2015/09/22 Selected Topics in Theoretical High Energy physics@Tbilisi State Univ., Georgia Towards the gravity/CYBE correspondence Kentaroh Yoshida (Dept. of Phys., Kyoto U.) Based on collaboration with Takuya Matsumoto (Nagoya U.) Io Kawaguchi, Takashi Kameyama, Marcos Crichigno, Domenico Orlando, Susanne Reffert, Jun-ichi Sakamoto, Hideki Kyono, Andrzej Borowiec, Jerzy Lukierski 1 The AdS/CFT correspondence type IIB string on AdS5 x S5 Recent progress: 4D SU(N) SYM the discovery of integrability behind the AdS/CFT [For a big review, Beisert et al., 1012.3982] The integrable structure provides powerful tools. It enables us to check the conjectured relations in the AdS/CFT without SUSY, even at finite coupling. EX anomalous dimensions, amplitudes etc. An enormous amount of works have been done, so far. Motivated by this success, our interest here is the classical integrability on the string-theory side. The existence of Lax pair (kinematical integrability) 2 The classical integrability of the AdS5 x S5 superstring The coset structure of AdS5 x S5 is closely related to the integrability. : symmetric coset Z2-grading classical integrability Including fermions : super coset [Metsaev-Tseytlin, 1998] Z4-grading classical integrability elucidated by [Bena-Polchinski-Roiban, 2003] This fact is the starting point of our later argument. 3 The next issue Integrable deformations of the AdS5 x S5 superstring Integrable deformations (as exactly solvable models) Integrability techniques EX Integrable twists deformed AdS5 x S5 geometries Solutions of type IIB SUGRA solution generation techniques EX TsT transformations One may consider various kinds of integrable deformations. There should be many associated solutions of type IIB SUGRA. Motive A classification of SUGRA solutions based on integrable deformations 4 A systematic deformation scheme Yang-Baxter sigma model Integrable deformation! [Klimcik, 2002, 2008] : const R : a linear op. a classical r-matrix satisfying modified classical Yang-Baxter eq. (mCYBE) The insertion of is a characteristic of this method. NOTE • An integrable deformation is specified by a classical r-matrix. • Given a classical r-matrix, a Lax pair follows automatically. 5 R-operators and classical r-matrices A linear R-operator A skew-symmetric classical r-matrix Two sources of classical r-matrix 1) modified classical Yang-Baxter eq. (mCYBE) the original work by Klimcik 2) classical Yang-Baxter eq. (CYBE) a possible generalization 6 The list of generalizations of Yang-Baxter sigma models (2 classes) (i) modified classical Yang-Baxter eq. (trigonometric) 1) Principal chiral model [Klimcik, hep-th/0210095, 0802.3518] 2) Symmetric coset sigma model [Delduc-Magro-Vicedo, 1308.3581] 3) Type IIB superstring on AdS5xS5 [Delduc-Magro-Vicedo, 1309.5850] (ii) classical Yang-Baxter eq. (rational) NOTE 1) Principal chiral model [Matsumoto-KY, 1501.03665] 2) Symmetric coset sigma model [Matsumoto-KY, 1501.03665] 3) Type IIB superstring on AdS5xS5 [Kawaguchi-Matsumoto-KY, 1401.4855] bi-Yang-Baxter sigma models are also constructed. [Klimcik, 0802.3518, 1402.2105] 7 Integrable deformations of the AdS5 x S5 superstring [Delduc-Magro-Vicedo, 1309.5850] [Kawaguchi-Matsumoto-KY, 1401.4855] Gravity/CYBE correspondence solutions of type IIB SUGRA classical r-matrices Claim The moduli space of a certain class of solutions of type IIB SUGRA is described by the classical Yang-Baxter equation. c.f., a droplet picture of free fermion in the bubbling geometry Droplet free fermion classical r-matrix CYBE [Lin-Lunin-Maldacena, 2005] (Just an analogy!) One may construct a new bubbling-like scenario. 