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Related papers: Top Mass Measurement at CLIC at 500 GeV

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We present a measurement of the top quark mass using a sample of t-tbar decays into an electron or a muon, a neutrino, and four jets. The data were collected in p-pbar collisions at sqrt(s)=1.8 TeV with the Collider Detector at Fermilab and…

High Energy Physics - Experiment · Physics 2010-05-12 F. Abe

The D0 collaboration has performed a measurement of the top quark mass based on six candidate events for the process t tbar -> b W+ bbar W-, where the W bosons decay to e nu or mu nu. This sample was collected during an exposure of the D0…

High Energy Physics - Experiment · Physics 2008-11-26 B. Abbott

The threshold scan at future lepton colliders is the most precise known method to determine the top quark mass (well below 100 MeV), a fundamental parameter of the Standard Model that co-determines the stability properties of the…

High Energy Physics - Phenomenology · Physics 2018-11-12 Jürgen Reuter , Bijan Chokoufé Nejad , Andre Hoang , Wolfgang Kilian , Maximilian Stahlhofen , Thomas Teubner , Christian Weiss

We present recent measurements of the top quark mass by the ATLAS and CMS experiments in the $\mathrm{t}\overline{\mathrm{t}}$ lepton+jets, all-hadronic, and dilepton channels. In addition, we present a measurement using a topology enriched…

High Energy Physics - Experiment · Physics 2015-12-09 Nathan Mirman

We report two measurements of the top quark mass M_top using the CDF II detector at the Fermilab Tevatron in a 318 pb^-1 data sample observed in the lepton + jets final state. One method uses an event-based likelihood technique resulting in…

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

Lepton colliders are considered as options to complement and to extend the physics programme at the Large Hadron Collider. The Compact Linear Collider (CLIC) is an $e^+e^-$ collider under development aiming at centre-of-mass energies of up…

Instrumentation and Detectors · Physics 2014-01-14 C. Adloff , J. -J. Blaising , M. Chefdeville , C. Drancourt , R. Gaglione , N. Geffroy , Y. Karyotakis , I. Koletsou , J. Prast , G. Vouters , J. Repond , J. Schlereth , J. Smith , L. Xia , E. Baldolemar , J. Li , S. T. Park , M. Sosebee , A. P. White , J. Yu , G. Eigen , M. A. Thomson , D. R. Ward , D. Benchekroun , A. Hoummada , Y. Khoulaki , J. Apostolakis , D. Dannheim , A. Dotti , K. Elsener , G. Folger , C. Grefe , V. Ivantchenko , M. Killenberg , W. Klempt , E. van der Kraaij , C. B. Lam , L. Linssen , A. -I. Lucaci-Timoce , A. Muennich , S. Poss , A. Ribon , A. Sailer , D. Schlatter , J. Strube , V. Uzhinskiy , C. Carloganu , P. Gay , S. Manen , L. Royer , M. Tytgat , N. Zaganidis , G. C. Blazey , A. Dyshkant , J. G. R. Lima , V. Zutshi , J. -Y. Hostachy , L. Morin , U. Cornett , D. David , A. Ebrahimi , G. Falley , N. Feege , K. Gadow , P. Goettlicher , C. Guenter , O. Hartbrich , B. Hermberg , S. Karstensen , F. Krivan , K. Krueger , S. Lu , B. Lutz , S. Morozov , V. Morgunov , C. Neubueser , M. Reinecke , F. Sefkow , P. Smirnov , M. Terwort , E. Garutti , S. Laurien , I. Marchesini , M. Matysek , M. Ramilli , K. Briggl , P. Eckert , T. Harion , H. -Ch. Schultz-Coulon , W. Shen , R. Stamen , B. Bilki , E. Norbeck , D. Northacker , Y. Onel , G. W. Wilson , K. Kawagoe , Y. Sudo , T. Yoshioka , P. D. Dauncey , M. Wing , F. Salvatore , E. Cortina Gil , S. Mannai , G. Baulieu , P. Calabria , L. Caponetto , C. Combaret , R. Della Negra , G. Grenier , R. Han , J-C. Ianigro , R. Kieffer , I. Laktineh , N. Lumb , H. Mathez , L. Mirabito , A. Petrukhin , A. Steen , W. Tromeur , M. Vander Donckt , Y. Zoccarato , E. Calvo Alamillo , M. -C. Fouz , J. Puerta-Pelayo , F. Corriveau , B. Bobchenko , M. Chadeeva , M. Danilov , A. Epifantsev , O. Markin , R. Mizuk , E. Novikov , V. Popov , V. Rusinov , E. Tarkovsky , N. Kirikova , V. Kozlov , P. Smirnov , Y. Soloviev , D. Besson , P. Buzhan , A. Ilyin , V. Kantserov , V. Kaplin , A. Karakash , E. Popova , V. Tikhomirov , C. Kiesling , K. Seidel , F. Simon , C. Soldner , M. Szalay , M. Tesar , L. Weuste , M. S. Amjad , J. Bonis , S. Callier , S. Conforti di Lorenzo , P. Cornebise , Ph. Doublet , F. Dulucq , J. Fleury , T. Frisson , N. van der Kolk , H. Li , G. Martin-Chassard , F. Richard , Ch. de la Taille , R. Poeschl , L. Raux , J. Rouene , N. Seguin-Moreau , M. Anduze , V. Balagura , V. Boudry , J-C. Brient , R. Cornat , M. Frotin , F. Gastaldi , E. Guliyev , Y. Haddad , F. Magniette , G. Musat , M. Ruan , T. H. Tran , H. Videau , B. Bulanek , J. Zacek , J. Cvach , P. Gallus , M. Havranek , M. Janata , J. Kvasnicka , D. Lednicky , M. Marcisovsky , I. Polak , J. Popule , L. Tomasek , M. Tomasek , P. Ruzicka , P. Sicho , J. Smolik , V. Vrba , J. Zalesak , B. Belhorma , H. Ghazlane , K. Kotera , T. Takeshita , S. Uozumi , S. Chang , A. Khan , D. H. Kim , D. J. Kong , Y. D. Oh , M. Goetze , J. Sauer , S. Weber , C. Zeitnitz

