×

Deformation of \(d = 4\), \(\mathcal{N} \geq 5\) supergravities breaks nonlinear local supersymmetry. (English) Zbl 07716862

Summary: We study \(d = 4\), \(\mathcal{N} \geq 5\) supergravities and their deformation via candidate counterterms, with the purpose to absorb UV divergences. We generalize the earlier studies of deformation and twisted self-duality constraint to the case with unbroken local \(\mathcal{H}\)-symmetry in presence of fermions. We find that the deformed action breaks nonlinear local supersymmetry. We show that all known cases of enhanced UV divergence cancellations are explained by nonlinear local supersymmetry.
This result implies, in particular, that if \(\mathcal{N} = 5\) supergravity at five loop will turn out to be UV divergent, the deformed theory will be BRST inconsistent. If it will be finite, it will be a consequence of nonlinear local supersymmetry and E7-type duality.

MSC:

83E50 Supergravity
81T60 Supersymmetric field theories in quantum mechanics
83C45 Quantization of the gravitational field
81T30 String and superstring theories; other extended objects (e.g., branes) in quantum field theory
81T50 Anomalies in quantum field theory

References:

[1] Kallosh, RE, The renormalization in non-Abelian gauge theories, Nucl. Phys. B, 78, 293 (1974) · doi:10.1016/0550-3213(74)90284-3
[2] M.H. Goroff and A. Sagnotti, The ultraviolet behavior of Einstein gravity, Nucl. Phys. B266 (1986) 709 [INSPIRE].
[3] Gibbons, GW; Hawking, SW; Perry, MJ, Path integrals and the indefiniteness of the gravitational action, Nucl. Phys. B, 138, 141 (1978) · doi:10.1016/0550-3213(78)90161-X
[4] S. Abreu et al., Two-loop four-graviton scattering amplitudes, Phys. Rev. Lett.124 (2020) 211601 [arXiv:2002.12374] [INSPIRE].
[5] Becchi, C.; Rouet, A.; Stora, R., Renormalization of gauge theories, Annals Phys., 98, 287 (1976) · doi:10.1016/0003-4916(76)90156-1
[6] I.V. Tyutin, Gauge invariance in field theory and statistical physics in operator formalism, arXiv:0812.0580 [INSPIRE].
[7] Cremmer, E.; Julia, B., The SO(8) supergravity, Nucl. Phys. B, 159, 141 (1979) · doi:10.1016/0550-3213(79)90331-6
[8] B. de Wit and H. Nicolai, N = 8 supergravity, Nucl. Phys. B208 (1982) 323 [INSPIRE].
[9] Kallosh, RE, Counterterms in extended supergravities, Phys. Lett. B, 99, 122 (1981) · doi:10.1016/0370-2693(81)90964-3
[10] Howe, PS; Lindstrom, U., Higher order invariants in extended supergravity, Nucl. Phys. B, 181, 487 (1981) · doi:10.1016/0550-3213(81)90537-X
[11] Brink, L.; Howe, PS, The N = 8 supergravity in superspace, Phys. Lett. B, 88, 268 (1979) · doi:10.1016/0370-2693(79)90464-7
[12] Howe, PS, Supergravity in superspace, Nucl. Phys. B, 199, 309 (1982) · doi:10.1016/0550-3213(82)90349-2
[13] Brink, L.; Kim, S-S; Ramond, P., E_7(7)on the light cone, JHEP, 06, 034 (2008) · doi:10.1088/1126-6708/2008/06/034
[14] R. Kallosh, N = 8 supergravity on the light cone, Phys. Rev. D80 (2009) 105022 [arXiv:0903.4630] [INSPIRE]. · Zbl 1171.83007
