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Dark dimension and the grand unification of forces

Jonathan J. Heckman1,2,*, Cumrun Vafa3,†, Timo Weigand4,‡, and Fengjun Xu5,§

  • *jheckman@sas.upenn.edu
  • vafa@g.harvard.edu
  • timo.weigand@desy.de
  • §xufengjun321@gmail.com

Phys. Rev. D 111, 046014 – Published 10 February, 2025

DOI: https://doi.org/10.1103/PhysRevD.111.046014

Abstract

The dark dimension scenario, predicting one extra mesoscopic dimension in the micron range, has emerged by applying various swampland principles to the dark energy. In this note we find that realizing the grand unification of gauge forces is highly constraining in this context. Without actually constructing any grand unified theory (GUT) models, we argue that the mere assumption of grand unification of forces in this scenario, together with the experimental bounds on massive replicas of the Standard Model gauge bosons, predicts an upper bound for the GUT scale, MGUT1016GeV. Combined with the experimental bound on the proton lifetime, this predicts that the X gauge boson mediating proton decay is a 5D solitonic string of Planckian tension stretched across a length scale L(110TeV)1 ending on gauge branes of the same diameter L. This leads to a mass of MX10151016GeV. In particular assuming grand unification in the dark dimension scenario results in a tower of Kaluza-Klein excitations of Standard Model gauge bosons on the gauge branes in the 1–10 TeV range. This suggests that the diameter/separation L of the gauge branes correlates with both the weak scale 1/L near a TeV and the GUT scale M52L at 1016GeV.

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References (57)