8 The current status of the two deformations 1) Standard q-deformation ← mCYBE Talks by Arutyunov, Hoare Classical r-matrix of Drinfeld-Jimbo type Metric and B-field [Delduc-Magro-Vicedo, 1309.5850] [Arutyunov-Borsaro-Frolov, 1312.3542] AdSn x Sn [Hoare-Roiban-Tseytlin, 1403.5517] RR fluxes and dilaton for AdS2 x S2 and AdS3 x S3 Towards the complete gravity solution [Arutyunov-Borsaro-Frolov, 1507.04239] Minimal surfaces, quark-antiquark potential [Kameyama-KY, 1410.5544, 1510.NNNNN] c.f., Drukker-Forini, 1105.5144 2) [Lunin-Roiban-Tseytlin, 1411.1066] [Hoare-Tseytlin, 1508.01150] Poseter by Kameyama Non-standard q-deformation (Jordanian deformations) ← CYBE A lot of classical r-matrices [Kawaguchi-Matsumoto-KY, 1401.4855] i) Partial deformations are possible (i.e., only AdS5 or only S5 ) ii) Many r-matrices have been identified with solutions of type IIB SUGRA [Kawaguchi-Matsumoto-KY, 1402.6147] [Matsumoto-KY, 1404.1838, 1404.3657, 1412.3658, 1502.00740] 9 Jordanian deformation of the AdS5 x S5 superstring [Kawaguchi-Matsumoto-KY, 1401.4855] RJor satisfies CYBE. The undeformed limit: the Metsaev-Tseytlin action [Metsaev-Tseytlin, hep-th/9805028] • Lax pair is constructed classical integrability • Kappa invariance a consistency as string theory NOTE This is a generalization of the work of Delduc-Magro-Vicedo for mCYBE. The replacement: mCYBE → CYBE modifies Lax pair and kappa-transformation. 10 3 Examples: i) 3-parameter gamma-deformations of S5 [Matsumoto-KY, 1404.1838] Abelian r-matrix: Metric: B-field: [Lunin-Maldacena, Frolov, 2005] A special case: Lunin-Maldacena background Identification of parameters: 11 ii) Gravity duals for SYM on non-commutative space [Matsumoto-KY, 1404.3657] Abelian Jordanian r-matrix: where , , [Hashimoto-Itzhaki, Maldacena-Russo, 1999] Metric: B-field: Identification of parameters: Note: This background can be reproduced as a special limit of -deformed AdS5 [Arutyunov-Borsaro-Frolov, 1507.04239] [Kameyama-Kyono-Sakamoto-KY, 1509.00173] 12 iii) Schrödinger spacetimes [Matsumoto-KY, 1502.00740] Mixed r-matrix: Metric: [Herzog-Rangamani-Ross, 0807.1099] [Maldacena-Martelli-Tachikawa, 0807.1100] B-field: [Adams-Balasubramanian-McGreevy, 0807.1111] S5 -coordinates: NOTE: Classical r-matrix for 3-parameter cases [Bobev-Kundu, 0904.2873] Classical r-matrix for general Melvin twists [Bobev-Kundu-Pilch, 0905.0673] 13 Other examples: NC deformations of global AdS5 [McLaughlin-Swanson, hep-th/0605018] [Dhokarh-Haque-Hashimoto, 0801.3812] AdS pp-wave background [Hubeby-Rangamani-Ross, hep-th/0504034] Schrödinger AdS pp-wave [Kawaguchi-Matsumoto-KY, 1402.6147] [Matsumoto-KY, 1412.3658] Dipole backgrounds [Bergman-Dasgupta-Ganor-Karzmarek-Rajesh, hep-th/0103090] Remarks 1) Solutions can also be derived as TsT transformations of AdS5 x S5. TsT trans. are well described by Yang-Baxter deformations. In fact, 3 examples presented here can be interpreted as the undeformed theory with twisted periodic b.c. c.f., Frolov, Alday-Arutyunov-Frolov, 2) [Kameyama-Kyono-Sakamoto-KY, 1509.00173] RR sector and dilaton have not been confirmed yet. Schrödinger spacetimes are good candidates. The dilaton is const. and the RR sector is the same as the usual AdS5 x S5 . 