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相关论文: Light Gluino, Light Bottom Squark Scenario, and LE…

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The light gluino (12 - 16 GeV) and light sbottom (2 - 6 GeV) scenario has been used to explain the apparent overproduction of b-quarks at the Tevatron. This scenario also predicts the decay Z -> b b-bar ~g ~g where the gluinos subsequently…

高能物理 - 唯象学 · 物理学 2011-01-27 Rahul Malhotra , Duane A. Dicus

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…

高能物理 - 唯象学 · 物理学 2011-01-27 Rahul Malhotra

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…

高能物理 - 唯象学 · 物理学 2014-11-17 Adam K. Leibovich , David Rainwater

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 $2-5.5$…

高能物理 - 唯象学 · 物理学 2009-09-01 kingman Cheung , Wai-Yee Keung

In the framework of minimal supersymmetric model we examine the Z-peak constraints on the scenario of one light sbottom (2--5.5 GeV) and light gluino (12--16 GeV), which has been successfully used to explain the excess of bottom quark…

高能物理 - 唯象学 · 物理学 2011-01-27 Junjie Cao , Zhaohua Xiong , Jin Min Yang

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…

高能物理 - 唯象学 · 物理学 2008-11-26 E. L. Berger , B. W. Harris , D. E. Kaplan , Z. Sullivan , T. M. P. Tait , C. E. M. Wagner

We consider single squark production in $p\overline{p}$ collisions at $\sqrt{s}=1800$ Gev in the light gluino scenario, where production is dominated by the parton subprocess $qg\rightarrow \tilde{q}\tilde{g}\rightarrow…

高能物理 - 唯象学 · 物理学 2008-11-26 I. Terekhov , L. Clavelli

The minimal supersymmetric model with light sbottom ($\sim m_b$) and light gluino (12 $\sim$ 16 GeV) can explain the excess of bottom quark production cross section at hadron colliders and has drawn much attention. We calculate one-loop…

高能物理 - 唯象学 · 物理学 2008-11-26 Seungwon Baek

An interesting prediction of a string-inspired {\em one-parameter} $SU(5)\times U(1)$ supergravity model, is the fact that the lightest member ($\tilde t_1$) of the top-squark doublet $(\tilde t_1,\tilde t_2)$, may be substantially lighter…

高能物理 - 唯象学 · 物理学 2009-08-25 J. Lopez , D. Nanopoulos , A. Zichichi

A very light gluino ($m_{\tilde g} \lsim 2 \gev$) is still consistent with experimental data and is attractive from a theoretical standpoint. This has been shown to lead to a small gluino content of the proton. We use this effect to…

高能物理 - 唯象学 · 物理学 2007-05-23 Debajyoti Choudhury

In some supersymmetric models, the gluino is predicted to be light and stable. In that case, it would hadronize to form R-hadrons. In these models, the missing energy signature of the lightest supersymmetric particle is no longer valid,…

高能物理 - 实验 · 物理学 2008-11-26 The DELPHI Collaboration , J. Abdallah

We search for physics beyond the standard model using events with a photon, two or more hadronic jets, and an apparent imbalance in transverse energy, in $p\bar{p}$ collisions at the Fermilab Tevatron at $\sqrt{s}=1.8$ TeV. Such events are…

高能物理 - 实验 · 物理学 2008-11-26 B. Abbott

We consider the production of gravitinos ($\widetilde G$) in association with gluinos ($\tilde g$) or squarks ($\tilde q$) at hadron colliders, including the three main sub-processes: $q \bar q -> \tilde g\widetilde G$, $qg -> \tilde…

高能物理 - 唯象学 · 物理学 2009-08-25 Jaewan Kim , Jorge L. Lopez , D. V. Nanopoulos , Raghavan Rangarajan , A. Zichichi

We address the compatibility of a light sbottom (mass $2\sim 5.5 \gev$) and a light gluino (mass $12\sim 16 \gev$) with electroweak precision measurements. Such light particles have been suggested to explain the observed excess in the $b$…

高能物理 - 唯象学 · 物理学 2008-11-26 Gi-Chol Cho

In supersymmetric models where the magnitude of the GUT scale gaugino mass parameter M_3 is suppressed relative to M_1 and M_2, the lightest neutralino can be a mixed higgsino-bino state with a thermal relic abundance in agreement with the…

高能物理 - 唯象学 · 物理学 2008-11-26 Howard Baer , Azar Mustafayev , Stefano Profumo , Xerxes Tata

Within the supergravity framework, sleptons are expected to be considerably lighter than squarks if gluinos and squarks are approximately degenerate. This can lead to a significant enhancement in leptonic branching ratio for neutralinos,…

高能物理 - 唯象学 · 物理学 2009-12-30 H. Baer , C. Kao , X. Tata

In scenarios with relatively light down squarks, motivated, e.g., by SO(10) D terms, jets + missing $E_T$ signals can be observed at the luminosity upgraded Tevatron even if the squarks are much heavier than the gluinos and the common…

高能物理 - 唯象学 · 物理学 2008-11-26 Amitava Datta , Shyamapada Maity , Anindya Datta

The effects of light, long-lived gluinos on $2\to 2$ processes at hadron colliders are examined. Such particles can mediate single squark resonant production via $q\glu\to\sq\to q\glu$ which would significantly modify the dijet data sample.…

高能物理 - 唯象学 · 物理学 2008-11-26 J. Hewett , T. Rizzo , M. Doncheski

We calculate the production cross-sections for the vector and pseudoscalar bound states of two gluinos. It is shown that existing and future colliders imply a realistic chance of observing gluinonium as a narrow peak in the two-jet…

高能物理 - 唯象学 · 物理学 2008-11-26 E. Chikovani , V. Kartvelishvili , R. Shanidze , G. Shaw , .

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.…

高能物理 - 唯象学 · 物理学 2016-11-23 Edmond L. Berger
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