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Related papers: Accessing CKM suppressed top decays at the LHC

200 papers

We present a search for a new heavy particle $M$ produced in association with a top quark, $p\bar{p}\rightarrow t(M \rightarrow \bar{t}q)$ or $p\bar{p}\rightarrow \bar{t}(\bar{M}\rightarrow t\bar{q})$, where $q$ stands for up quarks and…

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

An overview of recent results on top quark properties and interactions is given, obtained using data collected with the CMS and ATLAS experiments during the years 2011 and 2012 at 7 TeV and 8 TeV centre-of-mass energies. Measurements of top…

High Energy Physics - Experiment · Physics 2019-08-13 Carlo Battilana

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

ATLAS has made several measurements of the top quark mass using proton-proton collision data recorded in 2012 at the LHC with a centre-of-mass energy of 8 TeV. Those summarised here include an indirect determination of the top quark pole…

High Energy Physics - Experiment · Physics 2017-11-28 Benjamin Pearson

We present a measurement of the ttbar production cross section multiplied by the branching ratio to tau lepton decaying semihadronically plus jets, at a center of mass energy sqrt{s}=1.96 TeV using 1 fb^(-1) of integrated luminosity…

High Energy Physics - Experiment · Physics 2010-11-02 D0 Collaboration , V. Abazov

At the LHC, a generic supersymmetric cascade can be a source of top quark. Specifically third generation squarks and gluino are the major sources of top quark which could also be boosted. In this article, we have shown that jet substructure…

High Energy Physics - Phenomenology · Physics 2011-09-13 Priyotosh Bandyopadhyay , Biplob Bhattacherjee

Due to a recent more precise evaluation of $V_{ud}$ and $V_{us}$, the unitarity condition of the first row in the Cabibbo-Kobayashi-Maskawa (CKM) matrix: $|V_{ud}|^2 + |V_{us}|^2 + |V_{ub}|^2 = 0.99798 \pm 0.00038$ now stands at a deviation…

High Energy Physics - Phenomenology · Physics 2020-06-24 Kingman Cheung , Wai-Yee Keung , Chih-Ting Lu , Po-Yan Tseng

Recently, the CDF experiment at the Fermilab Tevatron has used complementary methods to make multiple measurements of the singly produced top quark cross section. All analyses use the same dataset with more than 2 fb^-1 of CDF data and…

High Energy Physics - Experiment · Physics 2008-10-10 R. C. Group , C. I. Ciobanu , K. Lannon , C. Plager

The top quark mass measurements are based either on a direct kinematic reconstruction of the top quark decay products or on indirect measurements, where an observable sensitive to the top quark mass, such as the production cross section, is…

High Energy Physics - Experiment · Physics 2024-01-11 Mikael Myllymäki

We present a novel method for measuring $|V_{cb}|$ at the LHC using an advanced boosted-jet tagger to identify "$bc$ signatures". By associating boosted $W \rightarrow bc$ signals with $bc$-matched jets from top-quark decays, we enable an…

High Energy Physics - Phenomenology · Physics 2025-04-04 Yuzhe Zhao , Congqiao Li , Antonios Agapitos , Dawei Fu , Leyun Gao , Yajun Mao , Qiang Li

A search for pair production of heavy scalar leptoquarks (LQs), each decaying into a top quark and a $\tau$ lepton, is presented. The search considers final states with an electron or a muon, one or two $\tau$ leptons that decayed to…

High Energy Physics - Experiment · Physics 2018-09-05 CMS Collaboration

Several observables sensitive to the fragmentation of $b$-quarks into $b$-hadrons are measured using 36 fb${}^{-1}$ of $\sqrt s = 13$ TeV proton-proton collision data collected with the ATLAS detector at the LHC. Jets containing $b$-hadrons…

High Energy Physics - Experiment · Physics 2022-09-13 ATLAS Collaboration

In March 2009, the DZero Collaboration first observed the electroweak production of single top quarks at 5 sigma significance. We measured the cross section for the combined s-channel and t-channel production modes, and set a lower limit on…

High Energy Physics - Experiment · Physics 2019-08-13 A. P. Heinson

We propose to extract the electric and weak dipole moments of the top quark via $t\bar t\gamma$ and $t\bar t Z$ productions at the CERN LHC. With the large numbers of events available at the LHC, these dipole moments can be measured to the…

