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9 - Emergent spacetime

Published online by Cambridge University Press:  05 August 2012

Robert De Mello Koch
Affiliation:
University of the Witwatersrand
Jeff Murugan
Affiliation:
University of Cape Town
Jeff Murugan
Affiliation:
University of Cape Town
Amanda Weltman
Affiliation:
University of Cape Town
George F. R. Ellis
Affiliation:
University of Cape Town
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Summary

We give an introductory account of the AdS/CFT correspondence in the ½-BPS sector of N =4 super Yang-Mills theory. Six of the dimensions of the string theory are emergent in the Yang-Mills theory. In this chapter we suggest how these dimensions and local physics in these dimensions emerge. The discussion is aimed at non-experts.

Introduction

The problem of quantizing gravity has proved to be a difficult one. To solve this problem, it seems to be necessary to answer the question “What is spacetime?” This challenges the most basic assumptions we are used to making; a radical new idea may be needed. Further, the hope of any guidance from experiment seems to be out of the question. One might conclude that the situation is hopeless. Drawing on recent insights from the AdS/CFT correspondence, we are nonetheless, optimistic.

The AdS/CFT correspondence [1] claims an exact equality between N =4 super Yang-Mills theory in flat (3+1)-dimensional Minkowski spacetime and Type IIB string theory on an asymptotically AdS5×S5 background. Type IIB string theory is a theory of closed strings; at least within string perturbation theory, theories of closed strings provide a consistent UV completion of gravity. The fact that such an equality exists is highly unexpected and non-trivial, and (as we will try to convince the reader) can be used to gain insight into the nature of spacetime. George Ellis opened the Foundations of Space and Time workshop by holding up two fingers and asking “are there an infinite or a finite number of places a particle could occupy between my fingers?” We don't know the answer to George's question.

Type
Chapter
Information
Foundations of Space and Time
Reflections on Quantum Gravity
, pp. 164 - 184
Publisher: Cambridge University Press
Print publication year: 2012

