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We analyze certain brane bound states in M-theory and their descendants in type IIA string theory, all involving 3-form or 2-form background fluxes. Among them are configurations which represent NCYM, NCOS and ODp-theories in the scaling…

High Energy Physics - Theory · Physics 2016-10-26 Boris Kors , Dieter Lust , Andre Miemiec

In this paper we study general properties of noncommutative field theories obtained from the Seiberg-Witten limit of string theories in the presence of an external B-field. We analyze the extension of the Wightman axioms to this context and…

High Energy Physics - Theory · Physics 2010-04-06 L. Alvarez-Gaume , M. A. Vazquez-Mozo

We study scalar field and string theory on non commutative q-deformed spaces. We define a product of functions on a non commutative algebra of functions resulting from the q-deformation analogue to the Moyal product for canonically non…

High Energy Physics - Theory · Physics 2023-01-10 Poula Tadros

It is shown that the dual of the double compactified D=11 Supermembrane and a suitable compactified D=10 Super 4D-brane with nontrivial wrapping on the target space may be formulated as noncommutative gauge theories. The Poisson bracket…

High Energy Physics - Theory · Physics 2011-05-19 I. Martin , J. Ovalle , A. Restuccia

We describe how the presence of the antisymmetric tensor (torsion) on the world sheet action of string theory renders the size of the target space a gauge non invariant quantity. This generalizes the R <--> 1/R symmetry in which momenta and…

High Energy Physics - Theory · Physics 2009-10-31 Fedele Lizzi

In this paper we consider the quantization of open strings ending on D-branes with a background B field. We find that spacetime coordinates of the open string end-points become noncommutative, and correspondingly the D-brane worldvolume…

High Energy Physics - Theory · Physics 2009-10-31 Chong-Sun Chu , Pei-Ming Ho

The non-commutative geometry of a large auxiliary $B$-field simplifies the construction of D-branes as solitons in open string field theory. Similarly, fundamental strings are constructed as localized flux tubes in the string field theory.…

High Energy Physics - Theory · Physics 2009-10-31 Jeffrey A. Harvey , Per Kraus , Finn Larsen , Emil J. Martinec

In typical examples of the AdS/CFT correspondence, the world-sheet theory with holes in the presence of D-branes is assumed to be equivalent in a low-energy limit to a world-sheet theory without holes for a different background such as…

High Energy Physics - Theory · Physics 2020-07-01 Yuji Okawa

Infinite-dimensional Grassmannian manifold contains moduli spaces of Riemann surfaces of all genera. This well known fact leads to a conjecture that non-perturbative string theory can be formulated in terms of Grassmannian. We present new…

High Energy Physics - Theory · Physics 2010-11-19 Albert Schwarz

In an earlier work it was shown that the IR singularities arising in the nonplanar one loop two point function of a noncommutative ${\cal N}=2$ gauge theory can be reproduced exactly from the massless closed string exchanges. The…

High Energy Physics - Theory · Physics 2009-11-11 Swarnendu Sarkar

The consequences of noncommutativity of space coordinates of string theory in the proposed large extra dimension solution to the hierarchy problem are explored; in particular the large dimension stabilization and the graviton reabsorption…

High Energy Physics - Theory · Physics 2007-05-23 Farhad Ardalan

We investigate the open string modes, describing the world-volume of a D p-brane, for its cyclic symmetry in presence of a magnetic field. It is argued that the constant coordinate modes receive non-perturbative correction. We show that…

High Energy Physics - Theory · Physics 2009-10-31 Supriya Kar

We outline a brief description of non commutative geometry and present some applications in string theory. We use the fuzzy torus as our guiding example.

High Energy Physics - Theory · Physics 2009-11-10 Daniela Bigatti

We examine the role of non-commutative geometry in D$p$-branes within large R-R field backgrounds. In this context, the background of a significant ($p-1$)-form R-R field can be effectively described using a ($p-1$)-bracket, similar to the…

High Energy Physics - Theory · Physics 2025-11-17 Chen-Te Ma

We construct a simple physical model of a particle moving on the infinite noncommutative 2-plane. The model consists of a pair of opposite charges moving in a strong magnetic field. In addition, the charges are connected by a spring. In the…

High Energy Physics - Theory · Physics 2009-10-07 Daniela Bigatti , Leonard Susskind

Nowadays, noncommutative geometry is a growing domain of mathematics, which can appear as a promising framework for modern physics. Quantum field theories on "noncommutative spaces" are indeed much investigated, and suffer from a new type…

Mathematical Physics · Physics 2011-08-22 Axel de Goursac

We perform the consistent quantization of open string D-brane in non-constant NS-NS closed string B field background by directly imposing the worldsheet conformal symmetry. In addition to the previous noncommutative D-brane coordinates…

High Energy Physics - Theory · Physics 2016-09-06 Jen-Chi Lee

The Seiberg-Witten limit of fermionic N=2 string theory with nonvanishing B-field is governed by noncommutative self-dual Yang-Mills theory (ncSDYM) in 2+2 dimensions. Conversely, the self-duality equations are contained in the equation of…

High Energy Physics - Theory · Physics 2009-11-07 Matthias Ihl , Sebastian Uhlmann

A remarkable feature of D-branes is the appearance of a nonabelian gauge theory in the description of several (nearly) coincident branes. This nonabelian structure plays an important role in realizing various geometric effects with…

High Energy Physics - Theory · Physics 2009-11-10 Robert C. Myers

The large order growth of string perturbation theory in $c\le 1$ conformal field theory coupled to world sheet gravity implies the presence of $O(e^{-{1\over g_s}})$ non-perturbative effects, whose leading behavior can be calculated in the…

High Energy Physics - Theory · Physics 2009-11-10 Sergei Yu. Alexandrov , Vladimir A. Kazakov , David Kutasov