Radiative corrections toe + ?e ? scattering mediated by neutral vector bosons

1966 ◽  
Vol 195 (4) ◽  
pp. 357-364
Author(s):  
A. D. Karpf
1995 ◽  
Vol 10 (29) ◽  
pp. 2193-2196 ◽  
Author(s):  
G. CYNOLTER ◽  
E. LENDVAI ◽  
G. PÓCSIK

Oblique radiative corrections are calculated to the parameter S in a version of the standard model where the Higgs doublet is replaced by a doublet of vector bosons and the gauge symmetry is broken dynamically. We show that to each momentum scale there exists a domain of the masses of charged and neutral vector bosons where S is compatible with the experiments. At a scale of 1 TeV this requires vector boson masses of at least m0 ≈ 400–550 GeV , m+ ≈ 200–350 GeV .


1980 ◽  
Vol 166 (3) ◽  
pp. 460-492 ◽  
Author(s):  
David Albert ◽  
William J. Marciano ◽  
Daniel Wyler ◽  
Zohreh Parsa

1991 ◽  
Vol 267 (3) ◽  
pp. 395-399 ◽  
Author(s):  
W. Buchmüller ◽  
C. Greub ◽  
P. Minkowski

1993 ◽  
Vol 08 (28) ◽  
pp. 5063-5077
Author(s):  
A.A. LIKHODED ◽  
M.V. SHEVLYAGIN ◽  
O.P. YUSHCHENKO

After the example of the extended electroweak models, which predict the existence of the heavy neutral vector boson Z′, we discuss, for the e+e− linear colliders of the new generation, the possibilities of searching for the extra boson effects provided that various configurations of the beam polarizations will be available. For the most popular models [E6-superstring-inspired, LR- and Y(YL)-composite models] we show that realization of the specific beam polarizations can substantially enhance the experiment sensitivity to the Z′ signal in comparison with the case of the unpolarized beams.


1976 ◽  
Vol 13 (7) ◽  
pp. 1856-1867 ◽  
Author(s):  
R. W. Brown ◽  
Leon B. Gordon ◽  
J. Smith ◽  
Karnig O. Mikaelian
Keyword(s):  

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