Approaches to Quantum Gravity

186 G. Horowitz and J. Polchinski[29] H. Lin, O. Lunin & J. Maldacena, Bubbling AdS space and 1/2 BPS geometries,JHEP 0410 (2004) 025 [arXiv:hep-th/0409174].[30] J. M. Maldacena, The large N limit of superconformal field theories andsupergravity. Adv. Theor. Math. Phys. 2 (1998) 231 [arXiv:hep-th/9711200].[31] J. M. Maldacena, Wilson loops in large N field theories. Phys. Rev. Lett. 80 (1998)4859 [arXiv:hep-th/9803002].[32] J. M. Maldacena & A. Strominger, AdS(3) black holes and a stringy exclusionprinciple. JHEP 9812 (1998) 005 [arXiv:hep-th/9804085].[33] J. McGreevy, L. Susskind & N. Toumbas, Invasion of the giant gravitons fromanti-de Sitter space. JHEP 0006 (2000) 008 [arXiv:hep-th/0003075].[34] J. Polchinski & M. J. Strassler, Deep inelastic scattering and gauge/string duality.JHEP 0305 (2003) 012 [arXiv:hep-th/0209211].[35] S. J. Rey & J. T. Yee, Macroscopic strings as heavy quarks in large N gauge theoryand anti-de Sitter supergravity. Eur. Phys. J. C 22 (2001) 379[arXiv:hep-th/9803001].[36] E. Silverstein, (A)dS backgrounds from asymmetric orientifolds (2001)arXiv:hep-th/0106209.[37] A. Strominger, The dS/CFT correspondence. JHEP 0110 (2001) 034[arXiv:hep-th/0106113].[38] L. Susskind, The world as a hologram. J. Math. Phys. 36 (1995) 6377[arXiv:hep-th/9409089].[39] L. Susskind, The anthropic landscape of string theory (2003) arXiv:hep-th/0302219.[40] K. S. Thorne, R. H. Price & D. A. Macdonald, Black Holes: The MembraneParadigm (New Haven, Yale, 1986).[41] S. Weinberg & E. Witten, Limits on massless particles. Phys. Lett. B 96 (1980)59–62.[42] E. Witten, Anti-de Sitter space and holography. Adv. Theor. Math. Phys. 2 (1998)253 [arXiv:hep-th/9802150].[43] E. Witten, Anti-de Sitter space, thermal phase transition, and confinement in gaugetheories. Adv. Theor. Math. Phys. 2 (1998) 505 [arXiv:hep-th/9803131].[44] E. Witten, Quantum gravity in de Sitter space (2001) arXiv:hep-th/0106109.