brane intersection of D2-branes with D6-branes; special case of Dp-D(p+4)-brane bound state
brane intersections/bound states/wrapped branes/polarized branes
D-branes and anti D-branes form bound states by tachyon condensation, thought to imply the classification of D-brane charge by K-theory
intersecting D-branes/fuzzy funnels:
Dp-D(p+6) brane bound state
As black branes (D2-D6-NS5 brane bound state):
Konstadinos Sfetsos, Kostas Skenderis, Section 2.2 of: Microscopic derivation of the Bekenstein-Hawking entropy formula for non-extremal black holes, Nucl. Phys. B517 (1998) 179-204 (arXiv:hep-th/9711138)
Oskar Pelc, Ruud Siebelink, The D2-D6 System and a Fibered AdS Geometry, Nucl. Phys. B 558 (1999) 127-158 [arXiv:hep-th/9902045, doi:10.1016/S0550-3213(99)00332-6]
Federico Faedo, Yolanda Lozano, Nicolo Petri, Searching for surface defect CFTs within , JHEP 11 (2020) 052 (arXiv:2007.16167)
blackD4-D8-brane bound states in massive type IIA string theory, with defect D2-D6-brane bound states inside them realizing AdS3-CFT2 “inside” AdS7-CFT6:
Giuseppe Dibitetto, Nicolò Petri, Surface defects in the D4 − D8 brane system, JHEP 01 (2019) 193 (arxiv:1807.07768)
Giuseppe Dibitetto, Nicolò Petri, vacua and surface defects in massive IIA (arxiv:1904.02455)
Discussion of black hole entropy of D2-D6 brane bound states as black holes in string theory:
Juan Maldacena, Andrew Strominger, Statistical Entropy of Four-Dimensional Extremal Black Holes, Phys. Rev. Lett. 77:428-429, 1996 (arXiv:hep-th/9603060)
Konstadinos Sfetsos, Kostas Skenderis, Microscopic derivation of the Bekenstein-Hawking entropy formula for non-extremal black holes, Nucl. Phys. B517 (1998) 179-204 (arXiv:hep-th/9711138)
Last revised on June 18, 2023 at 16:44:00. See the history of this page for a list of all contributions to it.