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Related papers: Single superpartner production at Tevatron Run II

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We study the single production of first generation leptoquarks in association with a e+/- at the Fermilab Tevatron. We focus our attention on final states exhibiting a e+e- pair and jets, and perform a detailed analyses of signal and…

High Energy Physics - Phenomenology · Physics 2016-09-06 O. J. P. Eboli , T. L. Lungov

Searches for the electroweak production of single top quarks have been started at the Fermilab Tevatron proton-antiproton collider using Run II data by both the D0 and CDF collaborations. Using a dataset of approximately 160pb^-1, neither…

High Energy Physics - Experiment · Physics 2019-08-14 Reinhard Schwienhorst

We study two CP sensitive triple-product asymmetries for neutralino production e+e- \to\tilde\chi^0_i \tilde\chi^0_j and the subsequent leptonic two-body decay \tilde\chi^0_i \to \tilde l l, \tilde l \to \tilde\chi^0_1 l, for \l=…

High Energy Physics - Phenomenology · Physics 2009-11-10 A. Bartl , H. Fraas , O. Kittel , W. Majerotto

We investigate an important radiative correction to the slepton and chargino production processes. We consider a supersymmetric spectrum with a large splitting between the squark and slepton masses. In this case, in the effective theory…

High Energy Physics - Phenomenology · Physics 2009-10-30 Mihoko M. Nojiri , Damien M. Pierce , Youichi Yamada

We report the results of a search for associated production of charginos and neutralinos using a data set corresponding to an integrated luminosity of 2.3 fb-1 collected with the D0 experiment during Run II of the Tevatron proton-antiproton…

High Energy Physics - Experiment · Physics 2009-09-28 D0 Collaboration , V. Abazov

We study two CP sensitive triple-product asymmetries for neutralino production e+e- \to \tilde\chi^0_i \tilde\chi^0_j and the subsequent leptonic two-body decays \tilde\chi^0_i \to \tilde{l} l of one of the neutralinos and of the slepton…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. Bartl , H. Fraas , O. Kittel , W. Majerotto

We present a search for the pair production of scalar top quarks ($\tilde{t}_{1}$), the lightest supersymmetric partners of the top quarks, in $p\bar{p}$ collisions at a center-of-mass energy of 1.96 TeV, using data corresponding to an…

