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Related papers: Top-Squark Study at a Future e^+e^- Linear Collide…

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We study the potential of high-energy linear $e^+e^-$ colliders for the production of gluino pairs within the Minimal Supersymmetric Standard Model (MSSM). In this model, the process $e^+e^-\to\tilde{g}\tilde{g}$ is mediated by quark/squark…

High Energy Physics - Phenomenology · Physics 2011-03-23 Stefan Berge , Michael Klasen

It is shown how the fundamental gaugino and higgsino parameters of the chargino and neutralino system in the MSSM can completely be determined in high--precision experiments at e+e- linear colliders even if in their initial phase only the…

High Energy Physics - Phenomenology · Physics 2007-05-23 Jan Kalinowski

We analyze the production of neutral Higgs particles in association with the supersymmetric scalar partners of the third generation quarks at future high--energy hadron colliders [upgraded Tevatron, LHC] and $e^+e^-$ linear machines…

High Energy Physics - Phenomenology · Physics 2009-10-31 A. Djouadi , J. -L. Kneur , G. Moultaka

This paper presents a search for top-squark pair production in final states with a top quark, a charm quark and missing transverse momentum. The data were collected with the ATLAS detector during LHC Run 2 and corresponds to an integrated…

High Energy Physics - Experiment · Physics 2024-08-23 ATLAS Collaboration

We report the result of a search for the pair production of the lightest supersymmetric partner of the top quark ($\tilde{t}_1$) in $p\bar{p}$ collisions at a center-of-mass energy of 1.96 TeV at the Fermilab Tevatron collider corresponding…

