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Related papers: D-Branes and Physical States

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We consider low energy, non-relativistic scattering of two Dirichlet zero-branes as an exercise in quantum mechanics. For weak string coupling and sufficiently small velocity, the dynamics is governed by an effective U(2) gauge theory in…

High Energy Physics - Theory · Physics 2008-11-26 Daniel Kabat , Philippe Pouliot

We use the boundary state formalism to study, from the closed string point of view, superpositions of branes and anti-branes which are relevant in some non-perturbative string dualities. Treating the tachyon instability of these systems as…

High Energy Physics - Theory · Physics 2010-11-26 M. Frau , L. Gallot , A. Lerda , P. Strigazzi

S(pacelike)D-branes are objects arising naturally in string theory when Dirichlet boundary conditions are imposed on the time direction. SD-brane physics is inherently time-dependent. Previous investigations of gravity fields of SD-branes…

High Energy Physics - Theory · Physics 2009-11-10 Frederic Leblond , Amanda W. Peet

All bound states of fundamental strings, D-branes and NS-branes of string theory, both type-IIA and type-IIB, which may be described by a null geodesic motion on the coset G/K(G) where G is a group of type A, D or E embedded within E(11)…

High Energy Physics - Theory · Physics 2015-05-30 Paul P. Cook

Using properties of the DBI action we find D-branes on $S^3$ of the radius $Q_5$ corresponding to the conjugacy classes of SU(2). The branes are stable due to nonzero 2-form NSNS background. In the limit of large $Q_5$ the dynamics of…

High Energy Physics - Theory · Physics 2009-10-31 Jacek Pawełczyk

In previous papers we built (multiple) D-branes in flat space-time as classical solutions of the string field theory based on the tachyon vacuum. In this paper we construct classical solutions describing all D-branes in any fixed space-time…

High Energy Physics - Theory · Physics 2009-11-07 Leonardo Rastelli , Ashoke Sen , Barton Zwiebach

We have studied a problem of the tachyon mediated D-brane - D-brane annihilation from the underlying world-volume gauge field theory point of view. The initial state was chosen in the form of two D-branes crossing at a non-zero angle, which…

High Energy Physics - Theory · Physics 2010-11-19 Anatoly Morosov

A method of determining the mass spectrum of BPS D-branes in any phase limit of a gauged linear sigma model is introduced. A ring associated to monodromy is defined and one considers K-theory to be a module over this ring. A simple but…

High Energy Physics - Theory · Physics 2014-11-20 Paul S. Aspinwall , M. Ronen Plesser

We consider the dynamics of a single probe brane on various cosmological brane backgrounds. The on-shell condition of the static probe brane leads to the supersymmetric intersection rules for static BPS configurations, though the…

High Energy Physics - Theory · Physics 2014-10-24 Kunihito Uzawa , Kentaroh Yoshida

We construct intersecting D-branes as noncommutative solitons in bosonic and type II string theory. ``Defect'' branes which are D-branes containing bubbles of the closed string vacuum play an important role in the construction.

High Energy Physics - Theory · Physics 2009-11-07 Li-Sheng Tseng

The physical states in a world-volume model of a non-critical 3-brane are systematically constructed using techniques of four-dimensional conformal field theories on R*S^3 developed recently. Invariant combinations of creation modes under a…

High Energy Physics - Theory · Physics 2009-11-10 Ken-ji Hamada

We obtain actions for N D-branes occupying points in a manifold with arbitrary Kahler metric. In one complex dimension, the action is uniquely determined (up to second order in commutators) by the requirement that it reproduce the masses of…

High Energy Physics - Theory · Physics 2008-02-03 Michael R. Douglas

We construct Spin(p+1,p+1) covariant Dp-brane bound states by using that the potentials in the RR sector of toroidically compactified type II supergravity transform as a chiral spinor of the T-duality group. As an application, we show the…

High Energy Physics - Theory · Physics 2009-10-31 Per Sundell

The entropy of a near-extremal black hole made of parallel D-branes has been shown to agree, upto a numerical factor, with that of the gas of massless open string states on the brane worldvolume when the string coupling is chosen suitably.…

High Energy Physics - Theory · Physics 2008-11-26 Sumit R. Das

We discuss how the BPS branes of M-theory could be described as bound states of non-BPS M10-branes. This conjectured M10-brane is constructed as an unstable spacetime-filling brane in the massive eleven dimensional supergravity defined with…

High Energy Physics - Theory · Physics 2009-10-31 Laurent Houart , Yolanda Lozano

In the process of identifying heterotic and Type $II$ BPS string states with extremal dilaton black holes, it has been suggested that solutions with scalar/Maxwell parameters $a=\sqrt{3}$, $1$, $1/\sqrt{3}$ and $0$ correspond to $1-$, $2-$,…

High Energy Physics - Theory · Physics 2015-06-26 M. J. Duff , J. Rahmfeld

A six dimensional braneworld scenario based on a model describing the interaction of gravity, gauge fields and 3+1 branes in a conformally invariant way is described. The action of the model is defined using a measure of integration built…

General Relativity and Quantum Cosmology · Physics 2015-06-25 E. I. Guendelman

A worldsheet approach to the study of non-abelian D-particle dynamics is presented based on viewing matrix-valued D-brane coordinate fields as coupling constants of a deformed sigma-model which defines a logarithmic conformal field theory.…

High Energy Physics - Theory · Physics 2007-05-23 Nick E. Mavromatos , Richard J. Szabo

We reformulate the lifting problem in the D1-D5 CFT as a supercharge cohomology problem, and enumerate BPS states according to the fortuitous/monotone classification. Working in the deformed $T^4$ symmetric orbifold theory, we give precise…

High Energy Physics - Theory · Physics 2026-02-24 Chi-Ming Chang , Ying-Hsuan Lin , Haoyu Zhang

Current universe (assumed here to be normal matter on the brane) is pressureless from observations. In this case the energy condition is $\rho_0\geq0$ and $p_0=0$. By using this condition, brane models can be distinguished. Then, assuming…

General Relativity and Quantum Cosmology · Physics 2008-12-18 Yongli Ping , Lixin Xu , Baorong Chang , Hongya Liu
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