No cosmological domain wall problem for weakly coupled fields

ArXiv hep-ph/0106272 (2001)

Authors:

Horacio Casini, Subir Sarkar

Abstract:

After inflation occurs, a weakly coupled scalar field will in general not be in thermal equilibrium but have a distribution of values determined by the inflationary Hubble parameter. If such a field subsequently undergoes discrete symmetry breaking, then the different degenerate vacua may not be equally populated so the domain walls which form will be `biased' and the wall network will subsequently collapse. Thus the cosmological domain wall problem may be solved for sufficiently weakly coupled fields in a post-inflationary universe. We quantify the criteria for determining whether this does happen, using a Higgs-like potential with a spontaneously broken $Z_2$ symmetry.

No cosmological domain wall problem for weakly coupled fields

(2001)

Authors:

Horacio Casini, Subir Sarkar

Brane-World Inflation and the Transition to Standard Cosmology

(2001)

Authors:

Andre Lukas, David Skinner

A Minimal S^1/(Z_2 x Z_2') Orbifold GUT

ArXiv hep-ph/0106166 (2001)

Authors:

A Hebecker, J March-Russell

Abstract:

We investigate supersymmetric SU(5) grand-unified theories (GUTs) realized in 5 space-time dimensions and broken down to the MSSM by SU(5)-violating boundary conditions on a S^1/(Z_2 x Z_2') orbifold with two 3-branes. The doublet-triplet splitting problem is entirely avoided by locating the MSSM Higgs doublets on the brane on which SU(5) is not a good symmetry. An extremely simple model is then described in which the MSSM matter is also located on this SU(5)-violating brane. Although this model does not unify the MSSM matter within SU(5) multiplets, it explains gauge coupling unification. A second model with MSSM matter in the SU(5)-symmetric bulk preserves both the SU(5) explanation of fermion quantum numbers as well as gauge-coupling unification. Both models naturally avoid problematic SU(5) predictions for the Yukawa couplings of the first two generations and are consistent with proton decay constraints. We analyse the running of gauge couplings above the compactification scale in terms of a 5d effective action and derive the implications for the values of compactification scale, unification scale and of the scale at which the bulk gauge theory becomes strongly coupled.

A Minimal S^1/(Z_2 x Z_2') Orbifold GUT

(2001)

Authors:

A Hebecker, J March-Russell