14 Summary Towards the gravity/CYBE correspondence EX Lunin-Maldacena-Frolov, Maldacena-Russo, Schrödinger spacetimes Need to make efforts for the RR-sector and dilaton Further generalizations 1) Application to non-integrable case: EX AdS5 x T1,1 : non-integrability & chaos [Basu-Pando Zayas, 1103.4107] [Asano-Kawai-Kyono-KY, 1505.07583] Yang-Baxter sigma models can capture deformations of T1,1 as well. [Crichigno-Matsumoto-KY, 1406.2249] 2) Yang-Baxter deformations of Minkowski spacetime: [Matsumoto-Orlando-Reffert-Sakamoto-KY, 1505.04553] Relation to kappa-Poincare algebras [Borowiec-Kyono-Lukierski-Sakamoto-KY, 1510.NNNNN] 15 The limitation of the gravity/CYBE correspondence? To what extent the correspondence can work? What is the mathematical origin of Yang-Baxter deformations? The associated deformations of N=4 super Yang-Mills theory? It is significant to study the fundamental aspect of Yang-Baxter deformations Thank you! 16 Back up 17 Question How prevalent is integrability in various kinds AdS/CFTs? NOTE: Integrable subsectors are ubiquitous. EX integrable subsectors in large N QCD in 4 D So we will concentrate on the full integrability below. There are various kinds of AdS/CFT Real (or complex) beta-deformations Gravity duals for NC gauge theories AdS5 x T1,1 [Klebanov-Witten] Klebanov-Strassler, AdS BH [Lunin-Maldacena, Frolov] [Hashimoto-Itzhaki, Maldacena-Russo] AdS5 x Yp,q [Gauntlett-Martelli-Sparks-Waldram] Maldacena-Nunez [Horowitz-Strominger] AdS solitons [Witten, Horowitz-Myers] AdS/NRCFT [Son,Balasubramanian-McGreevy, Kachru-Liu-Mulligan] q-deformation of AdS5xS5 [Delduc-Magro-Vicedo, Arutyunov-Borsato-Frolov] 18 A classification list (would not be complete) Integrable backgrounds Real beta-deformations [Frolov, hep-th/0503201] Gravity duals for NC gauge theories [Matsumoto-KY, 1403.2703] q-deformation of AdS5 x S5 [Delduc-Magro-Vicedo, 1309.5850, Arutyunov-Borsato-Frolov, 1312.3542] [Hubeny-Rangamani-Ross , hep-th/0504034] [Dhokarh-Haque-Hashimoto , 0801.3812] [Kawaguchi-Matsumoto-KY, 1401.4855] TsT transformatios of AdS5 Non-integrable backgrounds Complex beta-deformations AdS5 x T1,1 AdS BH [Giataganas-Pando Zayas-Zoubos, 1311.3241] [Basu-Pando Zayas, 1103.4107] [Pando Zayas-Terrero Escalante, 1007.0277] Klebanov-Strassler, Maldacena-Nunez AdS5 x Yp,q [Basu-Pando Zayas, 1105.2540] AdS solitons [Basu-Das-Ghosh, 1103.4101] [Basu-Das-Ghosh-Pando Zayas, 1201.5634] Schrödinger spacetime with [Giataganas-Sfetsos, 1403.2703] Lifshitz space (with hyper-scaling violation) [Giataganas-Sfetsos, 1403.2703] [Bai-Chen-Lee-Moon, 1406.5816] p-brane backgrounds [Stepanchuk-Tseytlin, 1211.3727] [Chervonyi-Lunin, 1311.1521] 19 A schematic picture (to see the gravity/CYBE correspondence) A classical r-matrix from CYBE A gravity solution of type IIB SUGRA correspondence substitute compare! rewrite the action & read off Deformed AdS5xS5 superstring action The metric (string frame) & NS-NS 2-form Note: The metric & NS-NS 2-form have successfully been obtained so far. However, further studies are necessary for the RR sector and dilaton, though the kappa-symmetry may ensure that they can be reproduced as well. 20 Jordanian deformation of the AdS5 x S5 superstring RJor satisfies CYBE. Maurer-Cartan 1-form Projection on the group manifold , Projection on the world-sheet 21 Yang-Baxter deformations of 4D Minkowski spacetime Exactly solvable Integrable Integrable? The results obtained so far support the integrability of YB-deformed action. 22