High Energy Physics - Experiment · Physics 2015-06-04 D0 Collaboration , V. M. Abazov , B. Abbott , B. S. Acharya , M. Adams , T. Adams , G. D. Alexeev , G. Alkhazov , A. Alton , G. Alverson , M. Aoki , A. Askew , B. Asman , S. Atkins , O. Atramentov , K. Augsten , C. Avila , J. BackusMayes , F. Badaud , L. Bagby , B. Baldin , D. V. Bandurin , S. Banerjee , E. Barberis , P. Baringer , J. Barreto , J. F. Bartlett , U. Bassler , V. Bazterra , A. Bean , M. Begalli , C. Belanger-Champagne , L. Bellantoni , S. B. Beri , G. Bernardi , R. Bernhard , I. Bertram , M. Besancon , R. Beuselinck , V. A. Bezzubov , P. C. Bhat , S. Bhatia , V. Bhatnagar , G. Blazey , S. Blessing , K. Bloom , A. Boehnlein , D. Boline , E. E. Boos , G. Borissov , T. Bose , A. Brandt , O. Brandt , R. Brock , G. Brooijmans , A. Bross , D. Brown , J. Brown , X. B. Bu , M. Buehler , V. Buescher , V. Bunichev , S. Burdin , T. H. Burnett , C. P. Buszello , B. Calpas , E. Camacho-Perez , M. A. Carrasco-Lizarraga , B. C. K. Casey , H. Castilla-Valdez , S. Chakrabarti , D. Chakraborty , K. M. Chan , A. Chandra , E. Chapon , G. Chen , S. Chevalier-Thery , D. K. Cho , S. W. Cho , S. Choi , B. Choudhary , S. Cihangir , D. Claes , J. Clutter , M. Cooke , W. E. Cooper , M. Corcoran , F. Couderc , M. -C. Cousinou , A. Croc , D. Cutts , A. Das , G. Davies , S. J. de Jong , E. De La Cruz-Burelo , F. Deliot , R. Demina , D. Denisov , S. P. Denisov , S. Desai , C. Deterre , K. DeVaughan , H. T. Diehl , M. Diesburg , P. F. Ding , A. Dominguez , T. Dorland , A. Dubey , L. V. Dudko , D. Duggan , A. Duperrin , S. Dutt , A. Dyshkant , M. Eads , D. Edmunds , J. Ellison , V. D. Elvira , Y. Enari , H. Evans , A. Evdokimov , V. N. Evdokimov , G. Facini , T. Ferbel , F. Fiedler , F. Filthaut , W. Fisher , H. E. Fisk , M. Fortner , H. Fox , S. Fuess , A. Garcia-Bellido , G. A. Garcia-Guerra , V. Gavrilov , P. Gay , W. Geng , D. Gerbaudo , C. E. Gerber , Y. Gershtein , G. Ginther , G. Golovanov , A. Goussiou , P. D. Grannis , S. Greder , H. Greenlee , Z. D. Greenwood , E. M. Gregores , G. Grenier , Ph. Gris , J. -F. Grivaz , A. Grohsjean , S. Grunendahl , M. W. Grunewald , T. Guillemin , G. Gutierrez , P. Gutierrez , A. Haas , S. Hagopian , J. Haley , L. Han , K. Harder , A. Harel , J. M. Hauptman , J. Hays , T. Head , T. Hebbeker , D. Hedin , H. Hegab , A. P. Heinson , U. Heintz , C. Hensel , I. Heredia-De La Cruz , K. Herner , G. Hesketh , M. D. Hildreth , R. Hirosky , T. Hoang , J. D. Hobbs , B. Hoeneisen , M. Hohlfeld , Z. Hubacek , V. Hynek , I. Iashvili , Y. Ilchenko , R. Illingworth , A. S. Ito , S. Jabeen , M. Jaffre , D. Jamin , A. Jayasinghe , R. Jesik , K. Johns , M. Johnson , A. Jonckheere , P. Jonsson , J. Joshi , A. W. Jung , A. Juste , K. Kaadze , E. Kajfasz , D. Karmanov , P. A. Kasper , I. Katsanos , R. Kehoe , S. Kermiche , N. Khalatyan , A. Khanov , A. Kharchilava , Y. N. Kharzheev , J. M. Kohli , A. V. Kozelov , J. Kraus , S. Kulikov , A. Kumar , A. Kupco , T. Kurca , V. A. Kuzmin , S. Lammers , G. Landsberg , P. Lebrun , H. S. Lee , S. W. Lee , W. M. Lee , J. Lellouch , H. Li , L. Li , Q. Z. Li , S. M. Lietti , J. K. Lim , D. Lincoln , J. Linnemann , V. V. Lipaev , R. Lipton , Y. Liu , A. Lobodenko , M. Lokajicek , R. Lopes de Sa , H. J. Lubatti , R. Luna-Garcia , A. L. Lyon , A. K. A. Maciel , D. Mackin , R. Madar , R. Magana-Villalba , S. Malik , V. L. Malyshev , Y. Maravin , J. Martinez-Ortega , R. McCarthy , C. L. McGivern , M. M. Meijer , A. Melnitchouk , D. Menezes , P. G. Mercadante , M. Merkin , A. Meyer , J. Meyer , F. Miconi , N. K. Mondal , G. S. Muanza , M. Mulhearn , E. Nagy , M. Naimuddin , M. Narain , R. Nayyar , H. A. Neal , J. P. Negret , P. Neustroev , S. F. Novaes , T. Nunnemann , G. Obrant , J. Orduna , N. Osman , J. Osta , G. J. Otero y Garzon , M. Padilla , A. Pal , N. Parashar , V. Parihar , S. K. Park , R. Partridge , N. Parua , A. Patwa , B. Penning , M. Perfilov , Y. Peters , K. Petridis , G. Petrillo , P. Petroff , R. Piegaia , M. -A. Pleier , P. L. M. Podesta-Lerma , V. M. Podstavkov , P. Polozov , A. V. Popov , M. Prewitt , D. Price , N. Prokopenko , J. Qian , A. Quadt , B. Quinn , M. S. Rangel , K. Ranjan , P. N. Ratoff , I. Razumov , P. Renkel , M. Rijssenbeek , I. Ripp-Baudot , F. Rizatdinova , M. Rominsky , A. Ross , C. Royon , P. Rubinov , R. Ruchti , G. Safronov , G. Sajot , P. Salcido , A. Sanchez-Hernandez , M. P. Sanders , B. Sanghi , A. S. Santos , G. Savage , L. Sawyer , T. Scanlon , R. D. Schamberger , Y. Scheglov , H. Schellman , T. Schliephake , S. Schlobohm , C. Schwanenberger , R. Schwienhorst , J. Sekaric , H. Severini , E. Shabalina , V. Shary , A. A. Shchukin , R. K. Shivpuri , V. Simak , V. Sirotenko , P. Skubic , P. Slattery , D. Smirnov , K. J. Smith , G. R. Snow , J. Snow , S. Snyder , S. Soldner-Rembold , L. Sonnenschein , K. Soustruznik , J. Stark , V. Stolin , D. A. Stoyanova , M. Strauss , D. Strom , L. Stutte , L. Suter , P. Svoisky , M. Takahashi , A. Tanasijczuk , M. Titov , V. V. Tokmenin , Y. -T. Tsai , K. Tschann-Grimm , D. Tsybychev , B. Tuchming , C. Tully , L. Uvarov , S. Uvarov , S. Uzunyan , R. Van Kooten , W. M. van Leeuwen , N. Varelas , E. W. Varnes , I. A. Vasilyev , P. Verdier , L. S. Vertogradov , M. Verzocchi , M. Vesterinen , D. Vilanova , P. Vokac , H. D. Wahl , M. H. L. S. Wang , J. Warchol , G. Watts , M. Wayne , M. Weber , J. Weichert , L. Welty-Rieger , A. White , D. Wicke , M. R. J. Williams , G. W. Wilson , M. Wobisch , D. R. Wood , T. R. Wyatt , Y. Xie , R. Yamada , W. -C. Yang , T. Yasuda , Y. A. Yatsunenko , W. Ye , Z. Ye , H. Yin , K. Yip , S. W. Youn , T. Zhao , B. Zhou , J. Zhu , M. Zielinski , D. Zieminska , L. Zivkovic

