Phenomenology of gluino decays via loops and top-quark Yukawa coupling

1990 ◽  
Vol 42 (5) ◽  
pp. 1568-1576 ◽  
Author(s):  
Howard Baer ◽  
Xerxes Tata ◽  
Jeffrey Woodside
1994 ◽  
Vol 50 (11) ◽  
pp. 7042-7047 ◽  
Author(s):  
X. Zhang ◽  
S. K. Lee ◽  
K. Whisnant ◽  
B.-L. Young
Keyword(s):  

1998 ◽  
Vol 57 (7) ◽  
pp. 3977-3985 ◽  
Author(s):  
Andrija Rašin
Keyword(s):  

2002 ◽  
Vol 66 (3) ◽  
Author(s):  
F. Maltoni ◽  
D. Rainwater ◽  
S. Willenbrock

1985 ◽  
Vol 31 (1) ◽  
pp. 95-98 ◽  
Author(s):  
Marc Sher ◽  
Dennis Silverman
Keyword(s):  

2021 ◽  
Vol 104 (5) ◽  
Author(s):  
Till Martini ◽  
Ren-Qi Pan ◽  
Markus Schulze ◽  
Meng Xiao

2015 ◽  
Vol 120 (3) ◽  
pp. 335-343 ◽  
Author(s):  
F. Bezrukov ◽  
M. Shaposhnikov
Keyword(s):  

2008 ◽  
Vol 86 (9) ◽  
pp. 1067-1070 ◽  
Author(s):  
F A Chishtie ◽  
M D Lepage ◽  
D GC McKeon ◽  
T G Steele ◽  
I Zakout

Taking the dominant couplings in the standard model to be the quartic scalar coupling, the Yukawa coupling of the top quark, and the SU(3) gauge coupling, we consider their associated running couplings to one-loop order. Despite the nonlinear nature of the differential equations governing these functions, we show that they can be solved exactly. The nature of these solutions is discussed and their singularity structure is examined. It is shown that for a sufficiently small Higgs mass, the quartic scalar coupling decreases with increasing energy scale and becomes negative, indicative of vacuum instability. This behavior changes for a Higgs mass greater than 168 GeV, beyond which this couplant increases with increasing energy scales and becomes singular prior to the ultraviolet pole of the Yukawa coupling. Upper and lower bounds on the Higgs mass corresponding to new physics at the TeV scale are obtained and compare favourably with the numerical results of the one-loop and two-loop analyses with inclusion of electroweak couplings.PACS Nos.: 11.10.Hi, 14.80.Bn


1987 ◽  
Vol 02 (04) ◽  
pp. 1181-1188
Author(s):  
V. Barger ◽  
N.G. Deshpande ◽  
K. Hagiwara
Keyword(s):  

We investigate the signatures of leptoquarks or diquarks of the rank 5 E6 superstring model produced in [Formula: see text] and pp machines. Leptoquark decays are characterized by lack of e, μ universality [Formula: see text] and diquark decays by quark flavor non-conservation (e.g., [Formula: see text]). If the top quark is heavier than one of the scalar superpartners [Formula: see text], then it may decay dominantly by two body modes (e.g., [Formula: see text] or [Formula: see text]), invalidating the usual signatures. Two body gluino decays [Formula: see text] may swamp its conventional signatures.


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