×

Exploring Reggeon bound states in strongly-coupled \(\mathcal{N} = 4\) super Yang-Mills. (English) Zbl 1521.81365

Summary: The multi-Regge limit of scattering amplitudes in strongly-coupled \(\mathcal{N} = 4\) super Yang-Mills is described by the large mass limit of a set of thermodynamic Bethe ansatz (TBA) equations. A non-trivial remainder function arises in this setup in certain kinematical regions due to excitations of the TBA equations which appear during the analytic continuation into these kinematical regions. So far, these analytic continuations were carried out on a case-by-case basis for the six- and seven-gluon remainder function. In this note, we show that the set of possible excitations appearing in any analytic continuation in the multi-Regge limit for any number of particles is rather constrained. In particular, we show that the BFKL eigenvalue of any possible Reggeon bound state is a multiple of the two-Reggeon BFKL eigenvalue appearing in the six-gluon case.

MSC:

81T60 Supersymmetric field theories in quantum mechanics
83C27 Lattice gravity, Regge calculus and other discrete methods in general relativity and gravitational theory
83C30 Asymptotic procedures (radiation, news functions, \(\mathcal{H} \)-spaces, etc.) in general relativity and gravitational theory
81T35 Correspondence, duality, holography (AdS/CFT, gauge/gravity, etc.)
81T13 Yang-Mills and other gauge theories in quantum field theory
81T40 Two-dimensional field theories, conformal field theories, etc. in quantum mechanics
81U05 \(2\)-body potential quantum scattering theory
81R12 Groups and algebras in quantum theory and relations with integrable systems

References:

[1] Z. Bern, L.J. Dixon and V.A. Smirnov, Iteration of planar amplitudes in maximally supersymmetric Yang-Mills theory at three loops and beyond, Phys. Rev. D72 (2005) 085001 [hep-th/0505205] [INSPIRE].
[2] Del Duca, V.; Duhr, C.; Smirnov, VA, The Two-Loop Hexagon Wilson Loop in N = 4 SYM, JHEP, 05, 084 (2010) · Zbl 1287.81080 · doi:10.1007/JHEP05(2010)084
[3] Dixon, LJ; Drummond, JM; Henn, JM, Bootstrapping the three-loop hexagon, JHEP, 11, 023 (2011) · Zbl 1306.81092 · doi:10.1007/JHEP11(2011)023
[4] Caron-Huot, S.; He, S., Jumpstarting the All-Loop S-matrix of Planar N = 4 Super Yang-Mills, JHEP, 07, 174 (2012) · Zbl 1397.81347 · doi:10.1007/JHEP07(2012)174
[5] Dixon, LJ; Drummond, JM; Henn, JM, Analytic result for the two-loop six-point NMHV amplitude in N = 4 super Yang-Mills theory, JHEP, 01, 024 (2012) · Zbl 1306.81093 · doi:10.1007/JHEP01(2012)024
[6] Dixon, LJ; Drummond, JM; von Hippel, M.; Pennington, J., Hexagon functions and the three-loop remainder function, JHEP, 12, 049 (2013) · Zbl 1342.81159 · doi:10.1007/JHEP12(2013)049
[7] Dixon, LJ; Drummond, JM; Duhr, C.; Pennington, J., The four-loop remainder function and multi-Regge behavior at NNLLA in planar N = 4 super-Yang-Mills theory, JHEP, 06, 116 (2014) · Zbl 1333.81238 · doi:10.1007/JHEP06(2014)116
[8] Dixon, LJ; von Hippel, M., Bootstrapping an NMHV amplitude through three loops, JHEP, 10, 065 (2014) · doi:10.1007/JHEP10(2014)065
[9] Drummond, JM; Papathanasiou, G.; Spradlin, M., A Symbol of Uniqueness: The Cluster Bootstrap for the 3-Loop MHV Heptagon, JHEP, 03, 072 (2015) · doi:10.1007/JHEP03(2015)072
[10] Dixon, LJ; von Hippel, M.; McLeod, AJ, The four-loop six-gluon NMHV ratio function, JHEP, 01, 053 (2016) · doi:10.1007/JHEP01(2016)053
[11] S. Caron-Huot, L.J. Dixon, A. McLeod and M. von Hippel, Bootstrapping a Five-Loop Amplitude Using Steinmann Relations, Phys. Rev. Lett.117 (2016) 241601 [arXiv:1609.00669] [INSPIRE].