A top-quark reconstruction method for CLIC is described. The reconstructed events are used to measure the e+ e- -> t \bar{t} cross-section as well as the forward-backward asymmetry. The results suggest that the relative measurement accuracy…

High Energy Physics - Experiment · Physics 2007-05-23 Laura Salmi

We study the sensitivity of possible CLIC and FCC-ee measurements of light-by-light scattering to old and new physics, including the Heisenberg-Euler Lagrangian in the Standard Model with possible contributions from loops of additional…

High Energy Physics - Phenomenology · Physics 2022-07-26 John Ellis , Nick E. Mavromatos , Philipp Roloff , Tevong You

The physics potential is briefly summarized for an e+e- linear collider operating at center-of-mass energies up to \sqrt{s} = 1 TeV and delivering integrated luminosities up to \int L = 0.5 ab^(-1) in one to two years. This machine will…

High Energy Physics - Phenomenology · Physics 2007-05-23 P. M. Zerwas

The FCC (Future Circular Collider) study represents a vision for the next large project in high energy physics, comprising an 80-100 km tunnel that can house a future 100 TeV hadron collider. The study also includes a high luminosity e+e-…

We employ a top-quark mass measurement technique in the dilepton channel with {\it in situ} jet energy scale calibration. Three variables having different jet energy scale dependences are used simultaneously to extract not only the…

High Energy Physics - Phenomenology · Physics 2012-09-19 Hyun Su Lee

Future e^+ e^- linear colliders will enable us to determine the top quark mass with high accuracy from the measurement of the 1S peak position of (remnant of) toponium. The estimated statistical error in this measurement is about 50 MeV…

High Energy Physics - Phenomenology · Physics 2007-05-23 Y. Kiyo

In the Standard Model (SM), flavour changing neutral current (FCNC) top decays, possible at loop level only, are very strongly suppressed. Observation of any such decay would be a direct signature of physics beyond the SM. Large…

High Energy Physics - Experiment · Physics 2017-09-13 Aleksander Filip Żarnecki

The International Linear Collider (ILC) will be able to precisely measure the electroweak couplings of the top in e+e- -> tt~. We compare the limits which can be achieved at the ILC with those which can be obtained in tt~gamma$ and tt~Z…

High Energy Physics - Phenomenology · Physics 2007-05-23 U. Baur

We report on the feasibility of the direct measurement of the top Yukawa coupling g_t at the International Linear Collider (ILC) during its first phase of operation with a center-of-mass energy of 500 GeV. The signal and background models…

High Energy Physics - Phenomenology · Physics 2011-08-11 Ryo Yonamine , Katsumasa Ikematsu , Tomohiko Tanabe , Keisuke Fujii , Yuichiro Kiyo , Yukinari Sumino , Hiroshi Yokoya

We show how to determine the electric and weak dipole moments of the top quark simultaneously and independently from $e^+e^-\to t\bar t$ at $\sqrt{s}=500$ GeV NLC. To obtain the best accuracies with which the dipole moments can be measured,…

High Energy Physics - Phenomenology · Physics 2009-10-31 Hong-Yi Zhou

We report a measurement of the top quark mass, M_t, in the dilepton decay channel of $t\bar{t}\to b\ell'^{+}\nu_{\ell'}\bar{b}\ell^{-}\bar{\nu}_{\ell}$ using an integrated luminosity of 1.0 fb^{-1} of p\bar{p} collisions collected with the…

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

We review the most recent measurements of the top quark mass using data collected by the CDF experiment at the Tevatron 1.96 TeV ppbar collider. The mass measurements are performed in all main decay modes of the produced ttbar pairs using…

High Energy Physics - Experiment · Physics 2010-11-11 N. van Remortel

We report the first measurement of the top quark mass using the decay length technique in ppbar collisions at a center-of-mass energy of 1.96 TeV. This technique uses the measured flight distance of the b hadron to infer the mass of the top…

High Energy Physics - Experiment · Physics 2010-05-12 A. Abulencia et al.

This contribution to LCWS2016 presents recent developments within the CLICdp collaboration. An updated scenario for the staged operation of CLIC has been published; the accelerator will operate at 380 GeV, 1.5 TeV and 3 TeV. The lowest…

Instrumentation and Detectors · Physics 2019-08-13 Naomi van der Kolk