The Electroweak Theory

Keyword(s):  
1987 ◽  
Vol 77 (1) ◽  
pp. 118-131 ◽  
Author(s):  
J. Fujimoto ◽  
M. Igarashi ◽  
Y. Shimizu

1982 ◽  
Vol 73 ◽  
pp. 1-226 ◽  
Author(s):  
Ken-ichi Aoki ◽  
Zenrō Hioki ◽  
Rokuo Kawabe ◽  
Michiji Konuma ◽  
Taizo Muta
Keyword(s):  

1984 ◽  
Vol 145 (3-4) ◽  
pp. 256-260 ◽  
Author(s):  
P.V.D. Swift
Keyword(s):  

2004 ◽  
Vol 602 (2) ◽  
pp. L109-L112 ◽  
Author(s):  
D. E. Winget ◽  
D. J. Sullivan ◽  
T. S. Metcalfe ◽  
S. D. Kawaler ◽  
M. H. Montgomery

1990 ◽  
Vol 42 (3) ◽  
pp. 919-925 ◽  
Author(s):  
J. I. Kapusta

2018 ◽  
Vol 33 (04) ◽  
pp. 1830005 ◽  
Author(s):  
C. Furey

We bring to light an electroweak model which has been reappearing in the literature under various guises.[Formula: see text] In this model, weak isospin is shown to act automatically on states of only a single chirality (left). This is achieved by building the model exclusively from the raising and lowering operators of the Clifford algebra [Formula: see text]. That is, states constructed from these ladder operators mimic the behaviour of left- and right-handed electrons and neutrinos under unitary ladder operator symmetry. This ladder operator symmetry is found to be generated uniquely by [Formula: see text] and [Formula: see text]. Crucially, the model demonstrates how parity can be maximally violated, without the usual step of introducing extra gauge and extra Higgs bosons, or ad hoc projectors.


2019 ◽  
pp. 230-259
Author(s):  
David Bailin ◽  
Alexander Love

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