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References

[1] J. M., Maldacena, “The large N limit of superconformal field theories and supergravity,” Adv. Theor. Math. Phys. 2, 231 (1998) [Int. J. Theor. Phys. 38, 1113 (1999)] [arXiv:hep-th/9711200];Google Scholar
S. S., Gubser, I. R., Klebanov, and A. M., Polyakov, “Gauge theory correlators from non-critical string theory,” Phys. Lett.B 428, 105 (1998) [arXiv:hep-th/9802109];Google Scholar
E., Witten, “Anti-de Sitter space and holography,” Adv. Theor. Math. Phys. 2, 253 (1998) [arXiv:hep-th/9802150].Google Scholar
[2] S. R., Das and A., Jevicki, “String field theory and physical interpretation of D = 1 Strings,” Mod. Phys. Lett.A 5, 1639 (1990).Google Scholar
[3] S., Corley, A., Jevicki, and S., Ramgoolam, “Exact correlators of giant gravitons from dual N = 4 SYM theory,” Adv. Theor. Math. Phys. 5, 809 (2002) [arXiv:hep-th/0111222].Google Scholar
[4] D., Berenstein, “A toy model for the AdS]CFT correspondence,” JHEP 0407, 018 (2004) [arXiv:hep-th/0403110].Google Scholar
[5] H., Lin, O., Lunin, and J.M., Maldacena, “Bubbling AdS space and 1/2 BPS geometries,” JHEP 0410, 025 (2004) [arXiv:hep-th/0409174].Google Scholar
[6] V., Balasubramanian, J., de Boer, V., Jejjala, and J., Simon, “The library of Babel: On the origin of gravitational thermodynamics,” JHEP 0512, 006 (2005) [arXiv:hep-th/0508023];Google Scholar
V., Balasubramanian, V., Jejjala, and J., Simon, “The library of Babel,” Int. J. Mod. Phys.D 14, 2181 (2005) [arXiv:hep-th/0505123].Google Scholar
[7] D., Berenstein, “Large N BPS states and emergent quantum gravity,” JHEP 0601, 125 (2006) [arXiv:hep-th/0507203].Google Scholar
[8] V., Balasubramanian, D., Berenstein, B., Feng, and M. x., Huang, “D-branes in Yang–Mills theory and emergent gauge symmetry,” JHEP 0503, 006 (2005) [arXiv:hep-th/0411205].Google Scholar
[9] S., Ramgoolam, “Schur–Weyl duality as an instrument of gauge–string duality,” arXiv:0804.2764 [hep-th].
[10] D., Berenstein, J. M., Maldacena, and H., Nastase, “Strings in flat space and pp waves from N = 4 super Yang–Mills,” JHEP 0204, 013 (2002) [arXiv:hep-th/0202021].Google Scholar
[11] E., Brezin, C., Itzykson, G., Parisi, and J. B., Zuber, “Planar diagrams,” Commun. Math. Phys. 59, 35 (1978).Google Scholar
[12] R. C., Myers, “Dielectric-branes,” JHEP 9912, 022 (1999) [arXiv:hep-th/9910053].
[13] J., McGreevy, L., Susskind, and N., Toumbas, “Invasion of the giant gravitons from anti-de Sitter space,” JHEP 0006, 008 (2000) [arXiv:hep-th/0003075].Google Scholar
[14] V., Balasubramanian, M., Berkooz, A., Naqvi, and M. J., Strassler, “Giant gravitons in conformal field theory,” JHEP 0204, 034 (2002) [arXiv:hep-th/0107119].Google Scholar
[15] R., de Mello Koch and R., Gwyn, “Giant graviton correlators from dual SU(N) super Yang–Mills theory,” JHEP 0411, 081 (2004) [arXiv:hep-th/0410236];Google Scholar
T. W., Brown, “Half-BPS SU(N) correlators in N = 4 SYM,” arXiv:hep-th/0703202.
[16] T. W., Brown, R., de Mello Koch, S., Ramgoolam, and N., Toumbas, “Correlators, probabilities and topologies in N = 4 SYM,” JHEP 0703, 072 (2007) [arXiv:hep-th/0611290].Google Scholar
[17] S., Corley and S., Ramgoolam, “Finite factorization equations and sumrules for BPS correlators in N = 4 SYM theory,” Nucl. Phys.B 641, 131 (2002) [arXiv:hep-th/0205221].Google Scholar
[18] T. W., Brown, P. J., Heslop, and S., Ramgoolam, “Diagonal multi-matrix correlators and BPS operators in N = 4 SYM,” arXiv:0711.0176 [hep-th];
T. W., Brown, “Permutations and the loop,” JHEP 0806, 008 (2008) [arXiv:0801.2094 [hep-th]];Google Scholar
T.W., Brown, P. J., Heslop, and S., Ramgoolam, “Diagonal free field matrix correlators, global symmetries and giant gravitons,” JHEP 0904, 089 (2009) [arXiv:0806.1911 [hep-th]].Google Scholar
[19] Y., Kimura and S., Ramgoolam, “Branes, anti-branes and Brauer algebras in gauge–gravity duality,” arXiv:0709.2158 [hep-th];
Y., Kimura, “Non-holomorphic multi-matrix gauge invariant operators based on Brauer algebra,” arXiv:0910.2170 [hep-th].
[20] R., Bhattacharyya, S., Collins, and R., de Mello Koch, “Exact multi-matrix correlators,” arXiv:0801.2061 [hep-th];