High Energy Physics - Phenomenology · Physics 2007-05-23 Hong-Yi Zhou

A measurement of the top-quark mass is presented using Tevatron data from proton-antiproton collisions at center-of-mass energy $\sqrt{s}=1.96$ TeV collected with the CDF II detector. Events are selected from a sample of candidates for…

High Energy Physics - Experiment · Physics 2011-10-17 CDF Collaboration , T. Aaltonen , B. Álvarez Gonzálezv , S. Amerio , D. Amidei , A. Anastassov , A. Annovi , J. Antos , G. Apollinari , J. A. Appel , A. Apresyan , T. Arisawa , A. Artikov , J. Asaadi , W. Ashmanskas , B. Auerbach , A. Aurisano , F. Azfar , W. Badgett , A. Barbaro-Galtieri , V. E. Barnes , B. A. Barnett , P. Barriaee , P. Bartos , M. Baucecc , G. Bauer , F. Bedeschi , D. Beecher , S. Behari , G. Bellettinidd , J. Bellinger , D. Benjamin , A. Beretvas , A. Bhatti , M. Binkley , D. Bisellocc , I. Bizjakii , K. R. Bland , C. Blocker , B. Blumenfeld , A. Bocci , A. Bodek , D. Bortoletto , J. Boudreau , A. Boveia , B. Braua , L. Brigliadoribb , A. Brisuda , C. Bromberg , E. Brucken , M. Bucciantoniodd , J. Budagov , H. S. Budd , S. Budd , K. Burkett , G. Busettocc , P. Bussey , A. Buzatu , S. Cabrerax , C. Calancha , S. Camarda , M. Campanelli , M. Campbell , F. Canelli , A. Canepa , B. Carls , D. Carlsmith , R. Carosi , S. Carrillok , S. Carron , B. Casal , M. Casarsa , A. Castrobb , P. Catastini , D. Cauz , V. Cavaliereee , M. Cavalli-Sforza , A. Cerrif , L. Cerritoq , Y. C. Chen , M. Chertok , G. Chiarelli , G. Chlachidze , F. Chlebana , K. Cho , D. Chokheli , J. P. Chou , W. H. Chung , Y. S. Chung , C. I. Ciobanu , M. A. Ciocciee , A. Clark , D. Clark , G. Compostellacc , M. E. Convery , J. Conway , M. Corbo , M. Cordelli , C. A. Cox , D. J. Cox , F. Cresciolidd , C. Cuenca Almenar , J. Cuevasv , R. Culbertson , D. Dagenhart , N. d'Ascenzot , M. Datta , P. de Barbaro , S. De Cecco , G. De Lorenzo , M. Dell'Orsodd , C. Deluca , L. Demortier , J. Dengc , M. Deninno , F. Devoto , M. d'Erricocc , A. Di Cantodd , B. Di Ruzza , J. R. Dittmann , M. D'Onofrio , S. Donatidd , P. Dong , T. Dorigo , K. Ebina , A. Elagin , A. Eppig , R. Erbacher , D. Errede , S. Errede , N. Ershaidataa , R. Eusebi , H. C. Fang , S. Farrington , M. Feindt , J. P. Fernandez , C. Ferrazzaff , R. Field , G. Flanaganr , R. Forrest , M. J. Frank , M. Franklin , J. C. Freeman , I. Furic , M. Gallinaro , J. Galyardt , J. E. Garcia , A. F. Garfinkel , P. Garosiee , H. Gerberich , E. Gerchtein , S. Giagugg , V. Giakoumopoulou , P. Giannetti , K. Gibson , C. M. Ginsburg , N. Giokaris , P. Giromini , M. Giunta , G. Giurgiu , V. Glagolev , D. Glenzinski , M. Gold , D. Goldin , N. Goldschmidt , A. Golossanov , G. Gomez , G. Gomez-Ceballos , M. Goncharov , O. González , I. Gorelov , A. T. Goshaw , K. Goulianos , A. Gresele , S. Grinstein , C. Grosso-Pilcher , R. C. Group , J. Guimaraes da Costa , Z. Gunay-Unalan , C. Haber , S. R. Hahn , E. Halkiadakis , A. Hamaguchi , J. Y. Han , F. Happacher , K. Hara , D. Hare , M. Hare , R. F. Harr , K. Hatakeyama , C. Hays , M. Heck , J. Heinrich , M. Herndon , S. Hewamanage , D. Hidas , A. Hocker , W. Hopkinsg , D. Horn , S. Hou , R. E. Hughes , M. Hurwitz , U. Husemann , N. Hussain , M. Hussein , J. Huston , G. Introzzi , M. Iorigg , A. Ivanovo , E. James , D. Jang , B. Jayatilaka , E. J. Jeon , M. K. Jha , S. Jindariani , W. Johnson , M. Jones , K. K. Joo , S. Y. Jun , T. R. Junk , T. Kamon , P. E. Karchin , Y. Katon , W. Ketchum , J. Keung , V. Khotilovich , B. Kilminster , D. H. Kim , H. S. Kim , H. W. Kim , J. E. Kim , M. J. Kim , S. B. Kim , S. H. Kim , Y. K. Kim , N. Kimura , S. Klimenko , K. Kondo , D. J. Kong , J. Konigsberg , A. Korytov , A. V. Kotwal , M. Kreps , J. Kroll , D. Krop , N. Krumnackl , M. Kruse , V. Krutelyovd , T. Kuhr , M. Kurata , S. Kwang , A. T. Laasanen , S. Lami , S. Lammel , M. Lancaster , R. L. Lander , K. Lannonu , A. Lath , G. Latinoee , I. Lazzizzera , T. LeCompte , E. Lee , H. S. Lee , J. S. Lee , S. W. Leew , S. Leodd , S. Leone , J. D. Lewis , C. -J. Lin , J. Linacre , M. Lindgren , E. Lipeles , A. Lister , D. O. Litvintsev , C. Liu , Q. Liu , T. Liu , S. Lockwitz , N. S. Lockyer , A. Loginov , D. Lucchesicc , J. Lueck , P. Lujan , P. Lukens , G. Lungu , J. Lys , R. Lysak , R. Madrak , K. Maeshima , K. Makhoul , P. Maksimovic , S. Malik , G. Mancab , A. Manousakis-Katsikakis , F. Margaroli , C. Marino , M. Martínez , R. Martínez-Ballarín , P. Mastrandrea , M. Mathis , M. E. Mattson , P. Mazzanti , K. S. McFarland , P. McIntyre , R. McNultyi , A. Mehta , P. Mehtala , A. Menzione , C. Mesropian , T. Miao , D. Mietlicki , A. Mitra , H. Miyake , S. Moed , N. Moggi , M. N. Mondragonk , C. S. Moon , R. Moore , M. J. Morello , J. Morlock , P. Movilla Fernandez , A. Mukherjee , Th. Muller , P. Murat , M. Mussinibb , J. Nachtmanm , Y. Nagai , J. Naganoma , I. Nakano , A. Napier , J. Nett , C. Neuz , M. S. Neubauer , J. Nielsene , L. Nodulman , O. Norniella , E. Nurse , L. Oakes , S. H. Oh , Y. D. Oh , I. Oksuzian , T. Okusawa , R. Orava , L. Ortolan , S. Pagan Grisocc , C. Pagliarone , E. Palenciaf , V. Papadimitriou , A. A. Paramonov , J. Patrick , G. Paulettahh , M. Paulini , C. Paus , D. E. Pellett , A. Penzo , T. J. Phillips , G. Piacentino , E. Pianori , J. Pilot , K. Pitts , C. Plager , L. Pondrom , K. Potamianos , O. Poukhov , F. Prokoshiny , A. Pronko , F. Ptohosh , E. Pueschel , G. Punzidd , J. Pursley , A. Rahaman , V. Ramakrishnan , N. Ranjan , I. Redondo , P. Renton , M. Rescigno , F. Rimondibb , L. Ristori , A. Robson , T. Rodrigo , T. Rodriguez , E. Rogers , S. Rolli , R. Roser , M. Rossi , F. Ruffiniee , A. Ruiz , J. Russ , V. Rusu , A. Safonov , W. K. Sakumoto , L. Santihh , L. Sartori , K. Sato , V. Savelievt , A. Savoy-Navarro , P. Schlabach , A. Schmidt , E. E. Schmidt , M. P. Schmidt , M. Schmitt , T. Schwarz , L. Scodellaro , A. Scribanoee , F. Scuri , A. Sedov , S. Seidel , Y. Seiya , A. Semenov , F. Sforzadd , A. Sfyrla , S. Z. Shalhout , T. Shears , P. F. Shepard , M. Shimojimas , S. Shiraishi , M. Shochet , I. Shreyber , A. Simonenko , P. Sinervo , A. Sissakian , K. Sliwa , J. R. Smith , F. D. Snider , A. Soha , S. Somalwar , V. Sorin , P. Squillacioti , M. Stanitzki , R. St. Denis , B. Stelzer , O. Stelzer-Chilton , D. Stentz , J. Strologas , G. L. Strycker , Y. Sudo , A. Sukhanov , I. Suslov , K. Takemasa , Y. Takeuchi , J. Tang , M. Tecchio , P. K. Teng , J. Thomg , J. Thome , G. A. Thompson , E. Thomson , P. Ttito-Guzmán , S. Tkaczyk , D. Toback , S. Tokar , K. Tollefson , T. Tomura , D. Tonelli , S. Torre , D. Torretta , P. Totarohh , M. Trovatoff , Y. Tu , N. Turiniee , F. Ukegawa , S. Uozumi , A. Varganov , E. Vatagaff , F. Vázquez , G. Velev , C. Vellidis , M. Vidal , I. Vila , R. Vilar , M. Vogel , G. Volpidd , P. Wagner , R. L. Wagner , T. Wakisaka , R. Wallny , S. M. Wang , A. Warburton , D. Waters , M. Weinberger , W. C. Wester , B. Whitehouse , D. Whitesonc , A. B. Wicklund , E. Wicklund , S. Wilbur , F. Wick , H. H. Williams , J. S. Wilson , P. Wilson , B. L. Winer , P. Wittichg , S. Wolbers , H. Wolfe , T. Wright , X. Wu , Z. Wu , K. Yamamoto , J. Yamaoka , T. Yang , U. K. Yangp , Y. C. Yang , W. -M. Yao , G. P. Yeh , K. Yim , J. Yoh , K. Yorita , T. Yoshidaj , G. B. Yu , I. Yu , S. S. Yu , J. C. Yun , A. Zanetti , Y. Zeng , S. Zucchelli

