1992
DOI: 10.1016/0550-3213(92)90052-d
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Axion hair and dynamical torsion from anomalies

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Cited by 100 publications
(250 citation statements)
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“…In an effective field theory framework [9,18], the derivative of the Kalb-Ramond axion field ∂ µ b couples to the axial fermion current ψ i γ µ γ 5 ψ i , where i runs over fermion species of the Standard Model (SM), but the scalars couple only gravitationally to the SM fields (unless they are composites of heavy fermions which may couple to SM fields through loops). Hence the actual production mechanism of the global monopole solution at colliders, such as the LHC, and their detection, needs to be examined carefully.…”
Section: Discussion: Constraining the Model By Experimentsmentioning
confidence: 99%
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“…In an effective field theory framework [9,18], the derivative of the Kalb-Ramond axion field ∂ µ b couples to the axial fermion current ψ i γ µ γ 5 ψ i , where i runs over fermion species of the Standard Model (SM), but the scalars couple only gravitationally to the SM fields (unless they are composites of heavy fermions which may couple to SM fields through loops). Hence the actual production mechanism of the global monopole solution at colliders, such as the LHC, and their detection, needs to be examined carefully.…”
Section: Discussion: Constraining the Model By Experimentsmentioning
confidence: 99%
“…Their inclusion for Abelian gauge fields could lead to additional interesting electromagnetic effects [17], which, however, are not of interest to us here. 7 In a Feynman path-integral formulation the dual theory for the Lagrangian (3.1) (in a Minkowski-signature space-time) is obtained [9,18] by implementing the Bianchi constraint (3.7) via a path-integral δ-function, which can then be represented using a Lagrange multiplier field b(x). The dual theory is obtained on integrating out the field H µνρ in the path-integral.…”
Section: A a Model For A Self-gravitating Global Monopole With Kalb-mentioning
confidence: 99%
“…The background field / B ≡ γ μ B μ is assumed at most a function of the cosmic time, so as to respect the isotropy and homogeneity of the early universe, where such backgrounds are non-trivial. We note at this point that, if the axial background field B μ is to be identified [43] with the totally antisymmetric field strength (H μνρ = ∂ μ B ρσ + cyclic permutation of indices) of the Kalb-Ramond [44] spin-one field B μν , that appears in the massless gravitational multiplet of string theory [45][46][47], then the latter is viewed as part of a torsion background [48]: B μ = μνρλ H νρλ . In such a case one should also consider the coupling of the axial field B μ to all other fermions of the SM sector, ψ j ( j = leptons, quarks) via a universal minimal prescription, with the coupling with all fermionic species ψ being the same :…”
Section: Review Of the Cpt Violating Model For Leptogenesismentioning
confidence: 99%
“…The model was based on a specific extension of the SM, involving massive Majorana right-handed neutrinos (RHN), propagating on a Lorentz and CPTV, constant in time, axial vector background coupling to fermions. The latter could be traced back to a specific configuration of a cosmological Kalb-Ramond (KR) antisymmetric tensor field [44] that appears in the gravitational multiplet of string theory [45][46][47][48][49], and plays the rôle of torsion in a generalised connection, although we do not restrict ourselves to such an identification. 2 The involvement of sterile RHN in the model is physically motivated primarily by the need to provide a natural explanation for the light neutrino masses of the SM sector.…”
Section: Introductionmentioning
confidence: 99%
“…It is an axial pseudovector field, one of the three types of structures appearing in the irreducible decomposition of T [850,853]. The gravitational part of the action can be written as…”
Section: Anomalous Majorana Neutrino Masses From Torsionful Quantum Gmentioning
confidence: 99%