scholarly journals Higgs boson and Top quark masses as tests of Electroweak Vacuum Stability

2013 ◽  
Author(s):  
Isabella MASINA
1989 ◽  
Vol 40 (5) ◽  
pp. 1725-1729 ◽  
Author(s):  
W. Marciano ◽  
G. Valencia ◽  
S. Willenbrock

1991 ◽  
Vol 06 (18) ◽  
pp. 1701-1707
Author(s):  
S. MAHAJAN ◽  
A. MUKHERJEE ◽  
N. PANCHAPAKESAN ◽  
R. P. SAXENA ◽  
S. K. SETHI

It is pointed out that by imposing the requirement of non-negativity on the running ϕ4 coupling λ(t) in the standard electroweak model, lower bounds on the masses of the Higgs boson and the top quark can be obtained. If m H ≳ 25 GeV , the bound corresponds to mt ≳ 45 GeV . More useful bounds can be derived in a temperature-dependent theory.


2020 ◽  
Vol 35 (21) ◽  
pp. 2050117
Author(s):  
Heng-Yu Chen ◽  
Ilia Gogoladze ◽  
Shan Hu ◽  
Tianjun Li ◽  
Lina Wu

We present a class of nonsupersymmetric models in which the so-called critical Higgs inflation [Formula: see text] can be naturally realized without using specific values for Higgs and top quark masses. In these scenarios, the Standard Model (SM) vacuum stability problem, gauge coupling unification, neutrino mass generation and Higgs inflation mechanism are linked to each other. We adopt in our models Type I seesaw mechanism for neutrino masses. An appropriate choice of the Type I seesaw scale allows us to have an arbitrarily small but positive value of SM Higgs quartic coupling around the inflation scale. We present a few benchmark points where we show that the scalar spectral indices are around 0.9626 and 0.9685 for the number of [Formula: see text]-folding [Formula: see text] and [Formula: see text], respectively. The tensor-to-scalar ratios are of the order of [Formula: see text]. The running of the scalar spectral index is negative and is of the order of [Formula: see text].


2006 ◽  
Vol 74 (9) ◽  
Author(s):  
Brian Feldstein ◽  
Lawrence J. Hall ◽  
Taizan Watari
Keyword(s):  

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