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Related papers: NS Fivebrane and Tachyon Condensation

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In this note we investigate certain topological aspects of the effective action of the NS5-brane in type IIA string theory. To facilitate the study of the corresponding partition function, we define a cohomology class whose vanishing is a…

High Energy Physics - Theory · Physics 2014-11-04 Hisham Sati

We show that all supersymmetric Type IIA D-branes can be constructed as bound states of a certain number of unstable non-supersymmetric Type IIA D9-branes. This string-theoretical construction demonstrates that D-brane charges in Type IIA…

High Energy Physics - Theory · Physics 2008-11-26 Petr Horava

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

We consider the type 0 theories, obtained from the closed NSR string by a diagonal GSO projection which excludes space-time fermions, and study the D-branes into these theories. The low-energy dynamics of N coincident D-branes is governed…

High Energy Physics - Theory · Physics 2009-09-17 I. R. Klebanov , A. A. Tseytlin

We introduce brane brick models, a novel type of Type IIA brane configurations consisting of D4-branes ending on an NS5-brane. Brane brick models are T-dual to D1-branes over singular toric Calabi-Yau 4-folds. They fully encode the infinite…

High Energy Physics - Theory · Physics 2016-02-16 Sebastian Franco , Sangmin Lee , Rak-Kyeong Seong

We derive the Nahm construction of monopoles from exact tachyon condensation on unstable D-branes. The Dirac operator used in the Nahm construction is identified with the tachyon profile in our D-brane approach, and we provide physical…

High Energy Physics - Theory · Physics 2009-11-11 Koji Hashimoto , Seiji Terashima

It has been conjectured that at the stationary point of the tachyon potential for the non-BPS D-brane or brane-anti-D-brane pair, the negative energy density cancels the brane tension. We study this conjecture using a cubic superstring…

High Energy Physics - Theory · Physics 2008-11-26 I. Ya. Aref'eva , D. M. Belov , A. S. Koshelev , P. B. Medvedev

Classical configurations of a M2-brane, a D2-brane and D0-branes are investigated in the background of an infinite array of M5-branes or NS5-branes. On the M2-brane, we discuss three kinds of configurations, such as a sphere, a cylinder and…

High Energy Physics - Theory · Physics 2009-11-07 Yoshifumi Hyakutake

Starting from an N=1 supersymmetric electric gauge theory with the multiple product gauge group and the bifundamentals, we apply Seiberg dual to each gauge group, obtain the N=1 supersymmetric dual magnetic gauge theories with dual matters…

High Energy Physics - Theory · Physics 2009-11-05 Changhyun Ahn

We consider a Dp brane within a D9 brane in the presence of a B-field whose polarization is {\em transverse} to the Dp brane. To be definite, we take a D3-D9 system. It is observed that the system has the same pattern of supersymmetry…

High Energy Physics - Theory · Physics 2009-10-31 M. Mihailescu , I. Y. Park , T. A. Tran

The study of open string tachyon condensation in string field theory can be drastically simplified by making an appropriate choice of coordinates on the space of string fields. We show that a very natural coordinate system is suggested by…

High Energy Physics - Theory · Physics 2009-10-31 David Kutasov , Marcos Marino , Gregory Moore

The moduli space of vacua for the confining phase of N=1 $Sp(N_c)$ supersymmetric gauge theories in four dimensions is studied by M theory fivebrane. We construct M theory fivebrane configuration corresponding to the perturbation of…

High Energy Physics - Theory · Physics 2009-10-30 Changhyun Ahn

We reconsider the dynamics of p anti-D3 branes inside the Klebanov-Strassler geometry, in which M units of R-R 3-form flux and K units of NS-NS 3-form flux are presented in deformed conifold. We find that anti-D3 branes blow up into a…

High Energy Physics - Theory · Physics 2007-05-23 Xiao-Jun Wang , Neng-Chao Xiao

We introduce a new type IIB 5-brane description for the E-string theory which is the world-volume theory on the M5-brane probing the end of the world M9-brane. The E-string in the new realization is depicted as spiral 5-branes web equipped…

High Energy Physics - Theory · Physics 2015-08-04 Sung-Soo Kim , Masato Taki , Futoshi Yagi

We investigate the effective worldvolume theories of branes in a background given by (the bosonic sector of) 10-dimensional massive IIA supergravity (``massive branes'') and their M-theoretic origin. In the case of the solitonic 5-brane of…

High Energy Physics - Theory · Physics 2009-10-30 E. Bergshoeff , Y. Lozano , T. Ortin

The near-horizon geometry of parallel NS5-branes is described by an exact superconformal 2d field theory based on K^10 = W(k)^4 x M^6, with M^6 a flat 5+1 space time and W(k)^4 =U(1) x SU(2)(k), a four dimensional background with…

High Energy Physics - Theory · Physics 2015-06-25 Costas Kounnas

We develop an approach to Khovanov homology of knots via gauge theory (previous physics-based approches involved other descriptions of the relevant spaces of BPS states). The starting point is a system of D3-branes ending on an NS5-brane…

High Energy Physics - Theory · Physics 2011-08-12 Edward Witten

An F-theory dual of a nonsupersymmetric orientifold is considered. It is argued that the condensation of both open and closed string tachyons in the orientifold corresponds to the annihilation of branes and anti-branes in the F-theory dual.…

High Energy Physics - Theory · Physics 2015-06-26 Atish Dabholkar

The worldvolume theory of coincident M5-branes is expected to contain a nonabelian 2-form/nonabelian gerbe gauge theory that is a higher analog of self-dual Yang-Mills theory. But the precise details -- in particular the global moduli /…

High Energy Physics - Theory · Physics 2015-03-13 Domenico Fiorenza , Hisham Sati , Urs Schreiber

We construct an action for NSNS 5-branes which is manifestly covariant under O(d,d). This is done by doubling $d$ of the spacetime coordinates which appear in the worldvolume action. By formulating the DBI part of the action in a manner…

High Energy Physics - Theory · Physics 2018-03-28 Chris D. A. Blair , Edvard T. Musaev