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## Macroscopic strings as heavy quarks in large N gauge theory and Anti-de Sitter supergravity

Venue: | PHYS. J. C22 |

Citations: | 508 - 1 self |

### Citations

5608 | The large N limit of superconformal field theories and supergravity
- Maldacena
- 1998
(Show Context)
Citation Context ...built on earlier study of near-horizon geometry of D- and M-branes [2] and their absorption and Hawking emission processes [3], Maldacena has put forward a remarkable proposal to the large N behavior =-=[4]-=-. According to his proposal, large N limit of d-dimensional conformal field theories with sixteen supercharges is governed in dual description by maximal supergravity theories (chiral or non-chiral de... |

2753 |
Gauge theory correlators from non-critical string theory, Phys. Lett. B428
- Gubser, Klebanov, et al.
- 1998
(Show Context)
Citation Context ...chiral or non-chiral depending on d) with thirty-two supercharges that are compactified on adSd+1 times internal round sphere. Extention [5] to nonconformally invariant field theories and new results =-=[6, 7, 8, 9]-=- extending Maldacena’s proposal have been reported. The most tractible example of Maldacena’s proposal is four-dimensional N = 4 super YangMills theory with gauge group U(N). The theory is superconfor... |

371 | Anti de Sitter space and holography
- Witten
- 1998
(Show Context)
Citation Context ...chiral or non-chiral depending on d) with thirty-two supercharges that are compactified on adSd+1 times internal round sphere. Extention [5] to nonconformally invariant field theories and new results =-=[6, 7, 8, 9]-=- extending Maldacena’s proposal have been reported. The most tractible example of Maldacena’s proposal is four-dimensional N = 4 super YangMills theory with gauge group U(N). The theory is superconfor... |

249 | Brane dynamics from the Born-Infeld action,” Nucl
- Callan, Maldacena
- 1998
(Show Context)
Citation Context ...f semi-infinite strings ending on D3-branes. From Polchinski’s conformal field theory point of view, which is exact at λIIB = 0, the end of 3 This is exactly the same argument as Callan and Maldacena =-=[11]-=-. 5fundamental string represents an electric charge (likewise, the end of D-string representing a magnetic charge). For semi-infinite string, the electrically charged object has infinite inertia mass... |

195 |
Born-Infeld particles and Dirichlet p-branes
- Gibbons
- 1998
(Show Context)
Citation Context ...as infinite inertia mass, hence, is identified with a heavy quark Q (or anti-quark ¯ Q). An important observation has been advanced recently by Callan and Maldacena [11] (and independently by Gibbons =-=[12]-=- and by Howe, Lambert and West [13]) that the semi-infinite fundamental string can be realized as a deformation of the D3-brane world-volume. It was also emphasized by Callan and Maldacena that full-f... |

73 | The self-dual string soliton
- Howe, Lambert, et al.
- 1998
(Show Context)
Citation Context ... identified with a heavy quark Q (or anti-quark ¯ Q). An important observation has been advanced recently by Callan and Maldacena [11] (and independently by Gibbons [12] and by Howe, Lambert and West =-=[13]-=-) that the semi-infinite fundamental string can be realized as a deformation of the D3-brane world-volume. It was also emphasized by Callan and Maldacena that full-fledged Born-Infeld analysis is nece... |

61 | Probing Five-Dimensional Black Holes with D-Branes
- Douglas, Polchinski, et al.
(Show Context)
Citation Context ...ction to string theory but it has never been clear how and to what extent the string is related to the fundamental string. Recently, built on earlier study of near-horizon geometry of D- and M-branes =-=[2]-=- and their absorption and Hawking emission processes [3], Maldacena has put forward a remarkable proposal to the large N behavior [4]. According to his proposal, large N limit of d-dimensional conform... |

53 | Spectrum of large N gauge theory from supergravity
- Horowitz, Ooguri
- 1998
(Show Context)
Citation Context ...chiral or non-chiral depending on d) with thirty-two supercharges that are compactified on adSd+1 times internal round sphere. Extention [5] to nonconformally invariant field theories and new results =-=[6, 7, 8, 9]-=- extending Maldacena’s proposal have been reported. The most tractible example of Maldacena’s proposal is four-dimensional N = 4 super YangMills theory with gauge group U(N). The theory is superconfor... |

43 |
Three-Pronged Strings and 1/4
- Bergman
- 1998
(Show Context)
Citation Context ...o look for a string configuration that can be interpreted as a N-quark state on the D3-brane world-volume. Recently, utilizing triple BPS string junction [?], such a configuration has been identified =-=[24]-=-: N-pronged string junction interconnecting N D3-branes. For example, for gauge group SU(3) realized by three D3-branes, multi-monopole configuration that may be interpreted as the static baryon is a ... |

35 |
Shigehara: Realizing discontinuous wave functions with renormalized short-range potentials, Phys. Lett. A243
- Cheon, T
- 1998
(Show Context)
Citation Context ... Dirichlet and Neumann boundary conditions, respectively. For the worldvolume BPS soliton, we will show that these boundary conditions arise quite naturally as a consequence of self-adjoint extension =-=[14, 15]-=- of small fluctuation operators along the elongated D3-brane worldvolume of BPS soliton. This paper is organized as follows. In Section 2, we study dynamics of a macroscopic Type IIB string, using the... |

34 |
Gauge fields as composite boundary excitations”, CERN preprint CERN-TH-98-49
- Ferrara, Fronsdal
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Citation Context |

11 | A matrix string interpretation of the large N loop equation,” hep-th/9705029
- Verlinde
(Show Context)
Citation Context ...son loop as the area enclosed is slightly deformed. More recently, based on dual description of large N gauge theory in 1+1 dimensions in terms of near-critical electric field on a D-string, Verlinde =-=[24]-=- has shown that Wilson loop equation follows as the conformal Ward identity on the string world-sheet. Immediate question that arise is, relying on the SO(4, 2) conformal invariance of large N super Y... |

2 |
461; Planar Diagram Field Theories
- B72
- 1974
(Show Context)
Citation Context ...erstanding of D-brane dynamics, new approaches to outstanding problems in gauge theory have become available. One of such problems is regarding the behavior of SU(N) gauge theory in the large N limit =-=[1]-=-: N → ∞ with ‘t Hooft coupoing g 2 eff = g 2 YMN fixed. Planar diagram dominance as shown first by ‘t Hooft has been regarded as an indicative of certain connection to string theory but it has never b... |

1 |
High-Energy Phys. 9712
- Douglas, Polchinski, et al.
- 1997
(Show Context)
Citation Context ...ction to string theory but it has never been clear how and to what extent the string is related to the fundamental string. Recently, built on earlier study of near-horizon geometry of D- and M-branes =-=[2]-=- and their absorption and Hawking emission processes [3], Maldacena has put forward a remarkable proposal to the large N behavior [4]. According to his proposal, large N limit of d-dimensional conform... |

1 |
High-Energy Phys. 9803
- B423
- 1998
(Show Context)
Citation Context ...figuration obeying N-ality. Clearly, we need to look for a string configuration that can be interpreted as a N-quark state on the D3-brane world-volume. Recently, utilizing triple BPS string junction =-=[17, 25]-=-, such a configuration has been identified [26]: N-pronged string junction interconnecting N D3-branes. For example, for gauge group SU(3) realized by three D3-branes, multi-monopole configuration tha... |