  1. M. Montero, C. Vafa, and I. Valenzuela, The dark dimension and the Swampland, J. High Energy Phys. 02 (2023) 022.
  2. E. Gonzalo, M. Montero, G. Obied, and C. Vafa, Dark dimension gravitons as dark matter, J. High Energy Phys. 11 (2023) 109.
  3. J. A. P. Law-Smith, G. Obied, A. Prabhu, and C. Vafa, Astrophysical constraints on decaying dark gravitons, J. High Energy Phys. 06 (2024) 047.
  4. G. Obied, C. Dvorkin, E. Gonzalo, and C. Vafa, Dark dimension and decaying dark matter gravitons, Phys. Rev. D 109, 063540 (2024).
  5. N. Gendler and C. Vafa, Axions in the dark dimension, J. High Energy Phys. 12 (2024) 127.
  6. L. A. Anchordoqui, Dark dimension, the Swampland, and the origin of cosmic rays beyond the Greisen-Zatsepin-Kuzmin barrier, Phys. Rev. D 106, 116022 (2022).
  7. L. A. Anchordoqui, I. Antoniadis, and D. Lüst, Dark dimension, the swampland, and the dark matter fraction composed of primordial black holes, Phys. Rev. D 106, 086001 (2022).
  8. R. Blumenhagen, M. Brinkmann, and A. Makridou, The dark dimension in a warped throat, Phys. Lett. B 838, 137699 (2023).
  9. L. A. Anchordoqui, I. Antoniadis, and D. Lüst, The dark universe: Primordial black hole dark graviton gas connection, Phys. Lett. B 840, 137844 (2023).
  10. L. A. Anchordoqui, I. Antoniadis, and D. Lüst, Aspects of the dark dimension in cosmology, Phys. Rev. D 107, 083530 (2023).
  11. L. A. Anchordoqui, I. Antoniadis, N. Cribiori, D. Lust, and M. Scalisi, The scale of supersymmetry breaking and the dark dimension, J. High Energy Phys. 05 (2023) 060.
  12. N. T. Noble, J. F. Soriano, and L. A. Anchordoqui, Probing the dark dimension with Auger data, Phys. Dark Universe 42, 101278 (2023).
  13. L. A. Anchordoqui, I. Antoniadis, and J. Cunat, Dark dimension and the standard model landscape, Phys. Rev. D 109, 016028 (2024).
  14. L. A. Anchordoqui, I. Antoniadis, and D. Lüst, Fuzzy dark matter and the dark dimension, Eur. Phys. J. C 84, 273 (2024).
  15. C. Cui and S. Ning, Casimir energy stabilization of standard model landscape in dark dimension, arXiv:2310.19592.
  16. L. A. Anchordoqui and I. Antoniadis, Large extra dimensions from higher-dimensional inflation, Phys. Rev. D 109, 103508 (2024).
  17. L. A. Anchordoqui, I. Antoniadis, and D. Lüst, Dark dimension, the Swampland, and the dark matter fraction composed of primordial near-extremal black holes, Phys. Rev. D 109, 095008 (2024).
  18. J. H. Schwarz, Comments concerning a hypothetical mesoscopic dark dimension, arXiv:2403.12899.
  19. L. A. Anchordoqui, I. Antoniadis, D. Lust, N. T. Noble, and J. F. Soriano, From infinite to infinitesimal: Using the universe as a dataset to probe Casimir corrections to the vacuum energy from fields inhabiting the dark dimension, Phys. Dark Universe 46, 101715 (2024).
  20. G. F. Casas, L. E. Ibáñez, and F. Marchesano, On small Dirac neutrino masses in string theory, arXiv:2406.14609.
  21. C. Vafa, Swamplandish unification of the dark sector, arXiv:2402.00981.
  22. I. Antoniadis, L. A. Anchordoqui, and D. Lüst, Landscape, Swampland and extra dimensions, Proc. Sci. CORFU2023 (2024) 215 [arXiv:2405.04427].
  23. L. E. Ibáñez and A. M. Uranga, String Theory and Particle Physics: An Introduction to String Phenomenology (Cambridge University Press, Cambridge, England, 2012).
  24. F. Marchesano, G. Shiu, and T. Weigand, The standard model from string theory: What have we learned?, Annu. Rev. Nucl. Part. Sci. 74, 113 (2024).
  25. H. Ooguri and C. Vafa, On the geometry of the string landscape and the Swampland, Nucl. Phys. B766, 21 (2007).
  26. D. Lüst, E. Palti, and C. Vafa, AdS and the Swampland, Phys. Lett. B 797, 134867 (2019).
  27. S.-J. Lee, W. Lerche, and T. Weigand, Emergent strings from infinite distance limits, J. High Energy Phys. 02 (2022) 190.
  28. ATLAS Collaboration, Search for new high-mass phenomena in the dilepton final state using 36fb1 of proton-proton collision data at s=13TeV with the ATLAS detector, J. High Energy Phys. 10 (2017) 182.
  29. CMS Collaboration, Search for resonant and nonresonant new phenomena in high-mass dilepton final states at s=13TeV, J. High Energy Phys. 07 (2021) 208.
  30. Particle Data Group Collaboration, Review of particle physics, Prog. Theor. Exp. Phys. 2022, 083C01 (2022).
  31. S. L. Glashow, J. Iliopoulos, and L. Maiani, Weak interactions with lepton-hadron symmetry, Phys. Rev. D 2, 1285 (1970).
  32. L. Maiani, The GIM mechanism: Origin, predictions and recent uses, in 48th Rencontres de Moriond on Electroweak Interactions and Unified Theories (2013), pp. 3–16, arXiv:1303.6154.
  33. R. Donagi and M. Wijnholt, Model building with F-theory, Adv. Theor. Math. Phys. 15, 1237 (2011).
  34. C. Beasley, J. J. Heckman, and C. Vafa, GUTs and exceptional branes in F-theory—I, J. High Energy Phys. 01 (2009) 058.
  35. C. Beasley, J. J. Heckman, and C. Vafa, GUTs and exceptional branes in F-theory—II: Experimental predictions, J. High Energy Phys. 01 (2009) 059.
  36. H. Georgi and S. L. Glashow, Unity of all elementary particle forces, Phys. Rev. Lett. 32, 438 (1974).
  37. H. Fritzsch and P. Minkowski, Unified interactions of leptons and hadrons, Ann. Phys. (N.Y.) 93, 193 (1975).
  38. H. Georgi, Unified gauge theories, Stud. Nat. Sci. 9, 329 (1975).
  39. P. Candelas, G. T. Horowitz, A. Strominger, and E. Witten, Vacuum configurations for superstrings, Nucl. Phys. B258, 46 (1985).
  40. E. Witten, New issues in manifolds of SU(3) holonomy, Nucl. Phys. B268, 79 (1986).
  41. B. S. Acharya and E. Witten, Chiral fermions from manifolds of G(2) holonomy, arXiv:hep-th/0109152.
  42. L. J. Hall, Y. Nomura, T. Okui, and D. Tucker-Smith, SO(10) unified theories in six-dimensions, Phys. Rev. D 65, 035008 (2002).
  43. L. J. Hall and Y. Nomura, Gauge coupling unification from unified theories in higher dimensions, Phys. Rev. D 65, 125012 (2002).
  44. H. D. Kim and S. Raby, Unification in 5D SO(10), J. High Energy Phys. 01 (2003) 056.
  45. J. J. Heckman, A. Tavanfar, and C. Vafa, The point of E8 in F-theory GUTs, J. High Energy Phys. 08 (2010) 040.
  46. Super-Kamiokande Collaboration, Search for proton decay via pe+π0 and pμ+π0 with an enlarged fiducial volume in Super-Kamiokande I-IV, Phys. Rev. D 102, 112011 (2020).
  47. T. Ohlsson, Proton decay, Nucl. Phys. B993, 116268 (2023).
  48. A. Bedroya, C. Vafa, and D. H. Wu, The tale of three scales: The Planck, the species, and the black hole scales, arXiv:2403.18005.
  49. N. S. Manton, A new six-dimensional approach to the Weinberg-Salam model, Nucl. Phys. B158, 141 (1979).
  50. Y. Hosotani, Dynamical mass generation by compact extra dimensions, Phys. Lett. 126B, 309 (1983).
  51. N. Arkani-Hamed, A. G. Cohen, and H. Georgi, Electroweak symmetry breaking from dimensional deconstruction, Phys. Lett. B 513, 232 (2001).
  52. N. Haba, K. Takenaga, and T. Yamashita, Higgs mass in the gauge-Higgs unification, Phys. Lett. B 615, 247 (2005).
  53. R. Blumenhagen, L. Goerlich, B. Kors, and D. Lüst, Noncommutative compactifications of type I strings on tori with magnetic background flux, J. High Energy Phys. 10 (2000) 006.
  54. M. Cvetič, G. Shiu, and A. M. Uranga, Chiral four-dimensional N=1 supersymmetric type 2A orientifolds from intersecting D6 branes, Nucl. Phys. B615, 3 (2001).
  55. CDF Collaboration, High-precision measurement of the W boson mass with the CDF II detector, Science 376, 170 (2022).
  56. A. Strumia, Interpreting electroweak precision data including the W-mass CDF anomaly, J. High Energy Phys. 08 (2022) 248.
  57. M. Endo and S. Mishima, New physics interpretation of W-boson mass anomaly, Phys. Rev. D 106, 115005 (2022).

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