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Macroscopic strings as heavy quarks in large N gauge theory and Antide Sitter supergravity
 PHYS. J. C22
"... Maldacena has put forward large N correspondence between superconformal field theories on the brane and antide Sitter supergravity in spacetime. We study some aspects of the correspondence between N = 4 superconformal gauge theory on D3brane and maximal supergravity on adS5 × S5 by introducing mac ..."
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Cited by 508 (1 self)
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Maldacena has put forward large N correspondence between superconformal field theories on the brane and antide Sitter supergravity in spacetime. We study some aspects of the correspondence between N = 4 superconformal gauge theory on D3brane and maximal supergravity on adS5 × S5 by introducing
Solitonic Dbranes and brane annihilation
, 2002
"... We point out some intriguing analogies between field theoretic solitons (topological defects) and Dbranes. Annihilating solitonantisoliton pairs can produce stable solitons of lower dimensionality. Solitons that localize massless gauge fields in their world volume automatically imply the existence ..."
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We point out some intriguing analogies between field theoretic solitons (topological defects) and Dbranes. Annihilating solitonantisoliton pairs can produce stable solitons of lower dimensionality. Solitons that localize massless gauge fields in their world volume automatically imply
Tachyon condensation on the braneantibrane system
 JHEP
, 1998
"... A coincident Dbrane antiDbrane pair has a tachyonic mode. We present an argument showing that at the classical minimum of the tachyonic potential the negative energy density associated with the potential exactly cancels the sum of the tension of the brane and the antibrane, thereby giving a con ..."
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Cited by 307 (10 self)
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A coincident Dbrane antiDbrane pair has a tachyonic mode. We present an argument showing that at the classical minimum of the tachyonic potential the negative energy density associated with the potential exactly cancels the sum of the tension of the brane and the antibrane, thereby giving a
Brane/Flux Annihilation and the String Dual of a NonSupersymmetric Field Theory
, 2006
"... We consider the dynamics of p antiD3 branes inside the KlebanovStrassler geometry, the deformed conifold with M units of RR 3form flux around the S 3. We find that for p << M the system relaxes to a nonsupersymmetric NS 5brane “giant graviton ” configuration, which is classically stable, b ..."
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Cited by 170 (18 self)
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We consider the dynamics of p antiD3 branes inside the KlebanovStrassler geometry, the deformed conifold with M units of RR 3form flux around the S 3. We find that for p << M the system relaxes to a nonsupersymmetric NS 5brane “giant graviton ” configuration, which is classically stable
Heating in brane inflation and hidden dark matter
, 2006
"... Towards the end of brane inflation, the brane pair annihilation produces massive closed strings. The transfer of this energy to Standard Model (SM) open string modes depends on where the SM branes and the brane annihilation are located: in the bulk, in the same throat or in different throats. We fi ..."
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Cited by 21 (6 self)
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Towards the end of brane inflation, the brane pair annihilation produces massive closed strings. The transfer of this energy to Standard Model (SM) open string modes depends on where the SM branes and the brane annihilation are located: in the bulk, in the same throat or in different throats. We
Bound states and brane annihilation in 11 D SUGRA
, 1998
"... We study scattering of D0 branes in eleven dimensional supergravity (SUGRA) using the tree level four point amplitude. The range of validity of SUGRA allows us to make reliable calculations of relativistic brane scattering, inaccessible in string theory because of halo effects. We also compare the r ..."
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the rate of annihilation of D0 − ¯ D0 branes to the rate of elastic D0 − ¯ D0 scattering and find that the former is always smaller than the latter. We also find a pole in σD0−D0 ¯. We exploit the analogy with the positronium to argue that the brane antibrane pairs form branium atoms in 3 spatial
Annihilation
"... With a currentsplitting technique, we calculate the gaugeinvariant initialstate radiation to order O(ff) with softphoton exponentiation for on and offshell W pair production. This result generalizes the convolution formula, which is known from the description of the Z resonance, to the case ..."
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With a currentsplitting technique, we calculate the gaugeinvariant initialstate radiation to order O(ff) with softphoton exponentiation for on and offshell W pair production. This result generalizes the convolution formula, which is known from the description of the Z resonance, to the case
Confinement on the brane
 Nucl. Phys. B
, 2000
"... A nonperturbative confinement mechanism has been proposed to explain the fate of the unbroken gauge group on the worldvolume of annihilating DbraneantiDbrane pairs. In this paper, we examine this phenomenon closely from several different perspectives. Existence of the confinement mechanism is ..."
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Cited by 22 (2 self)
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A nonperturbative confinement mechanism has been proposed to explain the fate of the unbroken gauge group on the worldvolume of annihilating DbraneantiDbrane pairs. In this paper, we examine this phenomenon closely from several different perspectives. Existence of the confinement mechanism
Orientifolds and Mirror symmetry
, 2003
"... We study parity symmetries and crosscap states in classes of N = 2 supersymmetric quantum field theories in 1+1 dimensions, including nonlinear sigma models, gauged WZW models, LandauGinzburg models, and linear sigma models. The parity anomaly and its cancellation play important roles in many of t ..."
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Cited by 271 (11 self)
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of them. The case of the N = 2 minimal model are studied in RCFT, and LG models. We also identify mirror pairs of orientifolds, extending the correspondence between symplectic geometry and algebraic geometry by including unorientable worldsheets. Through the analysis in various models and comparison
hepth/0208068 Fluxbranes Delaying BraneAntibrane Annihilation
, 2002
"... By intersecting the RR charged Dp − ¯ Dp pair (p = 6,4,2,0) with the RR F7brane and by intersecting the NSNS charged F1 − ¯ F1 and NS5 − ¯ NS5 pairs with the NSNS F6branes, the possibility of stabilizing the braneantibrane systems is considered. The behavior of the corresponding supergravity so ..."
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By intersecting the RR charged Dp − ¯ Dp pair (p = 6,4,2,0) with the RR F7brane and by intersecting the NSNS charged F1 − ¯ F1 and NS5 − ¯ NS5 pairs with the NSNS F6branes, the possibility of stabilizing the braneantibrane systems is considered. The behavior of the corresponding supergravity
Results 1  10
of
1,471