[12] Dixon, LJ; Drummond, J.; Harrington, T.; McLeod, AJ; Papathanasiou, G.; Spradlin, M., Heptagons from the Steinmann Cluster Bootstrap, JHEP, 02, 137 (2017) · Zbl 1377.81197 · doi:10.1007/JHEP02(2017)137
[13] Drummond, J.; Foster, J.; Gürdoğan, O.; Papathanasiou, G., Cluster adjacency and the four-loop NMHV heptagon, JHEP, 03, 087 (2019) · Zbl 1414.81251 · doi:10.1007/JHEP03(2019)087
[14] S. Caron-Huot, L.J. Dixon, F. Dulat, M. von Hippel, A.J. McLeod and G. Papathanasiou, Six-Gluon amplitudes in planar \(\mathcal{N} = 4\) super-Yang-Mills theory at six and seven loops, JHEP08 (2019) 016 [arXiv:1903.10890] [INSPIRE]. · Zbl 1421.81136
[15] S. Caron-Huot, L.J. Dixon, F. Dulat, M. Von Hippel, A.J. McLeod and G. Papathanasiou, The Cosmic Galois Group and Extended Steinmann Relations for Planar \(\mathcal{N} = 4\) SYM Amplitudes, JHEP09 (2019) 061 [arXiv:1906.07116] [INSPIRE].
[16] Dixon, LJ; Liu, Y-T, Lifting Heptagon Symbols to Functions, JHEP, 10, 031 (2020) · Zbl 1456.81428 · doi:10.1007/JHEP10(2020)031
[17] Caron-Huot, S., Superconformal symmetry and two-loop amplitudes in planar N = 4 super Yang-Mills, JHEP, 12, 066 (2011) · Zbl 1306.81082 · doi:10.1007/JHEP12(2011)066
[18] S. He, Z. Li and C. Zhang, Two-loop octagons, algebraic letters and \(\overline{Q}\) equations, Phys. Rev. D101 (2020) 061701 [arXiv:1911.01290] [INSPIRE].
[19] He, S.; Li, Z.; Zhang, C., The symbol and alphabet of two-loop NMHV amplitudes from \(\overline{Q}\) equations, JHEP, 03, 278 (2021) · doi:10.1007/JHEP03(2021)278
[20] Golden, J.; McLeod, AJ, The two-loop remainder function for eight and nine particles, JHEP, 06, 142 (2021) · doi:10.1007/JHEP06(2021)142
[21] L.N. Lipatov, Reggeization of the Vector Meson and the Vacuum Singularity in NonAbelian Gauge Theories, Sov. J. Nucl. Phys.23 (1976) 338 [Yad. Fiz.23 (1976) 642] [INSPIRE].
[22] Fadin, VS; Kuraev, EA; Lipatov, LN, On the Pomeranchuk Singularity in Asymptotically Free Theories, Phys. Lett. B, 60, 50 (1975) · doi:10.1016/0370-2693(75)90524-9
[23] E.A. Kuraev, L.N. Lipatov and V.S. Fadin, Multi-Reggeon Processes in the Yang-Mills Theory, Sov. Phys. JETP44 (1976) 443 [Zh. Eksp. Teor. Fiz.71 (1976) 840] [INSPIRE].
[24] Balitsky, II; Lipatov, LN, The Pomeranchuk Singularity in Quantum Chromodynamics, Sov. J. Nucl. Phys., 28, 822 [INSPIRE] (1978)
[25] J. Bartels, L.N. Lipatov and A. Sabio Vera, BFKL Pomeron, Reggeized gluons and Bern-Dixon-Smirnov amplitudes, Phys. Rev. D80 (2009) 045002 [arXiv:0802.2065] [INSPIRE].
[26] J. Bartels, L.N. Lipatov and A. Sabio Vera, N = 4 supersymmetric Yang-Mills scattering amplitudes at high energies: The Regge cut contribution, Eur. Phys. J. C65 (2010) 587 [arXiv:0807.0894] [INSPIRE].
[27] L.N. Lipatov and A. Prygarin, BFKL approach and six-particle MHV amplitude in N = 4 super Yang-Mills, Phys. Rev. D83 (2011) 125001 [arXiv:1011.2673] [INSPIRE].
