Bulk and brane radiative effects in gauge theories on orbifolds

Details Bulk and brane radiative effects in gauge theories on orbifolds Bulk and brane radiative effects in gauge theories on orbifolds

2002-04-25

arxiv.org/abs/hep-th/0204223v1

Nucl.Phys.B635:127-157,2002

Physics

High Energy Physics

High Energy Physics - Theory

31 pages, uses axodraw.sty and mcite.sty

Scientific paper

10.1016/S0550-3213(02)00395-4

We have computed one-loop bulk and brane mass renormalization effects in a five-dimensional gauge theory compactified on the M_4 \times S^1/Z_2 orbifold, where an arbitrary gauge group G is broken by the orbifold action to its subgroup H. The space-time components of the gauge boson zero modes along the H generators span the gauge theory on the orbifold fixed point branes while the zero modes of the higher-dimensional components of the gauge bosons along the G/H generators play the role of Higgs fields with respect to the gauge group H. No quadratic divergences in the mass renormalization of the gauge and Higgs fields are found either in the bulk or on the branes. All brane effects for the Higgs field masses vanish (only wave function renormalization effects survive) while bulk effects are finite and can trigger, depending on the fermionic content of the theory, spontaneous Hosotani breaking of the brane gauge group H. For the gauge fields we do find logarithmic divergences corresponding to mass renormalization of their heavy Kaluza-Klein modes. Two-loop brane effects for Higgs field masses are expected from wave function renormalization brane effects inserted into finite bulk mass corrections.

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