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Electroweak renormalization of neutralino-Higgs interactions at one loop and its impacts on spin-independent direct detection of Wino-like dark matter

Subhadip Bisal, Arindam Chatterjee, Debottam Das, Syed Adil Pasha   +3 more
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The topology of the electroweak interaction [PDF]

Journal of Mathematical Physics, 2005
In this paper we show that the Higgs boson of the (minimal) standard model has at most three gauge inequivalent ground states. One of these states is related to ordinary electromagnetism and the other two to electromagnetism within magnetically charged vacua.
J. Tolksdorf
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The electroweak interaction

, 2015
Nuclear and Particle Physics provides an introductory course on nuclear and particle physics for undergraduate and early-graduate students, which the author has taught for several years at the University of Zurich.
C. Amsler
semanticscholar   +1 more source

SEE-SAW MASSES FOR QUARKS AND LEPTONS IN AN AMBIDEXTROUS ELECTROWEAK INTERACTION MODEL

, 1987
An ambidextrous electroweak interaction model with SU(2)L×SU(2)R×U(1) gauge symmetry is described in which the conventional quarks and leptons are accompanied by a set of new fermions that transform as singlets of SU(2)L×SU(2)R.
S. Rajpoot
semanticscholar   +1 more source

The electroweak interaction.

, 1986
Until the early 1970s, it was believed that there were four fundamental forces: strong nuclear, electromagnetic, weak nuclear, and gravity. It was by the work of S. Glashow, S. Weinberg, and A.
R. Turlay
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A note on the geometry of connections in gauge theories of the electroweak interaction

, 1982
It is shown that in gauge theories of the electroweak interaction, the symmetry-breaking process always defines a genuine connection on the electromagnetic sub-bundle.
B. McInnes
semanticscholar   +1 more source

THEORY OF TRANSITIONS, AND THE ELECTROWEAK INTERACTION

1988
G. Drake
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Chiral electroweak gauge interactions

Physical Review D, 1990
The hypercharge U(1){sub {ital Y}} of the standard electroweak model is split into chiral hypercharges U(1){sub {ital L}}{times}U(1){sub {ital R}}. Under the new gauge symmetry SU(2){sub {ital L}}{times}U(1){sub {ital L}}{times}U(1){sub {ital R}}, quarks and leptons are left-handed doublets transforming only under SU(2){sub {ital L}}{times}U(1){sub ...
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The state of electroweak interactions

AIP Conference Proceedings, 1984
I assess what we know and what we do not know about the electroweak interactions. In particular, I argue that existing data on the electroweak parameters ρ, sin2θw and GF and on the recently discovered W± and Z0 allow us reasonably to conclude that: (1) the W± and Z0 truly are the elementary massive gauge bosons of SU(2)×U(1) and not the composite ...
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Lagrangians of the Electroweak Interactions

1984
We proceed with the models of electromagnetic and weak interactions. To construct the Lagrangian for a unified model, the following steps are required. 1) Choosing the gauge group which determines the interaction-mediating fields; the number of the gauge fields is equal to the dimension of the adj oint representation of this group; 2)
Nikolai F. Nelipa, Masud Chaichian
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