[28] Fadin, VS; Lipatov, LN, BFKL equation for the adjoint representation of the gauge group in the next-to-leading approximation at N = 4 SUSY, Phys. Lett. B, 706, 470 (2012) · doi:10.1016/j.physletb.2011.11.048
[29] Dixon, LJ; Duhr, C.; Pennington, J., Single-valued harmonic polylogarithms and the multi-Regge limit, JHEP, 10, 074 (2012) · doi:10.1007/JHEP10(2012)074
[30] Bartels, J.; Kotanski, J.; Schomerus, V., Excited Hexagon Wilson Loops for Strongly Coupled N = 4 SYM, JHEP, 01, 096 (2011) · Zbl 1214.81290 · doi:10.1007/JHEP01(2011)096
[31] J. Bartels, J. Kotanski, V. Schomerus and M. Sprenger, The Excited Hexagon Reloaded, arXiv:1311.1512 [INSPIRE].
[32] Basso, B.; Caron-Huot, S.; Sever, A., Adjoint BFKL at finite coupling: a short-cut from the collinear limit, JHEP, 01, 027 (2015) · doi:10.1007/JHEP01(2015)027
[33] J. Bartels, A. Kormilitzin, L.N. Lipatov and A. Prygarin, BFKL approach and 2 → 5 maximally helicity violating amplitude in \(\mathcal{N} = 4\) super-Yang-Mills theory, Phys. Rev. D86 (2012) 065026 [arXiv:1112.6366] [INSPIRE].
[34] J. Bartels, A. Kormilitzin and L. Lipatov, Analytic structure of the N = 7 scattering amplitude in \(\mathcal{N} = 4\) SYM theory in the multi-Regge kinematics: Conformal Regge pole contribution, Phys. Rev. D89 (2014) 065002 [arXiv:1311.2061] [INSPIRE].
[35] J. Bartels, A. Kormilitzin and L.N. Lipatov, Analytic structure of the N = 7 scattering amplitude in \(\mathcal{N} = 4\) theory in multi-Regge kinematics: Conformal Regge cut contribution, Phys. Rev. D91 (2015) 045005 [arXiv:1411.2294] [INSPIRE].
[36] Del Duca, V., The seven-gluon amplitude in multi-Regge kinematics beyond leading logarithmic accuracy, JHEP, 06, 116 (2018) · Zbl 1395.81160 · doi:10.1007/JHEP06(2018)116
[37] Bartels, J.; Schomerus, V.; Sprenger, M., Heptagon Amplitude in the Multi-Regge Regime, JHEP, 10, 067 (2014) · Zbl 1392.81217 · doi:10.1007/JHEP10(2014)067
[38] J. Bartels, V. Schomerus and M. Sprenger, The Bethe roots of Regge cuts in strongly coupled \(\mathcal{N} = 4\) SYM theory, JHEP07 (2015) 098 [arXiv:1411.2594] [INSPIRE]. · Zbl 1388.81907
[39] M. Sprenger, Regge meets collinear in strongly-coupled \(\mathcal{N} = 4\) super Yang-Mills, JHEP01 (2017) 035 [arXiv:1610.07640] [INSPIRE]. · Zbl 1373.81339
[40] V. Del Duca et al., All-order amplitudes at any multiplicity in the multi-Regge limit, Phys. Rev. Lett.124 (2020) 161602 [arXiv:1912.00188] [INSPIRE].
[41] L.N. Lipatov, Integrability of scattering amplitudes in N = 4 SUSY, J. Phys. A42 (2009) 304020 [arXiv:0902.1444] [INSPIRE]. · Zbl 1176.81062
[42] J. Bartels, L.N. Lipatov and A. Prygarin, Integrable spin chains and scattering amplitudes, J. Phys. A44 (2011) 454013 [arXiv:1104.0816] [INSPIRE]. · Zbl 1270.81131
[43] Del Duca, V.; Duhr, C.; Dulat, F.; Penante, B., All two-loop MHV remainder functions in multi-Regge kinematics, JHEP, 01, 162 (2019) · Zbl 1409.81145 · doi:10.1007/JHEP01(2019)162
[44] J. Bartels, Analytic structure of the 8-point scattering amplitude in multi-Regge kinematics in N = 4 SYM: conformal Regge pole and Regge cut contributions, arXiv:2005.08818 [INSPIRE].
