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Related papers: The D0 Run IIb Luminosity Measurement

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We present a measurement of the elastic differential cross section $d\sigma(p\bar{p}\rightarrow p\bar{p})/dt$ as a function of the four-momentum-transfer squared t. The data sample corresponds to an integrated luminosity of $\approx 31…

High Energy Physics - Experiment · Physics 2013-05-30 D0 Collaboration , V. M. Abazov , B. Abbott , B. S. Acharya , M. Adams , T. Adams , G. D. Alexeev , G. Alkhazov , A. Alton , G. Alverson , G. A. Alves , M. Aoki , A. Askew , S. Atkins , K. Augsten , C. Avila , 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 , L. Bellantoni , S. B. Beri , G. Bernardi , R. Bernhard , I. Bertram , M. Besançon , 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 , C. P. Buszello , E. Camacho-Pérez , W. Carvalho , B. C. K. Casey , H. Castilla-Valdez , S. Caughron , S. Chakrabarti , D. Chakraborty , K. M. Chan , A. Chandra , E. Chapon , G. Chen , S. Chevalier-Théry , 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 , C. De Oliveira Martins , F. Déliot , R. Demina , D. Denisov , S. P. Denisov , S. Desai , C. Deterre , K. DeVaughan , H. T. Diehl , M. Diesburg , P. F. Ding , A. Dominguez , 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 , L. Feng , T. Ferbel , F. Fiedler , F. Filthaut , W. Fisher , H. E. Fisk , M. Fortner , H. Fox , S. Fuess , A. Garcia-Bellido , J. A. García-González , G. A. García-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 , E. M. Gregores , G. Grenier , Ph. Gris , J. -F. Grivaz , A. Grohsjean , S. Grünendahl , M. W. Grünewald , 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 , I. Howley , Z. Hubacek , V. Hynek , I. Iashvili , Y. Ilchenko , R. Illingworth , A. S. Ito , S. Jabeen , M. Jaffré , A. Jayasinghe , R. Jesik , K. Johns , E. Johnson , 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 , I. Kiselevich , J. M. Kohli , A. V. Kozelov , J. Kraus , S. Kulikov , A. Kumar , A. Kupco , T. Kurča , 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 , J. K. Lim , D. Lincoln , J. Linnemann , V. V. Lipaev , R. Lipton , H. Liu , Y. Liu , A. Lobodenko , M. Lokajicek , R. Lopes de Sa , H. J. Lubatti , R. Luna-Garcia , A. L. Lyon , A. K. A. Maciel , 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 , L. Mendoza , D. Menezes , P. G. Mercadante , M. Merkin , A. Meyer , J. Meyer , F. Miconi , J. Molina , N. K. Mondal , H. da Motta , M. Mulhearn , L. Mundim , E. Nagy , M. Naimuddin , M. Narain , R. Nayyar , H. A. Neal , J. P. Negret , P. Neustroev , S. F. Novaes , T. Nunnemann , G. Obrant , V. Oguri , J. Orduna , N. Osman , J. Osta , 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. Pétroff , M. -A. Pleier , P. L. M. Podesta-Lerma , V. M. Podstavkov , M. -E. Pol , A. V. Popov , W. L. Prado da Silva , M. Prewitt , D. Price , N. Prokopenko , J. Qian , A. Quadt , B. Quinn , M. S. Rangel , K. Ranjan , P. N. Ratoff , I. Razumov , P. Renkel , I. Ripp-Baudot , F. Rizatdinova , M. Rominsky , A. Ross , C. Royon , P. Rubinov , R. Ruchti , G. Sajot , P. Salcido , A. Sánchez-Hernández , M. P. Sanders , B. Sanghi , A. Santoro , A. S. Santos , G. Savage , L. Sawyer , T. Scanlon , R. D. Schamberger , Y. Scheglov , H. Schellman , S. Schlobohm , C. Schwanenberger , R. Schwienhorst , J. Sekaric , H. Severini , E. Shabalina , V. Shary , S. Shaw , A. A. Shchukin , R. K. Shivpuri , V. Simak , P. Skubic , P. Slattery , D. Smirnov , K. J. Smith , G. R. Snow , J. Snow , S. Snyder , S. Söldner-Rembold , L. Sonnenschein , K. Soustruznik , J. Stark , D. A. Stoyanova , M. A. Strang , M. Strauss , L. Stutte , L. Suter , P. Svoisky , M. Takahashi , 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 , A. Y. Verkheev , 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 , 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 , J. Zennamo , T. Zhao , T. G. Zhao , B. Zhou , J. Zhu , M. Zielinski , D. Zieminska , L. Zivkovic

The performance of the Tevatron collider demonstrated continuous growth over the course of Run II, with the peak luminosity reaching 4\times1032 cm-2 s-1, and the weekly integration rate exceeding 70 pb-1. This report presents a review of…

Accelerator Physics · Physics 2012-02-27 A. Valishev

Recent results from searches for non-supersymmetric particles by the CDF and D0 collaborations are reported. The sample taken during the RunII of the Fermilab T eVatron collider at Ecms=1.96 TeV is used. The integrated luminosity analyzed…

High Energy Physics - Experiment · Physics 2019-08-15 Philippe Gris

The D0 detector at The Fermilab Tevatron is undergoing a major upgrade to prepare for data taking with luminosities reaching 2 x 10^{32} cm^{-2} s^{-1}. The upgrade includes a new central tracking array, new muon detector components and…