The top quark pair production cross-section ${\sigma}_{t\bar{t}}$ has been measured in $p\bar{p}$ collisions at center of mass energies of 1.96 TeV using Tevatron Run 2 data. In the begining of Run 2 both CDF and D\O\ $\sigma_{t\bar{t}}$…

High Energy Physics - Experiment · Physics 2007-05-23 S. Cabrera

A search, in e^+e^- collisions, for chargino, neutralino, scalar lepton and scalar quark pair-production is performed, without assuming R-parity conservation in decays, in the case that only one of the coupling constants lambda_ijk or…

High Energy Physics - Experiment · Physics 2012-08-27 L3 Collaboration

The first observation of $\tau$ lepton pair production in ultraperipheral nucleus-nucleus collisions, a pure quantum electrodynamics (QED) process, is presented. The measurement is based on a data sample collected by the CMS experiment at a…

High Energy Physics - Experiment · Physics 2022-05-16 Arash Jofrehei

We examine for representative gaugino-higgsino mixing scenarios slepton-neutralino and slepton-chargino production in deep inelastic ep-scattering at $\sqrt{s}=1.8$ TeV. We find sneutrino-chargino production to be the dominant process with…

High Energy Physics - Phenomenology · Physics 2016-09-01 T. Woehrmann , H. Fraas

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…

High Energy Physics - Phenomenology · Physics 2009-08-25 J. Lopez , D. Nanopoulos , A. Zichichi

We consider the ATLAS and CMS searches for dijet resonances, as well as the ATLAS search for like-sign dimuon pairs at the LHC with 7 TeV center of mass energy. We interpret their exclusions in terms of bounds on the supersymmetric R-parity…

High Energy Physics - Phenomenology · Physics 2013-05-30 H. K. Dreiner , T. Stefaniak

The littlest Higgs model with T-parity predicts the existence of the T-odd particles, which can only be produced in pair. We consider pair production of the T-odd leptons in future high energy linear $e^{+}e^{-}$ collider ($ILC$). Our…

High Energy Physics - Phenomenology · Physics 2008-11-26 Chong-Xing Yue , Nan Zhang , Shi-Hai Zhu

An R-parity violating SUSY model with lepton-number violating couplings $\lambda'_{i33}$, i=2,3 can generate a neutrino mass spectrum that explains the recent results from neutrino oscillation experiments. These R-parity violating couplings…

High Energy Physics - Phenomenology · Physics 2009-09-15 V. Barger , T. Han , S. Hesselbach , D. Marfatia

Single top quark production at the Fermilab Tevatron Run II (a p \bar{p} collider with \sqrt{S} = 2 TeV) proceeds dominantly via two sub-processes, a t-channel W-gluon fusion process, and an s-channel W^* process. We show that these two…

High Energy Physics - Phenomenology · Physics 2016-09-06 Tim Tait , C. --P. Yuan

We study the phenomenology of same sign top pair production at the LHC in a model-independent way. The complete set of dimension six operators involving two top (or anti-top) quarks is introduced and the connection with all possible t- or…

High Energy Physics - Phenomenology · Physics 2015-03-19 Celine Degrande , Jean-Marc Gerard , Christophe Grojean , Fabio Maltoni , Geraldine Servant

A search is presented for $\tau$ slepton pairs produced in proton-proton collisions at a center-of-mass energy of 13 TeV. The search is carried out in events containing two $\tau$ leptons in the final state, on the assumption that each…

High Energy Physics - Experiment · Physics 2020-03-09 CMS Collaboration

Motivated by the shift in experimental attention towards electroweak supersymmetric particle production at the CERN LHC, we update in this paper our precision predictions at next-to-leading order of perturbative QCD matched to resummation…

High Energy Physics - Phenomenology · Physics 2014-02-07 Benjamin Fuks , Michael Klasen , David R. Lamprea , Marcel Rothering

We reviewed CDF and D0 searches for R-parity violation supersymmetry in leptons involved final states using up to 344+-21 pb-1 Tevatron Run II data of ppbar collisions at sqrt{s} = 1.96 TeV. All the results were in good agreement with the…

High Energy Physics - Experiment · Physics 2010-04-22 Shan-Huei Chuang
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