scholarly journals Higgs Scalar Fields and Discrete Symmetry

1995 ◽  
Vol 93 (6) ◽  
pp. 1093-1104 ◽  
Author(s):  
G. Konisi ◽  
T. Saito
2013 ◽  
Vol 28 (14) ◽  
pp. 1350054 ◽  
Author(s):  
ALFONSO R. ZERWEKH

In this paper, we explore the possibility of constructing the quantum chromodynamics of a massive color-octet vector field without introducing higher structures like extended gauge symmetries, extra dimensions or scalar fields. We show that gauge invariance is not enough to constraint the couplings. Nevertheless, the requirement of unitarity fixes the values of the coupling constants, which otherwise would be arbitrary. Additionally, it opens a new discrete symmetry which makes the coloron stable and avoid its resonant production at a collider. On the other hand, a judicious definition of the gauge fixing terms modifies the propagator of the massive field making it well-behaved in the ultraviolet limit. The relation between our model and the more general approach based on extended gauge symmetries is also discussed.


1991 ◽  
Vol 06 (37) ◽  
pp. 3375-3383 ◽  
Author(s):  
ANJAN S. JOSHIPURA ◽  
SAURABH D. RINDANI

A model with two Higgs doublets is presented where a discrete symmetry is imposed so that the flavor-changing neutral currents in the down-quark sector are naturally suppressed and obey a hierarchy determined by the hierarchy of the Kobayashi-Maskawa matrix elements. The fermion couplings to charged-Higgs bosons are different from those in models with natural flavor conservation. As a consequence, it is possible to have a light top quark which evades the Tevatron limit by decaying predominantly into a light charged Higgs with mass M H ≤ mt - mb. The model is also consistent with data on ε and [Formula: see text] mixing for a wide range of M H and the ratio of vacuum expectation values of the scalar fields.


2002 ◽  
Vol 80 (9) ◽  
pp. 1085-1091
Author(s):  
M -P Gagné-Portelance ◽  
D.G.C. McKeon

We examine a supersymmetric model in three dimensions containing two massless scalar superfields Φ1 and Φ2. The most generalized renormalizable interaction is characterized by two coupling if there is a discrete symmetry Φ1 [Formula: see text] ± Φ2; the renormalization group functions are computed to lowest order for these couplings. It is found that asymptotic freedom for one of these couplings occurs in a region of coupling-constant space. PACS Nos.: 11.30Pb


1994 ◽  
Vol 09 (10) ◽  
pp. 875-883 ◽  
Author(s):  
NOUREDDINE MOHAMMEDI

We consider gravity using the formalism of a differential Z2-graded algebra of 2 × 2 matrices whose elements are differential forms on space-time. The connection and the orthonormal frame are extended to incorporate additional scalar and vector fields. The extended torsion-free constraints are solved for a simple case. The resulting action describes a set of scalar fields minimally coupled to Einstein-Hilbert gravity.


2001 ◽  
Vol 16 (13) ◽  
pp. 2365-2390 ◽  
Author(s):  
L. V. LAPERASHVILI ◽  
H. B. NIELSEN

Using a one-loop renormalization group improvement for the effective potential in the Higgs model of electrodynamics with electrically and magnetically charged scalar fields, we argue for the existence of a triple (critical) point in the phase diagram ([Formula: see text]), where λ run is the renormalized running self-interaction constant of the Higgs scalar monopoles and g run is their running magnetic charge. This triple point is a boundary point of three first-order phase transitions in the dual sector of the Higgs scalar electrodynamics: The "Coulomb" and two confinement phases meet together at this critical point. Considering the arguments for the one-loop approximation validity in the region of parameters around the triple point A we have obtained the following triple point values of the running couplings: [Formula: see text], which are independent of the electric charge influence and two-loop corrections to [Formula: see text] with high accuracy of deviations. At the triple point the mass of monopoles is equal to zero. The corresponding critical value of the electric fine structure constant turns out to be [Formula: see text] by the Dirac relation. This value is close to the [Formula: see text], which in a U(1) lattice gauge theory corresponds to the phase transition between the "Coulomb" and confinement phases. In our theory for α ≥ α crit there are two phases for the confinement of the electrically charged particles. The results of the present paper are very encouraging for the antigrand unification theory which was developed previously as a realistic alternative to SUSY GUT's. The paper is also devoted to the discussion of this problem.


1980 ◽  
Vol 33 (6) ◽  
pp. 941 ◽  
Author(s):  
BG Wybourne

The. properties of Schur functions are used to enumerate the terms that must appear in a G-invariant symmetric quartic polynomial constructed from a set of Higgs fields. The importance of classifying Higgs fields as to their orthogonal, symplectic or complex representations is emphasized. The peculiar difficulties associated with symplectic irreps are noted. The groups SUs and SOlO are used to provide examples of the methods developed.


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