R., Bhattacharyya, R., de Mello Koch, and M., Stephanou, “Exact multi-restricted Schur polynomial correlators,” JHEP 0806, 101 (2008) [arXiv:0805.3025 [hep-th]];
S., Collins, “Restricted Schur polynomials and finite N counting,” Phys. Rev.D 79, 026002 (2009) [arXiv:0810.4217 [hep-th]].Google Scholar
[21] Y., Kimura and S., Ramgoolam, “Enhanced symmetries of gauge theory and resolving the spectrum of local operators,” Phys. Rev.D 78, 126003 (2008) [arXiv:0807.3696 [hep-th]].Google Scholar
[22] M., Bianchi, D. Z., Freedman, and K., Skenderis, “How to go with an RG flow,” JHEP 0108, 041 (2001) [arXiv:hep-th/0105276];Google Scholar
M., Bianchi, D. Z., Freedman, and K., Skenderis, “Holographic renormalization,” Nucl. Phys.B 631, 159 (2002) [arXiv:hep-th/0112119];Google Scholar
K., Skenderis, “Lecture notes on holographic renormalization,” Class. Quant. Grav. 19, 5849 (2002) [arXiv:hep-th/0209067].Google Scholar
[23] K., Skenderis and M., Taylor, “Kaluza–Klein holography,” JHEP 0605, 057 (2006) [arXiv:hep-th/0603016];Google Scholar
K., Skenderis and M., Taylor, “Anatomy of bubbling solutions,” JHEP 0709, 019 (2007) [arXiv:0706.0216 [hep-th]].Google Scholar
[24] S., Lee, S., Minwalla, M., Rangamani, and N., Seiberg, “Three-point functions of chiral operators in D =4, N = 4 SYM at large N,” Adv. Theor. Math. Phys. 2, 697 (1998) [arXiv:hep-th/9806074];Google Scholar
K. A., Intriligator, “Bonus symmetries of N = 4 super-Yang–Mills correlation functions via AdS duality,” Nucl. Phys.B 551, 575 (1999) [arXiv:hep-th/9811047];Google Scholar
B. U., Eden, P. S., Howe, A., Pickering, E., Sokatchev and P. C., West, “Four-point functions in N = 2 superconformal field theories,” Nucl. Phys.B 581, 523 (2000) [arXiv:hep-th/0001138];Google Scholar
B. U., Eden, P. S., Howe, E., Sokatchev and P. C., West, “Extremal and next-to-extremal n-point correlators in four-dimensional SCFT,” Phys. Lett.B 494, 141 (2000) [arXiv:hep-th/0004102].Google Scholar
[25] C., Kristjansen, J., Plefka, G. W., Semenoff and M., Staudacher, “A new double-scaling limit of N = 4 super Yang–Mills theory and PP-wave strings,” Nucl. Phys.B 643, 3 (2002) [arXiv:hep-th/0205033];Google Scholar
N. R., Constable, D. Z., Freedman, M., Headrick, S., Minwalla, L., Motl, A., Postnikov and W., Skiba, “PP-wave string interactions from perturbative Yang–Mills theory,” JHEP 0207, 017 (2002) [arXiv:hep-th/0205089].Google Scholar
[26] J.A., Minahan and K., Zarembo, “The Bethe-ansatz for N =4 super Yang–Mills,” JHEP 0303, 013 (2003) [arXiv:hep-th/0212208].Google Scholar
[27] N., Beisert and M., Staudacher, “The N =4 SYM Integrable Super Spin Chain,” Nucl. Phys.B 670, 439 (2003) [arXiv:hep-th/0307042].Google Scholar
[28] N., Beisert, C., Kristjansen and M., Staudacher, “The dilatation operator of N =4 super Yang–Mills theory,” Nucl. Phys.B 664, 131 (2003) [arXiv:hep-th/0303060].Google Scholar
[29] M., Kruczenski, “Spin chains and string theory,” Phys. Rev. Lett. 93, 161602 (2004) [arXiv:hep-th/0311203].Google Scholar
M., Kruczenski, A. V., Ryzhov and A.A., Tseytlin, “Large spin limit of AdS(5) × S**5 string theory and low energy expansion of ferromagnetic spin chains,” Nucl. Phys.B 692, 3 (2004) [arXiv:hep-th/0403120].Google Scholar
[30] M. T., Grisaru, R. C., Myers and O., Tafjord, “SUSY and Goliath,” JHEP 0008, 040 (2000) [arXiv:hep-th/0008015].Google Scholar
[31] A., Hashimoto, S., Hirano and N., Itzhaki, “Large branes in AdS and their field theory dual,” JHEP 0008, 051 (2000) [arXiv:hep-th/0008016].Google Scholar
[32] R., de Mello Koch, J., Smolic and M., Smolic, “Giant Gravitons - with Strings Attached (I),” JHEP 0706, 074 (2007), arXiv:hep-th/0701066.Google Scholar
[33] D., Berenstein, D. H., Correa and S. E., Vazquez, “A study of open strings ending on giant gravitons, spin chains and integrability,” [arXiv:hep-th/0604123];
D., Berenstein, D. H., Correa and S. E., Vazquez, “Quantizing open spin chains with variable length: An example from giant gravitons,” Phys. Rev. Lett. 95, 191601 (2005) [arXiv:hep-th/0502172];Google Scholar
D. H., Correa and G. A., Silva, “Dilatation operator and the super Yang–Mills duals of open strings on AdS giant gravitons,” JHEP 0611, 059 (2006) [arXiv:hep-th/0608128].Google Scholar
[34] R., de Mello Koch, J., Smolic and M., Smolic, “Giant gravitons – with strings attached (II),” JHEP 0709 049 (2007) [arXiv:hep-th/0701067];Google Scholar