High Energy Physics - Experiment · Physics 2011-02-01 V. M. Abazov , B. Abbott , M. Abolins , B. S. Acharya , M. Adams , T. Adams , G. D. Alexeev , G. Alkhazov , A. Altona , G. Alverson , G. A. Alves , L. S. Ancu , M. Aoki , Y. Arnoud , M. Arov , A. Askew , B. Åsman , O. Atramentov , 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 , S. Beale , A. Bean , M. Begalli , M. Begel , C. Belanger-Champagne , L. Bellantoni , S. B. Beri , G. Bernardi , R. Bernhard , I. Bertram , M. Besançon , R. Beuselinck , V. A. Bezzubov , P. C. Bhat , V. Bhatnagar , G. Blazey , S. Blessing , K. Bloom , A. Boehnlein , D. Boline , T. A. Bolton , E. E. Boos , G. Borissov , T. Bose , A. Brandt , O. Brandt , R. Brock , G. Brooijmans , A. Bross , D. Brown , J. Brown , X. B. Bu , D. Buchholz , M. Buehler , V. Buescher , V. Bunichev , S. Burdinb , T. H. Burnett , C. P. Buszello , B. Calpas , E. Camacho-Pérez , M. A. Carrasco-Lizarraga , B. C. K. Casey , H. Castilla-Valdez , S. Chakrabarti , D. Chakraborty , K. M. Chan , A. Chandra , G. Chen , S. Chevalier-Théry , D. K. Cho , S. W. Cho , S. Choi , B. Choudhary , T. Christoudias , S. Cihangir , D. Claes , J. Clutter , M. Cooke , W. E. Cooper , M. Corcoran , F. Couderc , M. -C. Cousinou , A. Croc , D. Cutts , M. Ćwiok , A. Das , G. Davies , K. De , S. J. de Jong , E. De La Cruz-Burelo , F. Déliot , M. Demarteau , 47 R. Demina , D. Denisov , S. P. Denisov , S. Desai , K. DeVaughan , H. T. Diehl , M. Diesburg , 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 , S. Eno , 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 , T. Gadfort , A. Garcia-Bellido , V. Gavrilov , P. Gay , W. Geist , 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. Grünendahl , M. W. Grünewald , F. Guo , J. Guo , G. Gutierrez , P. Gutierrez , A. Haasc , 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 , S. Hossain , Z. Hubacek , N. Huske , V. Hynek , I. Iashvili , R. Illingworth , A. S. Ito , S. Jabeen , M. Jaffré , S. Jain , D. Jamin , R. Jesik , K. Johns , M. Johnson , D. Johnston , A. Jonckheere , P. Jonsson , J. Joshi , A. Justed , K. Kaadze , E. Kajfasz , D. Karmanov , P. A. Kasper , I. Katsanos , R. Kehoe , S. Kermiche , N. Khalatyan , A. Khanov , A. Kharchilava , Y. N. Kharzheev , D. Khatidze , M. H. Kirby , J. M. Kohli , A. V. Kozelov , J. Kraus , A. Kumar , A. Kupco , T. Kurča , V. A. Kuzmin , J. Kvita , S. Lammers , G. Landsberg , P. Lebrun , H. S. Lee , S. W. Lee , W. M. Lee , J. Lellouch , L. Li , Q. Z. Li , S. M. Lietti , J. K. Lim , D. Lincoln , J. Linnemann , V. V. Lipaev , R. Lipton , Y. Liu , Z. Liu , A. Lobodenko , M. Lokajicek , P. Love , H. J. Lubatti , R. Luna-Garciae , A. L. Lyon , A. K. A. Maciel , D. Mackin , R. Madar , R. Magaña-Villalba , S. Malik , V. L. Malyshev , Y. Maravin , J. Martínez-Ortega , R. McCarthy , C. L. McGivern , M. M. Meijer , A. Melnitchouk , D. Menezes , P. G. Mercadante , M. Merkin , A. Meyer , J. Meyer , 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 Garzón , M. Owen , M. Padilla , M. Pangilinan , N. Parashar , V. Parihar , S. K. Park , J. Parsons , R. Partridgec , N. Parua , A. Patwa , B. Penning , M. Perfilov , K. Peters , Y. Peters , G. Petrillo , P. Pétroff , R. Piegaia , J. Piper , M. -A. Pleier , P. L. M. Podesta-Lermaf , V. M. Podstavkov , M. -E. Pol , P. Polozov , A. V. Popov , M. Prewitt , D. Price , S. Protopopescu , J. Qian , A. Quadt , B. Quinn , M. S. Rangel , K. Ranjan , P. N. Ratoff , I. Razumov , P. Renkel , P. Rich , M. Rijssenbeek , I. Ripp-Baudot , F. Rizatdinova , M. Rominsky , C. Royon , P. Rubinov , R. Ruchti , G. Safronov , G. Sajot , A. Sánchez-Hernández , 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. Söldner-Rembold , L. Sonnenschein , A. Sopczak , M. Sosebee , K. Soustruznik , B. Spurlock , J. Stark , V. Stolin , D. A. Stoyanova , E. Strauss , M. Strauss , D. Strom , L. Stutte , P. Svoisky , M. Takahashi , A. Tanasijczuk , W. Taylor , M. Titov , V. V. Tokmenin , D. Tsybychev , B. Tuchming , C. Tully , P. M. Tuts , 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. Vint , P. Vokac , H. D. Wahl , M. H. L. S. Wang , J. Warchol , G. Watts , M. Wayne , M. Weberg , L. Welty-Rieger , M. Wetstein , A. White , D. Wicke M. R. J. Williams , G. W. Wilson , S. J. Wimpenny , M. Wobisch , D. R. Wood , T. R. Wyatt , Y. Xie , C. Xu , S. Yacoob , R. Yamada , W. -C. Yang , T. Yasuda , Y. A. Yatsunenko , Z. Ye , H. Yin , K. Yip , H. D. Yoo , S. W. Youn , J. Yu , S. Zelitch , T. Zhao , B. Zhou , J. Zhu , M. Zielinski , D. Zieminska , L. Zivkovic

If supersymmetry (SUSY) is realized at the electroweak scale, its underlying structure and breaking mechanism may be explored with great precision by a future linear $e^+ e^-$ collider (LC) with a clean environment, tunable collision…

High Energy Physics - Phenomenology · Physics 2017-08-23 S. Y. Choi

In the context of the Minimal Supersymmetric extension of the Standard Model, we analyze the production at future high-energy $e^+e^-$ colliders of second and third generation scalar leptons as well as scalar quarks in association with…

High Energy Physics - Phenomenology · Physics 2009-01-07 Aseshkrishna Datta , Abdelhak Djouadi

In an R-parity violating supersymmetric scenario, the lightest neutralino $\tilde \chi^0_1$ is no longer a stable particle. We calculate the branching ratio for the decay mode $\tilde \chi^0_1 \longrightarrow \nu \gamma$ which occurs at the…

High Energy Physics - Phenomenology · Physics 2009-10-31 Biswarup Mukhopadhyaya , Sourov Roy