[45] Alday, LF; Gaiotto, D.; Maldacena, JM; Sever, A.; Vieira, P., An Operator Product Expansion for Polygonal null Wilson Loops, JHEP, 04, 088 (2011) · Zbl 1250.81071 · doi:10.1007/JHEP04(2011)088
[46] Gaiotto, D.; Maldacena, JM; Sever, A.; Vieira, P., Bootstrapping Null Polygon Wilson Loops, JHEP, 03, 092 (2011) · Zbl 1301.81125 · doi:10.1007/JHEP03(2011)092
[47] Gaiotto, D.; Maldacena, JM; Sever, A.; Vieira, P., Pulling the straps of polygons, JHEP, 12, 011 (2011) · Zbl 1306.81153 · doi:10.1007/JHEP12(2011)011
[48] Sever, A.; Vieira, P.; Wang, T., OPE for Super Loops, JHEP, 11, 051 (2011) · Zbl 1306.81362 · doi:10.1007/JHEP11(2011)051
[49] B. Basso, A. Sever and P. Vieira, Spacetime and Flux Tube S-Matrices at Finite Coupling for N = 4 Supersymmetric Yang-Mills Theory, Phys. Rev. Lett.111 (2013) 091602 [arXiv:1303.1396] [INSPIRE].
[50] B. Basso, A. Sever and P. Vieira, Hexagonal Wilson loops in planar \(\mathcal{N} = 4\) SYM theory at finite coupling, J. Phys. A49 (2016) 41LT01 [arXiv:1508.03045] [INSPIRE]. · Zbl 1349.81170
[51] Basso, B., Exciting the GKP string at any coupling, Nucl. Phys. B, 857, 254 (2012) · Zbl 1246.81206 · doi:10.1016/j.nuclphysb.2011.12.010
[52] B. Basso, A. Sever and P. Vieira, Space-time S-matrix and Flux tube S-matrix II. Extracting and Matching Data, JHEP01 (2014) 008 [arXiv:1306.2058] [INSPIRE].
[53] Belitsky, AV; Derkachov, SE; Manashov, AN, Quantum mechanics of null polygonal Wilson loops, Nucl. Phys. B, 882, 303 (2014) · Zbl 1285.81047 · doi:10.1016/j.nuclphysb.2014.03.007
[54] B. Basso, A. Sever and P. Vieira, Space-time S-matrix and Flux-tube S-matrix III. The two-particle contributions, JHEP08 (2014) 085 [arXiv:1402.3307] [INSPIRE].
[55] B. Basso, A. Sever and P. Vieira, Space-time S-matrix and Flux-tube S-matrix IV. Gluons and Fusion, JHEP09 (2014) 149 [arXiv:1407.1736] [INSPIRE].
[56] Belitsky, AV, Nonsinglet pentagons and NMHV amplitudes, Nucl. Phys. B, 896, 493 (2015) · Zbl 1331.81283 · doi:10.1016/j.nuclphysb.2015.05.002
[57] Belitsky, AV, Fermionic pentagons and NMHV hexagon, Nucl. Phys. B, 894, 108 (2015) · Zbl 1328.81156 · doi:10.1016/j.nuclphysb.2015.02.025
[58] Basso, B.; Caetano, J.; Cordova, L.; Sever, A.; Vieira, P., OPE for all Helicity Amplitudes, JHEP, 08, 018 (2015) · Zbl 1388.81277 · doi:10.1007/JHEP08(2015)018
[59] Belitsky, AV, On factorization of multiparticle pentagons, Nucl. Phys. B, 897, 346 (2015) · Zbl 1329.81263 · doi:10.1016/j.nuclphysb.2015.05.024
[60] B. Basso, J. Caetano, L. Cordova, A. Sever and P. Vieira, OPE for all Helicity Amplitudes II. Form Factors and Data Analysis, JHEP12 (2015) 088 [arXiv:1508.02987] [INSPIRE]. · Zbl 1388.81278
[61] Drummond, JM; Papathanasiou, G., Hexagon OPE Resummation and Multi-Regge Kinematics, JHEP, 02, 185 (2016) · doi:10.1007/JHEP02(2016)185
[62] Fioravanti, D.; Piscaglia, S.; Rossi, M., Asymptotic Bethe Ansatz on the GKP vacuum as a defect spin chain: scattering, particles and minimal area Wilson loops, Nucl. Phys. B, 898, 301 (2015) · Zbl 1329.82024 · doi:10.1016/j.nuclphysb.2015.07.007
[63] Bonini, A.; Fioravanti, D.; Piscaglia, S.; Rossi, M., Strong Wilson polygons from the lodge of free and bound mesons, JHEP, 04, 029 (2016)
[64] Córdova, L., Hexagon POPE: effective particles and tree level resummation, JHEP, 01, 051 (2017) · Zbl 1373.81349 · doi:10.1007/JHEP01(2017)051
[65] Lam, HT; von Hippel, M., Resumming the POPE at One Loop, JHEP, 12, 011 (2016) · doi:10.1007/JHEP12(2016)011
[66] B. Basso, L.J. Dixon and G. Papathanasiou, Origin of the Six-Gluon Amplitude in Planar N = 4 Supersymmetric Yang-Mills Theory, Phys. Rev. Lett.124 (2020) 161603 [arXiv:2001.05460] [INSPIRE].
