensor, vector, and scalar modes. For both models, the corresponding gravitational zero mode is localized on the brane, which leads to the four-dimensional Newton's law; while the massive modes are nonlocalized and only contribute a small correction to the Newton's law at a large distance.Comment: 7 pages, 2 figures, improved version, accepted by Eur. Phys. J.

    U(1)U(1) gauge vector field on a codimension-2 brane

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    In this paper, we obtain a gauge invariant effective action for a bulk massless U(1)U(1) gauge vector field on a brane with codimension two by using a general Kaluza-Klein (KK) decomposition for the field. It suggests that there exist two types of scalar KK modes to keep the gauge invariance of the action for the massive vector KK modes. Both the vector and scalar KK modes can be massive. The masses of the vector KK modes m(n)m^{(n)} contain two parts, m1(n)m_{1}^{(n)} and m2(n)m_{2}^{(n)}, due to the existence of the two extra dimensions. The masses of the two types of scalar KK modes mϕ(n)m_{\phi}^{(n)} and mφ(n)m_{\varphi}^{(n)} are related to the vector ones, i.e., mϕ(n)=m1(n)m_{\phi}^{(n)}=m_{1}^{(n)} and mφ(n)=m2(n)m_{\varphi}^{(n)}=m_{2}^{(n)}. Moreover, we derive two Schr\"{o}dinger-like equations for the vector KK modes, for which the effective potentials are just the functions of the warp factor.Comment: 15 pages,no figures, accepted by JHE

    Entropy/Area spectra of the charged black hole from quasinormal modes

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    With the new physical interpretation of quasinormal modes proposed by Maggiore, the quantum area spectra of black holes have been investigated recently. Adopting the modified Hod's treatment, results show that the area spectra for black holes are equally spaced and the spacings are in a unified form, β–³A=8πℏ\triangle A=8\pi \hbar, in Einstein gravity. On the other hand, following Kunstatter's method, the studies show that the area spectrum for a nonrotating black hole with no charge is equidistant. And for a rotating (or charged) black hole, it is also equidistant and independent of the angular momentum JJ (or charge qq) when the black hole is far from the extremal case. In this paper, we mainly deal with the area spectrum of the stringy charged Garfinkle-Horowitz-Strominger black hole, originating from effective action that emerges in the low-energy string theory. We find that both methods give the same results-that the area spectrum is equally spaced and does not depend on the charge qq. Our study may provide new insights into understanding the area spectrum and entropy spectrum for stringy black holes.Comment: 13 pages, no figure
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