[15] Kallosh, R., The ultraviolet finiteness of N = 8 supergravity, JHEP, 12, 009 (2010) · Zbl 1294.83026 · doi:10.1007/JHEP12(2010)009
[16] Kallosh, R.; Ortin, T., New E_7(7)invariants and amplitudes, JHEP, 09, 137 (2012) · Zbl 1397.83040 · doi:10.1007/JHEP09(2012)137
[17] M. Gunaydin and R. Kallosh, Obstruction to E_7(7)deformation in N = 8 supergravity, arXiv:1303.3540 [INSPIRE].
[18] Kallosh, R., The action with manifest E_7type symmetry, JHEP, 05, 109 (2019) · doi:10.1007/JHEP05(2019)109
[19] Gunaydin, M.; Kallosh, R., Supersymmetry constraints on U-duality invariant deformations of N ≥ 5 supergravity, JHEP, 09, 105 (2019) · Zbl 1423.83092 · doi:10.1007/JHEP09(2019)105
[20] Kallosh, R.; Soroush, M., Explicit action of E_7(7)on N = 8 supergravity fields, Nucl. Phys. B, 801, 25 (2008) · Zbl 1189.83089 · doi:10.1016/j.nuclphysb.2008.04.006
[21] Z. Bern et al., Supergravity amplitudes, the double copy and ultraviolet behavior, arXiv:2304.07392 [INSPIRE].
[22] R. Kallosh, Is d = 4 maximal supergravity special?, arXiv:2304.13926 [INSPIRE].
[23] Z. Bern, S. Davies and T. Dennen, Enhanced ultraviolet cancellations in N = 5 supergravity at four loops, Phys. Rev. D90 (2014) 105011 [arXiv:1409.3089] [INSPIRE].
[24] G. Bossard, P.S. Howe, K.S. Stelle and P. Vanhove, The vanishing volume of D = 4 superspace, Class. Quant. Grav.28 (2011) 215005 [arXiv:1105.6087] [INSPIRE]. · Zbl 1230.83091
[25] Hartwell, GG; Howe, PS, (N, p, q) harmonic superspace, Int. J. Mod. Phys. A, 10, 3901 (1995) · Zbl 1044.58500 · doi:10.1142/S0217751X95001820
[26] S. Ferrara, R. Kallosh and A. Van Proeyen, Conjecture on hidden superconformal symmetry of N = 4 supergravity, Phys. Rev. D87 (2013) 025004 [arXiv:1209.0418] [INSPIRE]. · Zbl 1342.83527
[27] 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
[28] H. Elvang and Y.-T. Huang, Scattering amplitudes, arXiv:1308.1697 [INSPIRE]. · Zbl 1332.81010
[29] Freedman, DZ, Absence of U(1) anomalous superamplitudes in N ≥ 5 supergravities, JHEP, 05, 067 (2017) · Zbl 1380.83285 · doi:10.1007/JHEP05(2017)067
[30] Elvang, H.; Freedman, DZ; Kiermaier, M., Solution to the Ward identities for superamplitudes, JHEP, 10, 103 (2010) · Zbl 1291.81243 · doi:10.1007/JHEP10(2010)103
[31] Ferrara, S.; Kallosh, R., Creation of matter in the universe and groups of type E_7, JHEP, 12, 096 (2011) · Zbl 1306.81408 · doi:10.1007/JHEP12(2011)096
[32] E. Cremmer, B. Julia, H. Lu and C.N. Pope, Dualization of dualities. 2. Twisted self-duality of doubled fields, and superdualities, Nucl. Phys. B535 (1998) 242 [hep-th/9806106] [INSPIRE]. · Zbl 1080.81598
[33] Gaillard, MK; Zumino, B., Duality rotations for interacting fields, Nucl. Phys. B, 193, 221 (1981) · doi:10.1016/0550-3213(81)90527-7
[34] Andrianopoli, L.; D’Auria, R.; Ferrara, S., U duality and central charges in various dimensions revisited, Int. J. Mod. Phys. A, 13, 431 (1998) · Zbl 0921.53052 · doi:10.1142/S0217751X98000196