[67] Bartels, J.; Fadin, VS; Lipatov, LN; Vacca, GP, NLO Corrections to the kernel of the BKP-equations, Nucl. Phys. B, 867, 827 (2013) · Zbl 1262.81187 · doi:10.1016/j.nuclphysb.2012.10.024
[68] Bargheer, T.; Papathanasiou, G.; Schomerus, V., The Two-Loop Symbol of all Multi-Regge Regions, JHEP, 05, 012 (2016) · doi:10.1007/JHEP05(2016)012
[69] Bargheer, T.; Chestnov, V.; Schomerus, V., The Multi-Regge Limit from the Wilson Loop OPE, JHEP, 05, 002 (2020) · Zbl 1437.81087 · doi:10.1007/JHEP05(2020)002
[70] Alday, LF; Maldacena, JM, Gluon scattering amplitudes at strong coupling, JHEP, 06, 064 (2007) · doi:10.1088/1126-6708/2007/06/064
[71] Alday, LF; Maldacena, JM, Null polygonal Wilson loops and minimal surfaces in Anti-de-Sitter space, JHEP, 11, 082 (2009) · doi:10.1088/1126-6708/2009/11/082
[72] Alday, LF; Gaiotto, D.; Maldacena, JM, Thermodynamic Bubble Ansatz, JHEP, 09, 032 (2011) · Zbl 1301.81162 · doi:10.1007/JHEP09(2011)032
[73] L.F. Alday, J.M. Maldacena, A. Sever and P. Vieira, Y-system for Scattering Amplitudes, J. Phys. A43 (2010) 485401 [arXiv:1002.2459] [INSPIRE]. · Zbl 1204.81134
[74] Drummond, JM; Henn, J.; Korchemsky, GP; Sokatchev, E., Dual superconformal symmetry of scattering amplitudes in N = 4 super-Yang-Mills theory, Nucl. Phys. B, 828, 317 (2010) · Zbl 1203.81112 · doi:10.1016/j.nuclphysb.2009.11.022
[75] Yang, G., Scattering amplitudes at strong coupling for 4K gluons, JHEP, 12, 082 (2010) · Zbl 1294.81297 · doi:10.1007/JHEP12(2010)082
[76] Yang, G., A simple collinear limit of scattering amplitudes at strong coupling, JHEP, 03, 087 (2011) · Zbl 1301.81315 · doi:10.1007/JHEP03(2011)087
[77] Bartels, J.; Schomerus, V.; Sprenger, M., Multi-Regge Limit of the n-Gluon Bubble Ansatz, JHEP, 11, 145 (2012) · doi:10.1007/JHEP11(2012)145
[78] Eden, B.; Heslop, P.; Korchemsky, GP; Sokatchev, E., Constructing the correlation function of four stress-tensor multiplets and the four-particle amplitude in N = 4 SYM, Nucl. Phys. B, 862, 450 (2012) · Zbl 1246.81363 · doi:10.1016/j.nuclphysb.2012.04.013
[79] Dorey, P.; Tateo, R., Excited states by analytic continuation of TBA equations, Nucl. Phys. B, 482, 639 (1996) · Zbl 0925.82044 · doi:10.1016/S0550-3213(96)00516-0
[80] Dorey, P.; Tateo, R., Excited states in some simple perturbed conformal field theories, Nucl. Phys. B, 515, 575 (1998) · Zbl 0945.81055 · doi:10.1016/S0550-3213(97)00838-9
[81] Bargheer, T., Systematics of the Multi-Regge Three-Loop Symbol, JHEP, 11, 077 (2017) · Zbl 1383.81276 · doi:10.1007/JHEP11(2017)077
[82] Del Duca, V., Multi-Regge kinematics and the moduli space of Riemann spheres with marked points, JHEP, 08, 152 (2016) · Zbl 1390.81627 · doi:10.1007/JHEP08(2016)152
This reference list is based on information provided by the publisher or from digital mathematics libraries. Its items are heuristically matched to zbMATH identifiers and may contain data conversion errors. In some cases that data have been complemented/enhanced by data from zbMATH Open. This attempts to reflect the references listed in the original paper as accurately as possible without claiming completeness or a perfect matching.