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Related papers: Light Bottom Squark Phenomenology

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A new contribution from pair-production of light gluinos, of mass 12 to 16 GeV, with two-body decays into bottom quarks and light bottom squarks, helps to obtain a bottom-quark production rate in better agreement with hadron collider data.…

High Energy Physics - Phenomenology · Physics 2016-11-23 Edmond L. Berger

The production rate of bottom quarks at hadron colliders exceeds the expectations of next-to-leading order perturbative quantum chromodynamics. An additional contribution from pair-production of light gluinos, of mass 12 to 16 GeV, with…

High Energy Physics - Phenomenology · Physics 2014-11-17 Edmond L. Berger

A long-standing discrepancy between the bottom-quark production cross section and predictions of perturbative quantum chromodynamics is addressed. We show that pair production of light gluinos, of mass 12 to 16 GeV, with two-body decays…

High Energy Physics - Phenomenology · Physics 2008-11-26 E. L. Berger , B. W. Harris , D. E. Kaplan , Z. Sullivan , T. M. P. Tait , C. E. M. Wagner

It has been known for a long time that the cross section for bottom-quark $b$ production at hadron collider energies exceeds theoretical expectations. An additional contribution from pair-production of light gluinos $\tilde{g}$, of mass 12…

High Energy Physics - Phenomenology · Physics 2014-11-17 Edmond L. Berger

We investigate the prospects for the discovery of a neutral Higgs boson produced with one bottom quark followed by Higgs decay into a pair of bottom quarks at the CERN Large Hadron Collider (LHC) and the Fermilab Tevatron Collider. We work…

High Energy Physics - Phenomenology · Physics 2009-12-04 Chung Kao , Shankar Sachithanandam , Joshua Sayre , Yili Wang

The discrepancy between the measured and theoretical production cross section of $b$ quarks at the Tevatron can probably be explained by the recently proposed scenario of light gluinos of mass 12-16 GeV and light sbottoms of mass $2-5.5$…

High Energy Physics - Phenomenology · Physics 2009-09-01 kingman Cheung , Wai-Yee Keung

Light bottom squarks and gluinos have been invoked to explain the b quark pair production excess at the Tevatron. We investigate the associated production of ttbb at hadron colliders in this scenario, and find that the rates for this…

High Energy Physics - Phenomenology · Physics 2014-11-17 Adam K. Leibovich , David Rainwater

A search for a light pseudoscalar Higgs boson (A) produced in association with bottom quarks and decaying into a muon pair is reported. The search uses 19.7 inverse femtobarns of proton-proton collisions at a center-of-mass energy of 8 TeV,…

High Energy Physics - Experiment · Physics 2017-11-15 CMS Collaboration

In the context of the Minimal Supersymmetric extension of the Standard Model, I discuss the effects of relatively light top and bottom scalar quarks on the main production mechanism of the lightest SUSY neutral Higgs boson $h$ at the LHC,…

High Energy Physics - Phenomenology · Physics 2011-01-27 Abdelhak DJOUADI

At hadron colliders, one of the most important channels for sparticle production is expected to be the gluino pair production. In the scenario where the sbottom is lighter than the gluino, gluinos can decay into sbottom and bottom quarks.…

High Energy Physics - Phenomenology · Physics 2007-05-23 F. Mahmoudi , A. Deandrea

A recent HyperCP observation of three events in the decay Sigma^+ -> p mu^+ mu^- is suggestive of a new particle with mass 214.3 MeV. In order to confront models that contain a light Higgs boson with this observation, it is necessary to…

High Energy Physics - Phenomenology · Physics 2008-11-26 Xiao-Gang He , Jusak Tandean , G. Valencia

In the Minimal Supersymmetric Standard Model, one of the scalar top quarks can be relatively light and its couplings to Higgs bosons strongly enhanced. I will discuss two consequences of this feature: 1) the effects of scalar top loops on…

High Energy Physics - Phenomenology · Physics 2007-05-23 Abdelhak Djouadi

The presence of a light b-squark (with mass about 4 GeV) and gluino (with mass about 15 GeV) might explain the observed excess in b-quark production at the Tevatron. Though provocative, this model is not excluded by present data. The light…

High Energy Physics - Phenomenology · Physics 2008-11-26 Thomas Becher , Stephan Braig , Matthias Neubert , Alexander L. Kagan

We calculate the decay rate of scalar and pseudoscalar Higgs bosons into a pair of gluinos, within the Minimal Supersymmetric Standard Model. In the theoretically and experimentally allowed light gluino window, $\mg \sim $ 3--5 GeV, gluino…

High Energy Physics - Phenomenology · Physics 2009-10-28 A. Djouadi , M. Drees

The observation of the standard model (SM) Higgs boson decay to a pair of bottom quarks is presented. The main contribution to this result is from processes in which Higgs bosons are produced in association with a W or Z boson (VH), and are…

High Energy Physics - Experiment · Physics 2018-09-26 CMS Collaboration

A search is described for the production of a pair of bottom-type vector-like quarks (VLQs), each decaying into a b or $\mathrm{\bar{b}}$ quark and either a Higgs or a Z boson, with a mass greater than 1000 GeV. The analysis is based on…

High Energy Physics - Experiment · Physics 2021-01-04 CMS Collaboration

We investigate the phenomenological viability of a very light bottom squark, with a mass less than half of the Z boson mass. The decays of the Z and Higgs bosons to light sbottom pairs are, in a fairly model independent manner, strongly…

High Energy Physics - Phenomenology · Physics 2015-06-18 Brian Batell , Carlos E. M. Wagner , Lian-Tao Wang

In this talk, I describe a supersymmetric solution to the long-standing discrepancy between the bottom-quark production cross section and predictions of perturbative quantum chromodynamics. Pair production of light gluinos, of mass 12-16…

High Energy Physics - Phenomenology · Physics 2007-05-23 Z. Sullivan

We present a comprehensive analysis of observing a light Higgs boson in the mass range $70$ -- $110$ GeV at the 13/14 TeV LHC, in the context of the type-I two-Higgs-doublet model. The decay of the light Higgs to a pair of bottom quarks is…

High Energy Physics - Phenomenology · Physics 2018-04-11 Disha Bhatia , Ushoshi Maitra , Saurabh Niyogi

A low-energy supersymmetry scenario with a light gluino of mass 12 - 16 GeV and light sbottom (b1) of mass 2 - 6 GeV has been used to explain the apparent overproduction of b quarks at the Tevatron. In this scenario the other mass…

High Energy Physics - Phenomenology · Physics 2011-01-27 Rahul Malhotra
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