[35] Hillmann, C., E_7(7)invariant Lagrangian of d = 4, N = 8 supergravity, JHEP, 04, 010 (2010) · Zbl 1272.83085 · doi:10.1007/JHEP04(2010)010
[36] Bossard, G.; Hillmann, C.; Nicolai, H., E_7(7)symmetry in perturbatively quantised N = 8 supergravity, JHEP, 12, 052 (2010) · Zbl 1294.81168 · doi:10.1007/JHEP12(2010)052
[37] Kallosh, R., E_7(7)symmetry and finiteness of N = 8 supergravity, JHEP, 03, 083 (2012) · Zbl 1309.81250 · doi:10.1007/JHEP03(2012)083
[38] Kallosh, R., N = 8 counterterms and E_7(7)current conservation, JHEP, 06, 073 (2011) · Zbl 1298.81351 · doi:10.1007/JHEP06(2011)073
[39] Bossard, G.; Nicolai, H., Counterterms vs. dualities, JHEP, 08, 074 (2011) · Zbl 1298.81249 · doi:10.1007/JHEP08(2011)074
[40] J.J.M. Carrasco, R. Kallosh and R. Roiban, Covariant procedures for perturbative non-linear deformation of duality-invariant theories, Phys. Rev. D85 (2012) 025007 [arXiv:1108.4390] [INSPIRE].
[41] P. Pasti, D. Sorokin and M. Tonin, Covariant actions for models with non-linear twisted self-duality, Phys. Rev. D86 (2012) 045013 [arXiv:1205.4243] [INSPIRE].
[42] Kallosh, R.; Nicolai, H.; Roiban, R.; Yamada, Y., On quantum compatibility of counterterm deformations and duality symmetries in N ≥ 5 supergravities, JHEP, 08, 091 (2018) · Zbl 1396.83064 · doi:10.1007/JHEP08(2018)091
[43] Broedel, J.; Dixon, LJ, R^4counterterm and E_7(7)symmetry in maximal supergravity, JHEP, 05, 003 (2010) · Zbl 1288.81131 · doi:10.1007/JHEP05(2010)003
[44] Elvang, H.; Freedman, DZ; Kiermaier, M., A simple approach to counterterms in N = 8 supergravity, JHEP, 11, 016 (2010) · Zbl 1294.83023 · doi:10.1007/JHEP11(2010)016
[45] Beisert, N., E_7(7)constraints on counterterms in N = 8 supergravity, Phys. Lett. B, 694, 265 (2011) · doi:10.1016/j.physletb.2010.09.069
[46] Freedman, DZ; Tonni, E., The D^2kR^4invariants of N = 8 supergravity, JHEP, 04, 006 (2011) · Zbl 1250.83056 · doi:10.1007/JHEP04(2011)006
[47] Freedman, DZ; Kallosh, R.; Yamada, Y., Duality constraints on counterterms in supergravities, Fortsch. Phys., 66, 1800054 (2018) · Zbl 1535.83142 · doi:10.1002/prop.201800054
[48] Bossard, G.; Howe, PS; Stelle, KS, The ultra-violet question in maximally supersymmetric field theories, Gen. Rel. Grav., 41, 919 (2009) · Zbl 1177.83004 · doi:10.1007/s10714-009-0775-0
[49] Bern, Z., On the relationship between Yang-Mills theory and gravity and its implication for ultraviolet divergences, Nucl. Phys. B, 530, 401 (1998) · doi:10.1016/S0550-3213(98)00420-9
[50] Z. Bern, S. Davies, T. Dennen and Y.-T. Huang, Absence of three-loop four-point divergences in N = 4 supergravity, Phys. Rev. Lett.108 (2012) 201301 [arXiv:1202.3423] [INSPIRE].
[51] Carrasco, JJM; Kallosh, R.; Roiban, R.; Tseytlin, AA, On the U(1) duality anomaly and the S-matrix of N = 4 supergravity, JHEP, 07, 029 (2013) · Zbl 1342.83454 · doi:10.1007/JHEP07(2013)029
[52] Z. Bern et al., Ultraviolet properties of N = 4 supergravity at four loops, Phys. Rev. Lett.111 (2013) 231302 [arXiv:1309.2498] [INSPIRE].
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.