General upper bounds on the light-neutral-Higgs-boson mass in minimal low-energy supergravity

1986 ◽  
Vol 33 (3) ◽  
pp. 773-776 ◽  
Author(s):  
E. Reya
2014 ◽  
Vol 29 (18) ◽  
pp. 1430032 ◽  
Author(s):  
S. Heinemeyer ◽  
M. Mondragón ◽  
G. Zoupanos

Finite Unified Theories (FUTs) are N = 1 supersymmetric Grand Unified Theories (GUTs) which can be made finite to all-loop orders, based on the principle of reduction of couplings, and therefore are provided with a large predictive power. We confront the predictions of an SU(5) FUT with the top and bottom quark masses and other low-energy experimental constraints, resulting in a relatively heavy SUSY spectrum, naturally consistent with the nonobservation of those particles at the LHC. The light Higgs boson mass is automatically predicted in the range compatible with the Higgs discovery at the LHC. Requiring a light Higgs boson mass in the precise range of Mh= 125.6 ±2.1 GeV favors the lower part of the allowed spectrum, resulting in clear predictions for the discovery potential at current and future pp, as well as future e+e-colliders.


1996 ◽  
Vol 53 (11) ◽  
pp. 6689-6692 ◽  
Author(s):  
Jae Sik Lee ◽  
Jae Kwan Kim

1997 ◽  
Vol 55 (11) ◽  
pp. 7255-7262 ◽  
Author(s):  
Thomas Hambye ◽  
Kurt Riesselmann

1999 ◽  
Vol 14 (10) ◽  
pp. 1605-1632 ◽  
Author(s):  
DAVID DOOLING ◽  
KYUNGSIK KANG ◽  
SIN KYU KANG

We present lower bounds on the Higgs boson mass in the Standard Model with three and four fermion generations, SM (3,4), as well as upper bounds on the lightest Higgs boson mass in the minimal supersymmetric extension of the SM with three and four generations, MSSM (3,4). Our analysis utilizes the SM (3,4) renormalization-group-improved one-loop effective potential of the Higgs boson to find the upper bounds on the Higgs mass in the MSSM (3,4), while the lower bounds in the SM (3,4) are derived from considerations of vacuum stability. All the bounds increase as the degenerate fourth generation mass increases, providing more room in theory space that respects the increasing experimental lower limit of the Higgs mass.


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