Degenerate vacuum formalism for spontaneous symmetry breakdown

1971 ◽  
Vol 4 (5) ◽  
pp. 632-637 ◽  
Author(s):  
R N Sen ◽  
C Weil
Keyword(s):  
Symmetry Breakdown ◽  
Spontaneous Symmetry Breakdown

Decoupling in theories with spontaneous symmetry breakdown

1982 ◽  
Vol 26 (8) ◽  
pp. 2086-2091 ◽  
Author(s):  
Gerry McKeon
Keyword(s):  
Symmetry Breakdown ◽  
Spontaneous Symmetry Breakdown

CLEAN PRECISION TESTS OF THE ELECTROWEAK THEORY

1992 ◽  
Vol 07 (12) ◽  
pp. 1009-1021 ◽  
Author(s):  
ZENRŌ HIOKI
Keyword(s):  
Experimental Data ◽  
Top Quark ◽  
Higgs Mass ◽  
Quantum Correction ◽  
Electroweak Theory ◽  
Weak Boson ◽  
Yukawa Couplings ◽  
Symmetry Breakdown ◽  
Electroweak Precision ◽  
Spontaneous Symmetry Breakdown

Present status of electroweak precision tests via the weak boson masses is reviewed, emphasizing that the standard SU(2) × U(1) theory is phenomenologically very successful also at quantum correction level. In particular, it is shown that the latest experimental data indicate the existence not only of the whole one-loop corrections but also of the non-decoupling top-quark effects, independent of the Higgs mass, which are a characteristic feature of theories with masses generated by spontaneous symmetry breakdown plus large Yukawa couplings.

UNIFIED ELECTROWEAK MODEL BASED ON SPACE–TIME AND ISOSPIN SYMMETRIES

2005 ◽  
Vol 20 (01) ◽  
pp. 175-198 ◽  
Author(s):  
D. SPEHLER ◽  
G. C. MARQUES
Keyword(s):  
Degrees Of Freedom ◽  
Space Time ◽  
Scalar Particles ◽  
Symmetry Breakdown ◽  
Vector Bosons ◽  
Rank 2 ◽  
Electroweak Model ◽  
Spontaneous Symmetry Breakdown ◽  
Internal Degrees Of Freedom

We propose a spinorial approach to the unified electroweak interactions, in which no use is made of spontaneous symmetry breakdown. No scalar particles are needed in order to break the symmetry. No reference is made to gauge symmetry. Our approach stresses the role of space–time and isospin symmetries in the build up of the electroweak model. Internal degrees of freedom, such as isospin, are incorporated in the theory by using spinors carrying isospin indices. All vector bosons are described by a rank 2 field in the spinorial and the isospinorial indices. Leptons are accomodated in a rank 1 spinor field and in a rank 2 isospin field as well. The dynamical variables of the theory are the chiral and isochiral components of these fields.

Spontaneous symmetry breakdown and Regge intercepts

1974 ◽  
Vol 50 (4) ◽  
pp. 475-478 ◽  
Author(s):  
R.F. Cahalan ◽  
P.H. Frampton
Keyword(s):  
Symmetry Breakdown ◽  
Spontaneous Symmetry Breakdown

Particle mixing from spontaneous symmetry breakdown

1970 ◽  
Vol 65 (1) ◽  
pp. 89-98 ◽  
Author(s):  
G. Cicogna ◽  
R. Vergara Caffarelli
Keyword(s):  
Symmetry Breakdown ◽  
Particle Mixing ◽  
Spontaneous Symmetry Breakdown

Spontaneous symmetry breakdown in anSL(2n,C)⊗SL(2,C)-invariant gravitational model

1977 ◽  
Vol 15 (4) ◽  
pp. 983-995 ◽  
Author(s):  
Phillip W. Dennis ◽  
Justin C. Huang
Keyword(s):  
Symmetry Breakdown ◽  
Gravitational Model ◽  
Spontaneous Symmetry Breakdown

Typical spontaneous symmetry breakdown in solid state as revealed by Fe3O4

1979 ◽  
Vol 50 (B11) ◽  
pp. 7584 ◽  
Author(s):  
S. Iida ◽  
M. Mizoguchi ◽  
S. Umemura ◽  
J. Yoshida ◽  
K. Kato ◽  
...  
Keyword(s):  
Solid State ◽  
Symmetry Breakdown ◽  
Spontaneous Symmetry Breakdown

Spin-isospin mixing without spontaneous symmetry breakdown

1983 ◽  
Vol 17 (2) ◽  
pp. 141-144
Author(s):  
A. Mukhrejee ◽  
Probir Roy
Keyword(s):  
Symmetry Breakdown ◽  
Spontaneous Symmetry Breakdown
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