2016/03/10 by García-Jiménez, I., López-Osorio, M. A., Martínez-Pascual, E. +3
#FOS: Physical sciences #High Energy Physics - Phenomenology (hep-ph) #High Energy Physics - Theory (hep-th)
paper · doi:10.48550/arxiv.1603.03128
We construct an effective theory for the SM with extra dimensions. We start from a theory governed by the extra-dimensional groups ISO(1,3+n) and G\rm SM(\cal M4+n)=SUC(3,\cal M4+n)× SUL(2,\cal M4+n)× UY(1,\cal M4+n), characterized by an unknown energy scale Λ and valid at energies far below this scale. Assuming that the extra dimensions are much larger than the distance scale of this theory, we construct an effective theory with symmetry groups ISO(1,3), G\rm SM(\cal M4). The theories are connected by a canonical transformation that hides ISO(1,3+n), G\rm SM(\cal M4+n) into ISO(1,3), G\rm SM(\cal M4); KK fields receive mass. Using a set of orthogonal functions \f^(\underline0),f^(\underlinem)\, generated by the Casimir invariant P2 associated with the translations subgroup T(n)⊂ISO(n), we expand the degrees of freedom of ISO(1,3+n), G\rm SM(\cal M4+n) in general Fourier series, whose coefficients are the degrees of freedom of ISO(1,3), G(\cal M4). These functions, which correspond to the projection on \|x>\ of the discrete basis \|0>,|p^(\underlinem)>\ of P2, are central to define the effective theory. Components along the ground state f^(\underline0)= do not receive mass at the compactification scale, so they are the SM fields; components along excited states f^(\underlinem)= get mass at this scale, so they are KK excitations. For any direction |p^(\underlinem)≠0> there are a massive gauge field and a pseudo-Goldstone boson. We stress resemblances of this mass-generating mechanism with the Englert-Higgs mechanism and discuss physical implications. We include a full catalog of Lagrangian terms that can be used to calculate Feynman rules.