scholarly journals 126 GeV Higgs Boson Associated with D-term Triggered Dynamical Supersymmetry Breaking

Symmetry ◽  
2015 ◽  
Vol 7 (1) ◽  
pp. 193-205 ◽  
Author(s):  
Hiroshi Itoyama ◽  
Nobuhito Maru
2012 ◽  
Vol 85 (9) ◽  
Author(s):  
Patrick Draper ◽  
Patrick Meade ◽  
Matthew Reece ◽  
David Shih

1997 ◽  
Vol 12 (30) ◽  
pp. 2229-2236
Author(s):  
Sin Kyu Kang

We compute the charged Higgs boson mass in the minimal GMSB model. We find that the present experimental bounds on Br (b→ sγ) lead to mH±≳ 445 (686) GeV for tan β=3 (40) and Mt=175 GeV. The predictions of mH± imply that the decay mode t→ H+b is closed in the minimal GMSB model.


2014 ◽  
Vol 90 (1) ◽  
Author(s):  
Antonio Delgado ◽  
Mateo Garcia ◽  
Mariano Quiros

1994 ◽  
Vol 09 (39) ◽  
pp. 3663-3671 ◽  
Author(s):  
N.V. KRASNIKOV ◽  
G. KREYERHOFF ◽  
R. RODENBERG

We study the dependence of the Higgs boson mass on the scale of supersymmetry breaking in the minimal supersymmetric extension of the standard Weinberg-Salam model.


2014 ◽  
Vol 29 (27) ◽  
pp. 1450162 ◽  
Author(s):  
Tomáš Blažek ◽  
Peter Maták

We analyze the role of the left–left squark mixing in the rare [Formula: see text] decay within the minimal supersymmetry with a large tan β. A Higgs boson mass of 125 GeV has been taken into account leading to correlation between stop masses and trilinear soft supersymmetry breaking coupling [Formula: see text]. We find that measurable effects, similar to that of the well known LR squark mixing terms, are possible for large [Formula: see text] combined with the off-diagonal LL-insertions. Precise measurements of the decay rate are expected from the ongoing NA62 experiment at CERN. We emphasize that the effect we present can put certain limits on the left–left flavor changing structure of the squark mass matrix.


2015 ◽  
Vol 30 (15) ◽  
pp. 1540014
Author(s):  
Tony Gherghetta

The first run of the LHC has been tremendously successful, having discovered the Higgs boson as well as having set stringent limits on superpartner masses. This has severely constrained supersymmetric models. A consistent scenario based on LHC data suggests that the third generation sfermions, Higgsinos and the gluino must be light while the first two generation sfermions are heavy. Furthermore, an extra contribution to the Higgs quartic coupling is needed to explain the 126 GeV Higgs mass. Interestingly this spectrum can naturally arise from supersymmetry breaking in a warped geometry where the sfermion spectrum is related to the fermion mass hierarchy. Various possible scenarios are reviewed and compared with the data from the first run at the LHC.


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