scholarly journals Slepton mass-splittings as a signal of LFV at the LHC

2010 ◽  
Vol 2010 (6) ◽  
Author(s):  
Andrzej J. Buras ◽  
Lorenzo Calibbi ◽  
Paride Paradisi
Keyword(s):  
Slepton Mass

scholarly journals PROBING SO(10) SYMMETRY BREAKING PATTERNS THROUGH SFERMION MASS RELATIONS

2005 ◽  
Vol 20 (18) ◽  
pp. 4241-4257 ◽  
Author(s):  
B. ANANTHANARAYAN ◽  
P. N. PANDITA
Keyword(s):  
Standard Model ◽  
Supersymmetry Breaking ◽  
Gauge Group ◽  
Low Energy ◽  
Grand Unification ◽  
The Standard Model ◽  
Scalar Mass ◽  
Mass Terms ◽  
Standard Model Gauge Group ◽  
Slepton Mass

We consider supersymmetric SO(10) grand unification where the unified gauge group can break to the Standard Model gauge group through different chains. The breaking of SO(10) necessarily involves the reduction of the rank, and consequent generation of nonuniversal supersymmetry breaking scalar mass terms. We derive squark and slepton mass relations, taking into account these nonuniversal contributions to the sfermion masses, which can help distinguish between the different chains through which the SO(10) gauge group breaks to the Standard Model gauge group. We then study some implications of these nonuniversal supersymmetry breaking scalar masses for the low energy phenomenology.

scholarly journals SUPERSYMMETRY AT LINEAR COLLIDERS: THE IMPORTANCE OF BEING e-e-

1998 ◽  
Vol 13 (14) ◽  
pp. 2319-2328 ◽  
Author(s):  
JONATHAN L. FENG
Keyword(s):  
Pair Production ◽  
Mass Measurements ◽  
Fermion Number ◽  
Linear Colliders ◽  
Order Of Magnitude ◽  
Model Independent ◽  
Better Than ◽  
Slepton Mass ◽  
Integrated Luminosity

Advantages of the e-e- option at linear colliders for the study of supersymmetry are highlighted. The fermion number violating process [Formula: see text] provides unique opportunities for studies of slepton masses and flavor mixings. In particular, slepton mass measurements at the 100 MeV level through threshold scans of scalar pair production may be possible. Such measurements are over an order of magnitude better than those possible in e+e- mode, require far less integrated luminosity, and may lead to precise, model-independent measurements of tan β. Implications for studying gauginos and the importance of accurate beam polarimetry are also discussed.

scholarly journals Squark and slepton mass relations in grand unified theories

1995 ◽  
Vol 51 (9) ◽  
pp. 5289-5299 ◽  
Author(s):  
H.-C. Cheng ◽  
L. J. Hall
Keyword(s):  
Grand Unified Theories ◽  
Unified Theories ◽  
Slepton Mass

scholarly journals TeV-scale horizontal symmetry and the slepton mass problem of anomaly mediation

2004 ◽  
Vol 686 (1-2) ◽  
pp. 135-154 ◽  
Author(s):  
O.C. Anoka ◽  
K.S. Babu ◽  
I. Gogoladze
Keyword(s):  
Mass Problem ◽  
Anomaly Mediation ◽  
Horizontal Symmetry ◽  
Slepton Mass

scholarly journals Probing slepton mass nonuniversality ate+e−linear colliders

2001 ◽  
Vol 63 (9) ◽  
Author(s):  
Howard Baer ◽  
Csaba Balázs ◽  
Stefan Hesselbach ◽  
J. Kenichi Mizukoshi ◽  
Xerxes Tata
Keyword(s):  
Linear Colliders ◽  
Slepton Mass

scholarly journals Supersymmetric gauged $$ \mathrm{U}{(1)}_{L_{\mu }-{L}_{\tau }} $$ model for electron and muon (g − 2) anomaly

2021 ◽  
Vol 2021 (3) ◽  
Author(s):  
Heerak Banerjee ◽  
Bhaskar Dutta ◽  
Sourov Roy
Keyword(s):  
Magnetic Moment ◽  
First Generation ◽  
Magnetic Moments ◽  
Boson Mass ◽  
Lepton Flavor Violation ◽  
Lepton Flavor ◽  
Flavor Violation ◽  
Gauge Boson Mass ◽  
Electron Magnetic Moment ◽  
Slepton Mass

Abstract Minimal gauged $$ \mathrm{U}{(1)}_{L_{\mu }-{L}_{\tau }} $$ U 1 L μ − L τ models can provide for an additional source for the muon anomalous magnetic moment however it is difficult to accommodate the discrepancy in the electron magnetic moment in tandem. Owing to the relative sign between the discrepancies in these quantities, it seems unlikely that they arise from the same source. We show that a supersymmetric (SUSY) gauged $$ \mathrm{U}{(1)}_{L_{\mu }-{L}_{\tau }} $$ U 1 L μ − L τ model can accommodate both the muon and electron anomalous magnetic moments in a very simple and intuitive scenario, without utilizing lepton flavor violation. The currently allowed parameter space in this kind of a scenario is constrained from the latest LHC and various low energy experimental data,e.g., recent COHERENT data, CCFR, Borexino, BaBaR, supernova etc. These constraints, in conjunction with the requirement to explain both lepton magnetic moments, lead to an upper bound on the first generation slepton mass, a lower bound on the second generation slepton mass and constricts the allowed range for the new gauge boson mass and coupling. The scheme can be probed at the ongoing COHERENT and Coherent CAPTAIN-Mills experiments and at future experiments, e.g., DUNE, BELLE-II etc.

KL→μe: A possible probe of slepton mass splitting?

1990 ◽  
Vol 42 (9) ◽  
pp. 3215-3217 ◽  
Author(s):  
Biswarup Mukhopadhyaya ◽  
Amitava Raychaudhuri
Keyword(s):  
Mass Splitting ◽  
Slepton Mass

Photino pair creation in a magnetic field and astrophysical limits on slepton mass

JETP Letters ◽  
1996 ◽  
Vol 63 (5) ◽  
pp. 311-315 ◽  
Author(s):  
A. V. Kurilin ◽  
A. I. Ternov
Keyword(s):  
Magnetic Field ◽  
Pair Creation ◽  
Slepton Mass

scholarly journals Slepton Mass Matrices, µ→eγ Decay and EDM in SUSYS4Flavor Model

2011 ◽  
Vol 125 (4) ◽  
pp. 653-675 ◽  
Author(s):  
Hajime Ishimori ◽  
Morimitsu Tanimoto
Keyword(s):  
Mass Matrices ◽  
Slepton Mass
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