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Rolling tachyon with electromagnetic field in linear dilaton background,” Phys (0)

by K Nagami
Venue:Lett. B591
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Note on D-brane effective action in the linear dilaton background

by J. Klusoň - JHEP 0311 (2003) 068 [arXiv:hep-th/0310066
"... Abstract: In this paper we will study tachyon effective action for Dp-brane in bosonic string theory in the linear dilaton background. We obtain the tachyon effective Lagrangian from boundary state coeficient of Dp-brane in the linear dilaton background and compare it with tachyon effective Lagrangi ..."
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Abstract: In this paper we will study tachyon effective action for Dp-brane in bosonic string theory in the linear dilaton background. We obtain the tachyon effective Lagrangian from boundary state coeficient of Dp-brane in the linear dilaton background and compare it with tachyon effective Lagrangians that were proposed in previous papers. Keywords: D-branes. Contents

Black Hole - String Transition and Rolling D-brane

by Yu Nakayama
"... We investigate the black hole- string transition in the two-dimensional Lorentzian black hole system from the exact boundary states that describe the rolling D-brane falling down into the two-dimensional black hole. The black hole- string phase transition is one of the fundamental properties of the ..."
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We investigate the black hole- string transition in the two-dimensional Lorentzian black hole system from the exact boundary states that describe the rolling D-brane falling down into the two-dimensional black hole. The black hole- string phase transition is one of the fundamental properties of the non-supersymmetric black holes in string theory, and we will reveal the nature of the phase transition from the exactly solvable world-sheet conformal field theory viewpoint. Since the two-dimensional Lorentzian black hole system (SL(2; R)k/U(1) coset model at level k) typically appears as near-horizon geometries of various singularities such as NS5-branes in string theory, our results can be regarded as the probe of such singularities from the nonsupersymmetric probe rolling D-brane. The exact construction of boundary states for the rolling D0-brane falling down into the two-dimensional D-brane enables us to probe the phase transition at k = 1 directly in the physical amplitudes. During the study, we uncover three fundamental questions in string theory as a consistent theory of quantum gravity: small charge limit v.s. large charge limit of non-supersymmetric quantum black holes, analyticity v.s. non-analyticity in physical amplitudes and physical observables, and unitarity v.s. open closed duality in time-dependent string backgrounds.

Remark about non-BPS Dp-brane at the tachyon vacuum moving in curved background,” arXiv:hep-th/0504062

by J. Klusoň
"... hep-th/0504062 ..."
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hep-th/0504062
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...brane decays, the classical solution of the system is characterised as a two component fluid system: One is preasurless electric flux lines, known as string fluid, while the other is a tachyon matter =-=[36, 37, 38, 40, 41]-=-. As we claimed above the string fluid and tachyon matter must have a natural interpretation via closed string states. In fact, it was shown that string fluid reproduces the classical behaviour of fun...

Applications of Thirring Model to Inhomogenous Rolling Tachyon and Dissipative Quantum Mechanics

by Taejin Lee , 2008
"... We study the rolling tachyon and the dissipative quantum mechanics using the Thirring model with a boundary mass. We construct a boundary state for the dissipative quantum system in one dimension, which describes the system at the off-critical points as well as at the critical point. Then we extend ..."
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We study the rolling tachyon and the dissipative quantum mechanics using the Thirring model with a boundary mass. We construct a boundary state for the dissipative quantum system in one dimension, which describes the system at the off-critical points as well as at the critical point. Then we extend the Thirring model with a boundary mass in order to depict the time evolution of an unstable D-branes with one direction wrapped on a circle of radius R, which is termed the inhomogeneous rolling tachyon. The analysis based on the Thirring model shows that the time dependent evolution of the inhomogeneous tachyon is possible only when 2 √ 3 < R < 2.
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...string with its ends on an unstable D-brane develops a marginal boundary interaction, the tachyon field of the open string condensates [16, 17, 18, 19, 20, 21]. This process, called “rolling tachyon” =-=[22, 23, 24, 25, 26, 27, 28, 29, 30, 31, 32, 33, 34, 35, 36, 37, 38, 39, 40, 41, 42, 43, 44, 45, 46, 47, 48, 49, 50, 51, 52, 53]-=-, is believed to be responsible for the decay of the unstable D-brane. Recently, the theory with a periodic boundary potential is discussed in detail by applying the fermionization technique [54, 55]....

hep-th/0607188 ZZ Brane Decay in D Dimensions

by Ya-li He A, Peng Zhang B , 2006
"... In this paper we consider the ZZ brane decay in a D-dimensional background with a linear dilaton and a Liouville potential switched on. We mainly calculate the closed string emission rate during the decay process. For the case of a spacelike dilaton we find a similar Hagedorn behavior, in the closed ..."
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In this paper we consider the ZZ brane decay in a D-dimensional background with a linear dilaton and a Liouville potential switched on. We mainly calculate the closed string emission rate during the decay process. For the case of a spacelike dilaton we find a similar Hagedorn behavior, in the closed string UV region, with the brane decay in the usual 26d and 2d bosonic string theory. This means that all of the energy of the original brane converts into outgoing closed strings. In the IR region the result is finite. We also String theory in time-dependent backgrounds is one of the most important questions that need to be understood. Dealing with general time-dependent backgrounds is still out of our abilities. Therefore simple solvable models, capturing some important aspects of the realistic physics, are laboratories for theoretical ideas and tools, which may give us some
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...to be treated exactly. There are many interesting related works. In [17] the author discusses the D-brane decay in the linear dilaton background from the viewpoint of the effective dynamics, see also =-=[18]-=- with electromagnetic field turned on. In [19] the author makes a deformation of 2d string theory with the X0 direction replaced by a timelike linear dilaton, and discuss its matrix model description....

Liouville Field Theory -- A decade after the revolution

by Yu Nakayama , 2004
"... We review recent developments (up to January 2004) of the Liouville field theory and its matrix model dual. This review consists of three parts. In the part I, we review the bosonic Liouville theory. After briefly reviewing the necessary background, we discuss the bulk structure constants (the DOZZ ..."
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We review recent developments (up to January 2004) of the Liouville field theory and its matrix model dual. This review consists of three parts. In the part I, we review the bosonic Liouville theory. After briefly reviewing the necessary background, we discuss the bulk structure constants (the DOZZ formula) and the boundary states (the FZZT brane and the ZZ brane). Various applications are also presented. In the part II, we review the supersymmetric extension of the Liouville theory. We first discuss the bulk structure constants and the branes as in the bosonic Liouville theory, and then we present the matrix dual descriptions with some applications. In the part III, the Liouville theory on unoriented surfaces is reviewed. After introducing the crosscap state, we discuss the matrix model dual description and the tadpole cancellation condition. This review also includes some original material such as the derivation of the conjectured dual action for the N = 2 Liouville theory from other known dualities and the comparison of the Liouville crosscap state with the c = 0 unoriented matrix model. This is
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... in [259], [260], [261], [206], [262], [207], [180], [263], [264], [265], [266], [267], [268], [269], [270], [271], [272], [273], [204], [274], [275], [276], [277], [278], [205], [279], [280], [281], =-=[282]-=-. Other topics which we have not covered in the main text include Bm,n 110• The time dependent two dimensional background from the matrix model point of view, [283], [284], [285], [286]. • The applic...

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