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Related papers: Is $M_t\simeq M_w$ Ruled Out?

200 papers

We advocate the study of supergravity models as well motivated few-parameter low-energy supersymmetric models. In this context we survey a broad range of phenomenological constraints and future tests, including present and near-future…

High Energy Physics - Phenomenology · Physics 2007-05-23 J. Lopez

We adopt a Markov Chain Monte Carlo method to examine various new physics models which can generate the forward-backward asymmetry in top quark pair production observed at the Tevatron by the CDF Collaboration. We study the following new…

High Energy Physics - Phenomenology · Physics 2014-11-20 Qing-Hong Cao , David McKeen , Jonathan L. Rosner , Gabe Shaughnessy , Carlos E. M. Wagner

Various measurements of the top quark mass in the lepton+jets decay channel of top quark pair production are presented. The measurements are performed on data samples of up to 2.7 fb-1 of integrated luminosity acquired by the CDF and D0…

High Energy Physics - Experiment · Physics 2008-12-09 Christian Schwanenberger

A search for pair production of third-generation scalar leptoquarks decaying to top quark and tau lepton pairs is presented using proton-proton collision data at a center-of-mass energy of sqrt(s) = 8 TeV collected with the CMS detector at…

High Energy Physics - Experiment · Physics 2016-11-22 CMS Collaboration

We study the production and decays of top squarks (stops) at the Tevatron collider in models of low-energy supersymmetry breaking. We consider the case where the lightest Standard Model (SM) superpartner is a light neutralino that…

High Energy Physics - Phenomenology · Physics 2008-11-26 Marcela Carena , Debajyoti Choudhury , Rodolfo A. Diaz , Heather E. Logan , Carlos E. M. Wagner

A seesaw mass matrix model is reviewed as a unification model of quark and lepton mass matrices. The model can understand why top-quark mass m_t is so singularly enhanced compared with other quark masses, especially, why m_t >> m_b in…

High Energy Physics - Phenomenology · Physics 2007-05-23 Yoshio Koide

With the full Tevatron Run II and early LHC data samples, the opportunity for furthering our understanding of the properties of the top quark has never been more promising. Although the current knowledge of the top quark comes largely from…

High Energy Physics - Experiment · Physics 2015-06-03 Kevin Lannon , Fabrizio Margaroli , Chris Neu

Using a frequentist analysis of experimental constraints within two versions of the minimal supersymmetric extension of the Standard Model, we derive the predictions for the top quark mass, m_t, and the W boson mass, m_W. We find that the…

High Energy Physics - Phenomenology · Physics 2010-04-23 O. Buchmueller , R. Cavanaugh , A. De Roeck , J. R. Ellis , H. Flacher , S. Heinemeyer , G. Isidori , K. A. Olive , F. J. Ronga , G. Weiglein

The top quark is the most recently discovered quark. Relatively little is known about its properties so far. Due to its very large mass of about $175 \rm GeV/c^2$, the top quark behaves differently from all other quarks and provides a…

High Energy Physics - Experiment · Physics 2007-05-23 Arnulf Quadt

A sequential fourth generation is still viable, but the t' and b' quarks are constrained to be not too far apart in mass. The t'{\to}bW and b'{\to}tW decay channels are still being pursued at the Tevatron, which would soon be surpassed by…

High Energy Physics - Phenomenology · Physics 2011-08-09 Yuan Chao , Kai-Feng Chen , Shing-Kuo Chen , Wei-Shu Hou , Bo-Yan Huang , Yeong-Jyi Lei

Recent development of the universal seesaw mass matrix model is reviewed. The model was proposed in order to explain why quark and lepton masses are so small compared with the electroweak scale \Lambda_L =<\phi_L^0>=174 GeV. However, the…

High Energy Physics - Phenomenology · Physics 2009-09-25 Yoshio Koide

Motivated by the recent experimental observation of exclusive chi_c events at the Tevatron, we revisit earlier studies of central exclusive scalar chi_c0 meson production, before generalising the existing formalism to include chi_c1 and…

High Energy Physics - Phenomenology · Physics 2010-02-11 L. A. Harland-Lang , V. A. Khoze , M. G. Ryskin , W. J. Stirling

Existence of the fourth family follows from the basics of the Standard Model and the actual mass spectrum of the third family fermions. We discuss possible manifestations of the fourth SM family at existing and future colliders. The LHC and…

High Energy Physics - Phenomenology · Physics 2013-05-29 M. Sahin , S. Sultansoy , S. Turkoz

In the upcoming LHC Run 2, at $\sqrt{s} \sim13$ TeV, it is suggested to seek unusually charged ($Q= -4/3$ and $+5/3$) quarks with mass $M_Q \sim 3$ TeV which carry lepton number ($L = +2$ and $-2$ respectively) and decay superweakly to a…

High Energy Physics - Phenomenology · Physics 2015-04-23 Paul Howard Frampton

Data collected by the D0 detector at a p-pbar center-of-mass energy of 1.96 TeV at the Fermilab Tevatron Collider have been used to search for pair production of the lightest supersymmetric partner of the top quark decaying into $b \ell…

High Energy Physics - Experiment · Physics 2010-04-08 D0 Collaboration , V. Abazov

We perform a comparative study of the reach of future $e^+e^-$ collider options for the scale of non-resonant new physics effects in the top quark sector, phrased in the language of higher-dimensional operators. Our focus is on the…

High Energy Physics - Phenomenology · Physics 2017-10-26 Christoph Englert , Michael Russell

We propose a supersymmetric composite model with three generations in which supersymmetry and electroweak symmetry are broken dynamically, and masses of quarks and leptons are generated without introducing any mass scales by hand. All the…

High Energy Physics - Phenomenology · Physics 2007-05-23 Noriaki Kitazawa

We calculate the strength of the electroweak phase transition in a supersymmetric model with four chiral generations. The additional chiral fermions (and scalar partners) lower the critical temperature and thus strengthen the first-order…

High Energy Physics - Phenomenology · Physics 2008-11-26 Ricky Fok , Graham D. Kribs

The imminent start of the Large Hadron Collider, which is expected to produce $\sim 10^8$ $t\bar{t}$ pairs per year, provides an unprecedented opportunity for top physics. As the top quark is widely expected to be rather sensitive to…

High Energy Physics - Phenomenology · Physics 2010-05-12 Jennifer Kile , Amarjit Soni

The forward-backward asymmetry $A_{FB}^{t\bar t}$ in top quark production at the Tevatron has been observed to be anomalously large by both CDF and D0. It has been suggested that a model with a $W'$ coupling to $td$ and $ub$ might explain…

High Energy Physics - Phenomenology · Physics 2011-09-08 Nathaniel Craig , Can Kilic , Matthew J. Strassler