Constraining neutrino masses, the cosmological constant and BSM physics from the weak gravity conjecture

被引:58
作者
Ibanez, Luis E. [1 ,2 ]
Martin-Lozano, Victor [3 ,4 ]
Valenzuela, Irene [5 ,6 ,7 ]
机构
[1] Univ Autonoma Madrid, Dept Fis Teor, E-28049 Madrid, Spain
[2] Univ Autonoma Madrid, Inst Fis Teor UAM CSIC, E-28049 Madrid, Spain
[3] Univ Bonn, Bethe Ctr Theoret Phys, Nussallee 12, D-53115 Bonn, Germany
[4] Univ Bonn, Phys Inst, Nussallee 12, D-53115 Bonn, Germany
[5] Max Planck Inst Phys & Astrophys, Fohringer Ring 6, D-80805 Munich, Germany
[6] Univ Utrecht, Inst Theoret Phys, Leuvenland 4, NL-3584 CE Utrecht, Netherlands
[7] Univ Utrecht, Ctr Extreme Matter & Emergent Phenomena, Leuvenland 4, NL-3584 CE Utrecht, Netherlands
关键词
Beyond Standard Model; Models of Quantum Gravity; Quark Masses and SM Parameters; Superstring Vacua; NEUTRALIZATION;
D O I
10.1007/JHEP11(2017)066
中图分类号
O412 [相对论、场论]; O572.2 [粒子物理学];
学科分类号
摘要
It is known that there are AdS vacua obtained from compactifying the SM to 2 or 3 dimensions. The existence of such vacua depends on the value of neutrino masses through the Casimir effect. Using the Weak Gravity Conjecture, it has been recently argued by Ooguri and Vafa that such vacua are incompatible with the SM embedding into a consistent theory of quantum gravity. We study the limits obtained for both the cosmological constant Lambda(4) and neutrino masses from the absence of such dangerous 3D and 2D SM AdS vacua. One interesting implication is that Lambda(4) is bounded to be larger than a scale of order m(nu)(4), as observed experimentally. Interestingly, this is the first argument implying a non-vanishing Lambda(4) only on the basis of particle physics, with no cosmological input. Conversely, the observed Lambda(4) implies strong constraints on neutrino masses in the SM and also for some BSM extensions including extra Weyl or Dirac spinors, gravitinos and axions. The upper bounds obtained for neutrino masses imply (for fixed neutrino Yukawa and Lambda(4)) the existence of upper bounds on the EW scale. In the case of massive Majorana neutrinos with a see-saw mechanism associated to a large scale M similar or equal to 10(10-14) GeV and Y-nu 1 similar or equal to 10(-3), one obtains that the EW scale cannot exceed M-EW less than or similar to 10(2) - 10(4) GeV. From this point of view, the delicate fine-tuning required to get a small EW scale would be a mirage, since parameters yielding higher EW scales would be in the swampland and would not count as possible consistent theories. This would bring a new perspective into the issue of the EW hierarchy.
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页数:40
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共 74 条
[1]  
Abazajian K.N., ARXIV12045379
[2]   Discovery probability of next-generation neutrinoless double-β decay experiments [J].
Agostini, Matteo ;
Benato, Giovanni ;
Detwiler, Jason A. .
PHYSICAL REVIEW D, 2017, 96 (05)
[3]  
[Anonymous], JHEP
[4]  
[Anonymous], JHEP
[5]  
[Anonymous], JHEP
[6]  
[Anonymous], JHEP
[7]   The string landscape, black holes and gravity as the weakest force [J].
Arkani-Hamed, Nima ;
Motl, Lubos ;
Nicolis, Alberto ;
Vafa, Cumrun .
JOURNAL OF HIGH ENERGY PHYSICS, 2007, (06)
[8]   Quantum Horizons of the standard model landscape [J].
Arkani-Hamed, Nima ;
Dubovsky, Sergei ;
Nicolis, Alberto ;
Villadoro, Giovanni .
JOURNAL OF HIGH ENERGY PHYSICS, 2007, (06)
[9]   Standard model vacua for two-dimensional compactifications [J].
Arnold, Jonathan M. ;
Fornal, Bartosz ;
Wise, Mark B. .
JOURNAL OF HIGH ENERGY PHYSICS, 2010, (12)
[10]   String axiverse [J].
Arvanitaki, Asimina ;
Dimopoulos, Savas ;
Dubovsky, Sergei ;
Kaloper, Nemanja ;
March-Russell, John .
PHYSICAL REVIEW D, 2010, 81 (12)