We present a feasibility study of top-quark mass measurement using the energy distribution of a lepton from a W boson in a top quark decay in pp collisions at the LHC. The proposed method requires only the lepton energy distribution at the…

High Energy Physics - Experiment · Physics 2018-01-17 Seo Hyun An , Sayaka Kawabata , Tae Jeong Kim

We review the prospects of measurements of the CKM matrix elements corresponding to the first two generations of quarks, as well as measurements of leptonic and semileptonic charm meson decays at LHCb. We review the status of searches for…

High Energy Physics - Experiment · Physics 2019-01-16 Adam C. S. Davis

The mass of the top quark is measured using a sample of t t-bar candidate events with one electron or muon and at least four jets in the final state, collected by CMS in pp collisions at sqrt(s) = 7 TeV at the LHC. A total of 5174 candidate…

High Energy Physics - Experiment · Physics 2013-03-19 The CMS Collaboration

A comprehensive extension of the ordinary 2-Higgs Doublet Model (2HDM), supplemented by Vector-Like Quarks (VLQs), in the "alignment limit" is presented. In such a scenario, we study the possibility that Large Hadron Collider (LHC) searches…

High Energy Physics - Phenomenology · Physics 2025-01-13 Abdesslam Arhrib , Rachid Benbrik , Mohammed Boukidi , Bouzid Manaut , Stefano Moretti

The branching fraction for the decays of gluinos to third generation quarks is expected to be enhanced in classes of supersymmetric models where either third generation squarks are lighter than other squarks, or in mixed-higgsino dark…

High Energy Physics - Phenomenology · Physics 2008-11-26 R. H. K. Kadala , P. G. Mercadante , J. K. Mizukoshi , Xerxes Tata