We discuss the decays of the lightest scalar top quark $\tilde{t}_1$ in the Minimal Supersymmetric extension of the Standard Model and show that the final state $b\tau \nu_\tau \chi_1^0$, where $\chi_1^0$ is the lightest supersymmetric…

High Energy Physics - Phenomenology · Physics 2009-11-07 A. Djouadi , M. Guchait , Y. Mambrini

We study the potential of the LHC accelerator, and a future 33 TeV proton collider, to observe the production of a light top squark pair in association with the lightest Higgs boson (${\tilde t}_1 {\tilde t}_1 h_1$), as predicted by the…

High Energy Physics - Phenomenology · Physics 2017-12-20 Siba Prasad Das , Jorge Fraga , Carlos Avila

Pair production of light top squarks at the 8-TeV LHC can be used to probe the gaugino-Higgsino sector of the Minimal Supersymmetric Standard Model. The case where the lightest neutralino is a mixture of Bino and Higgsino, satisfying the…

High Energy Physics - Phenomenology · Physics 2013-05-15 Bhaskar Dutta , Teruki Kamon , Nikolay Kolev , Kuver Sinha , Kechen Wang , Sean Wu

Within the framework of the Next-To-Minimal Supersymmetric Standard Model (NMSSM) we study neutralino production $e^+e^- \longrightarrow \tilde{\chi}^0_i \tilde{\chi}^0_j$ ($i,j=1,\ldots ,5$) at center-of-mass energies between 100 and 600…

High Energy Physics - Phenomenology · Physics 2014-11-17 F. Franke , H. Fraas

Decays of the lightest neutralino are studied in R_p-violating models with operators lambda^{prime} L Q D^c and lambda L L E^c involving third-generation matter fields and with dominant lambda^{prime} and lambda couplings. Generalizations…

High Energy Physics - Phenomenology · Physics 2009-11-07 F. Borzumati , R. M. Godbole , J. L. Kneur , F. Takayama

The complete matrix element for $e^+e^-\rightarrow b\bar b W^+W^-$ is computed at tree-level within the Minimal Supersymmetric Standard Model. Rates of interest to phenomenological analyses at the Next Linear Collider are given. In…

High Energy Physics - Phenomenology · Physics 2007-05-23 Stefano Moretti

The Minimal Supersymmetric Standard Model opens the possibility of electroweak baryogenesis provided that the light scalar top quark (stop) is lighter than the top quark. In addition, the lightest neutralino is an ideal candidate to explain…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. Carena , A. Finch , A. Freitas , C. Milstene , H. Nowak , A. Sopczak

Assuming gauge-mediated supersymmetry breaking, we simulate precision measurements of fundamental parameters at a 500 GeV e+e- linear collider in the scenario where a neutralino is the next-to-lightest supersymmetric particle. Information…

High Energy Physics - Phenomenology · Physics 2007-05-23 Sandro Ambrosanio , Grahame A. Blair

A high energy $e^+e^-$ linear collider (NLC) is an excellent tool for studying the properties of the top quark. In this talk I review some of the theory of top quark production and decay in $e^+e^-$ collisions both at threshold and in the…

High Energy Physics - Phenomenology · Physics 2007-05-23 Carl R. Schmidt

Up to now, almost all discussion of supersymmetry at future colliders has been concerned with particle searches. However, if candidates for supersymmetric particles are found, there is much more that we will want to know about them.…

High Energy Physics - Phenomenology · Physics 2016-09-01 J. L. Feng , H. Murayama , M. E. Peskin , X. Tata

We propose several T-odd asymmetries in the decay chains of the top squarks $\tilde t_m \to t \tilde \chi^0_k$ and $t\to bW^+\to bl\nu$ and $\tilde\chi^0_k \to l^\pm\tilde l_n^\mp \to l^\pm l^\mp\tilde\chi^0_1$, for $l =e,\mu,\tau$. We…

High Energy Physics - Phenomenology · Physics 2009-11-10 A. Bartl , E. Christova , K. Hohenwarter-Sodek , T. Kernreiter

We provide the next-to-leading order (NLO) predictions for the neutralino pair production via quark-antiquark annihilation and gluon-gluon fusion at the CERN Large Hadron Collider, focusing on the lightest neutralino which is likely to be…

High Energy Physics - Phenomenology · Physics 2014-04-16 M. Demirci , A. I. Ahmadov