High Energy Physics - Experiment · Physics 2007-05-23 P. Petroff

We present a preliminary measurement of the inclusive jet cross-sections based on an integrated luminosity of 378 pb^{-1} acquired with the D0 detector between 2002 and 2004 at a center of mass energy of \sqrt{s}=1.96 TeV and a measurement…

High Energy Physics - Experiment · Physics 2010-04-22 Raimund Ströhmer

We measure the ratio of cross sections, {\sigma}(ppbar -> Z + b jet)/{\sigma}(ppbar -> Z + jet), for associated production of a Z boson with at least one jet. The ratio is also measured as a function of the jet transverse momentum, jet…

High Energy Physics - Experiment · Physics 2013-06-05 D0 Collaboration

We measure the ratio of cross sections, $\sigma(p\bar{p}\rightarrow Z+2~b~\text{jets})$/$\sigma(p\bar{p}\rightarrow Z+\text{2 jets})$, for associated production of a $Z$ boson with at least two jets with transverse momentum $p_T^{\rm jet} >…

High Energy Physics - Experiment · Physics 2015-11-23 D0 Collaboration

This article reports a measurement of the production cross section of prompt isolated photon pairs in proton-antiproton collisions at \sqrt{s} = 1.96 TeV using the CDF II detector at the Fermilab Tevatron collider. The data correspond to an…

High Energy Physics - Experiment · Physics 2011-10-06 CDF Collaboration , T. Aaltonen

A measurement of W->e nu + n-jet cross sections in ppbar collisions at sqrt(s)=1.96 TeV using the Collider Detector at Fermilab in Run II is presented. The measurement is based on an integrated luminosity of 320 pb-1, and includes events…

High Energy Physics - Experiment · Physics 2019-08-13 Andrea Messina

A measurement of the $\ttbar$ production cross section in $\ppbar$ collisions at $\sqrt{{\rm s}}$ = 1.96 TeV using events with two leptons, missing transverse energy, and jets is reported. The data were collected with the CDF II Detector.…

High Energy Physics - Experiment · Physics 2010-11-05 The CDF Collaboration , T. Aaltonen

Increasing luminosity at the Fermilab Tevatron collider has led the D0 collaboration to make improvements to its detector beyond those already in place for Run IIa, which began in March 2001. One of the cornerstones of this Run IIb upgrade…

Instrumentation and Detectors · Physics 2008-11-26 M. Abolins

A measurement of the top quark pair ($\mathrm{t\bar{t}}$) production cross section in proton-proton collisions at a centre-of-mass energy of 5.02 TeV is presented. The data were collected at the LHC in autumn 2017, in dedicated runs with…

High Energy Physics - Experiment · Physics 2025-04-28 CMS Collaboration

We report a measurement of the mass of the top quark in lepton+jets final states of ppbar->ttbar data corresponding to 2.6 fb^{-1} of integrated luminosity collected by the D0 experiment at the Fermilab Tevatron Collider. Using a matrix…

High Energy Physics - Experiment · Physics 2015-03-19 The D0 Collaboration , V. Abazov

A measurement of the cross section for the inclusive production of isolated photons by the CDF experiment at the Fermilab Tevatron collider is presented. The measurement covers the pseudorapidity region |eta^gamma|<1.0 and the transverse…

High Energy Physics - Experiment · Physics 2010-05-12 The CDF Collaboration , T. Aaltonen

The inclusive dijet production double differential cross section as a function of the dijet invariant mass and of the largest absolute rapidity of the two jets with the largest transverse momentum in an event is measured in proton…

High Energy Physics - Experiment · Physics 2010-10-28 D0 Collaboration , V. Abazov

The cross section for the inclusive production of isolated photons has been measured in p anti-p collisions at sqrt{s}=1.96 TeV with the D0 detector at the Fermilab Tevatron Collider. The photons span transverse momenta 23 to 300 GeV and…

High Energy Physics - Experiment · Physics 2012-08-27 D0 Collaboration

We discuss recent $B$ physics results from the D{\O}experiment at Fermilab. The results presented here use data sets with integrated luminosities ranging from $\sim 200-440 $ pb$^{-1}$, collected at the Tevatron, between April 2002 and…

High Energy Physics - Experiment · Physics 2010-04-22 Vivek Jain

We have made a precise measurement of the inclusive jet cross section at $\sqrt{s}$=1800 GeV. The result is based on an integrated luminosity of 92 pb^{-1} collected at the Fermilab Tevatron $\bar{p}p$ Collider with the D\O detector. The…

High Energy Physics - Experiment · Physics 2019-08-14 Levan Babukhadia

We present a measurement of R_B, the ratio of the branching fraction for the rare decay D0 -> K+ pi- to that for the Cabibbo-favored decay D0 -> K- pi+. Charge conjugate decays are implicitly included. A signal of 2005 +/- 104 events for…

High Energy Physics - Experiment · Physics 2010-05-12 CDF Collaboration , A. Abulencia

We have made a precise measurement of the inclusive jet cross section at 1800 GeV. The result is based on an integrated luminosity of 92 pb**-1 collected at the Fermilab Tevatron pbarp Collider with the DO detector. The measurement is…

High Energy Physics - Experiment · Physics 2007-05-23 V. Daniel Elvira