D., Bekker, R., de Mello Koch and M., Stephanou, “Giant gravitons – with strings attached (III),” JHEP 0802, 029 (2008) [arXiv:0710.5372 [hep-th]].Google Scholar
[35] A., Hamilton and J., Murugan, “On the shoulders of giants – quantum gravity and braneworld stability,” [arXiv:0806.3273 [gr-qc]]
[36] L., Grant, L., Maoz, J., Marsano, K., Papadodimas and V. S., Rychkov, “Minisuperspace quantization of ‘bubbling AdS’ and free fermion droplets,” JHEP 0508, 025 (2005) [arXiv:hep-th/0505079];Google Scholar
L., Maoz and V. S., Rychkov, “Geometry quantization from supergravity: The case of ‘bubbling AdS’,” JHEP 0508, 096 (2005) [arXiv:hep-th/0508059].Google Scholar
[37] R., de Mello Koch, “Geometries from Young diagrams,” JHEP 0811, 061 (2008) [arXiv:0806.0685 [hep-th]].Google Scholar
[38] R., de Mello Koch, N., Ives, and M., Stephanou, “Correlators in nontrivial backgrounds,” Phys. Rev.D 79, 026004 (2009) [arXiv:0810.4041 [hep-th]].Google Scholar
[39] K., Skenderis and M., Taylor, “Anatomy of bubbling solutions,” JHEP 0709, 019 (2007) [arXiv:0706.0216 [hep-th]].Google Scholar
[40] R., de Mello Koch, T. K., Dey, N., Ives, and M., Stephanou, “Correlators of operators with a large R-charge,” arXiv:0905.2273 [hep-th].
[41] S. E., Vazquez, “Reconstructing 1/2 BPS space-time metrics from matrix models and spin chains,” Phys. Rev.D 75, 125012 (2007) [arXiv:hep-th/0612014].Google Scholar
[42] H.Y., Chen, D. H., Correa, and G.A., Silva, “Geometry and topology of bubble solutions from gauge theory,” Phys. Rev.D 76, 026003 (2007) [arXiv:hep-th/0703068].Google Scholar
[43] G., Mandal, “Fermions from half-BPS supergravity,” JHEP 0508, 052 (2005) [arXiv:hep-th/0502104].Google Scholar
[44] M., Masuku and J. P., Rodrigues, “Laplacians in polar matrix coordinates and radial fermionization in higher dimensions,” arXiv:0911.2846 [hep-th];
Y., Kimura, S., Ramgoolam, and D., Turton, “Free particles from Brauer algebras in complexmatrix models,” arXiv:0911.4408 [hep-th].
[45] D., Berenstein, “A strong coupling expansion for N = 4 SYM theory and other SCFT's,” arXiv:0804.0383 [hep-th];
D. E., Berenstein and S. A., Hartnoll, “Strings on conifolds from strong coupling dynamics: quantitative results,” JHEP 0803 (2008) 072 [arXiv:0711.3026 [hep-th]];Google Scholar
D., Berenstein, “Strings on conifolds from strong coupling dynamics, part I,” JHEP 0804 (2008) 002 [arXiv:0710.2086 [hep-th]];Google Scholar
D. E., Berenstein, M., Hanada, and S.A., Hartnoll, “Multi-matrix models and emergent geometry,” JHEP 0902, 010 (2009) [arXiv:0805.4658 [hep-th]].Google Scholar
[46] A., Jevicki and B., Sakita, “The quantum collective field method and its application to the planar limit,” Nucl. Phys.B 165, 511 (1980);Google Scholar
A., Jevicki and B., Sakita, “Collective field approach to the large N limit: Euclidean field theories,” Nucl. Phys.B 185, 89 (1981).Google Scholar
[47] J. P., Rodrigues, “Large N spectrum of two matrices in a harmonic potential and BMN energies,” JHEP 0512, 043 (2005) [arXiv:hep-th/0510244];Google Scholar
A., Donos, A., Jevicki, and J. P., Rodrigues, “Matrix model maps in AdS/CFT,” Phys. Rev.D 72, 125009 (2005) [arXiv:hep-th/0507124];Google Scholar
R., de Mello Koch, A., Jevicki, and J. P., Rodrigues, “Instantons in c=0 CSFT,” JHEP 0504, 011 (2005) [arXiv:hep-th/0412319];Google Scholar
R., de Mello Koch, A., Donos, A., Jevicki, and J. P., Rodrigues, “Derivation of string field theory from the large N BMN limit,” Phys. Rev.D 68, 065012 (2003) [arXiv:hep-th/0305042];Google Scholar
R., de Mello Koch, A., Jevicki, and J. P., Rodrigues, “Collective string field theory of matrix models in the BMN limit,” Int. J. Mod. Phys.A 19, 1747 (2004) [arXiv:hep-th/0209155].Google Scholar
[48] A., Donos, “A description of 1/4 BPS configurations in minimal type IIB SUGRA,” Phys. Rev.D 75, 025010 (2007) [arXiv:hep-th/0606199/;Google Scholar
B., Chen et al., “Bubbling AdS and droplet descriptions of BPS geometries in IIB supergravity,” JHEP 0710, 003 (2007) [arXiv:0704.2233 [hep-th]];Google Scholar
O., Lunin, “Brane webs and 1/4-BPS geometries,” arXiv:0802.0735 [hep-th].

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