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Related papers: First results on e^+e^- -> 3 jets at NNLO

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We present the first fully analytic calculation of the Quantum Chromodynamics (QCD) event shape observable Energy-Energy Correlation in electron-positron annihilation at Next-To-Leading Order (NLO). This result sheds light on the analytic…

High Energy Physics - Phenomenology · Physics 2018-07-20 Lance J. Dixon , Ming-xing Luo , Vladyslav Shtabovenko , Tong-Zhi Yang , Hua Xing Zhu

We calculate the cross section of the process e^+e^- \to t\bar t near threshold by resumming Coulomb-like terms with next-to-next-to-leading (NNLO) accuracy. The nonrelativistic Green function formalism and the method of ``direct matching''…

High Energy Physics - Phenomenology · Physics 2008-11-26 Oleg Yakovlev

We consider the production of heavy quark jets at the $Z$-pole at the next-to-leading order (NLO) using the {\it Cambridge jet-algorithm}. We study the effects of the quark mass in two- and three-jet observables and the uncertainty due to…

High Energy Physics - Phenomenology · Physics 2009-10-31 Mikhail Bilenky , Susana Cabrera , Joan Fuster , Salvador Marti , German Rodrigo , Arcadi Santamaria

We report on the first next-to-leading order QCD computation of W + 3-jet production in hadronic collisions including all partonic subprocesses. We compare the results with CDF data from the Tevatron, and find excellent agreement. The…

High Energy Physics - Phenomenology · Physics 2010-04-21 C. F. Berger , Z. Bern , L. J. Dixon , F. Febres Cordero , D. Forde , T. Gleisberg , H. Ita , D. A. Kosower , D. Maitre

We compute theoretical predictions for the production of a W-boson in association with a bottom-quark pair at hadron colliders at next-to-next-to-leading order (NNLO) in QCD, including the leptonic decay of the W-boson, while treating the…

High Energy Physics - Phenomenology · Physics 2022-05-17 Heribertus Bayu Hartanto , Rene Poncelet , Andrei Popescu , Simone Zoia

We present results for the complete NNLL+NLO (~ \alpha_s) 1-jettiness (\tau_1) event shape distribution for single jet (J) production in electron-nucleus (N_A) collisions e^- + N_A \to e^- + J + X, in the deep inelastic scattering (DIS)…

High Energy Physics - Phenomenology · Physics 2014-07-30 Zhong-Bo Kang , Xiaohui Liu , Sonny Mantry

We compute the Next-to-Next-to-Leading Order (NNLO) QCD corrections to the partonic reaction that dominates top-pair production at the Tevatron. This is the first ever NNLO calculation of an observable with more than two colored partons,…

High Energy Physics - Phenomenology · Physics 2013-05-30 Peter Baernreuther , Michal Czakon , Alexander Mitov

We calculate the next-to-leading order (NLO) quantum chromodynamics (QCD) correction to the exclusive process $\gamma+\gamma\to J/\psi+J/\psi$ in the framework of non-relativistic QCD (NRQCD) factorization formalism. The cross sections at…

High Energy Physics - Phenomenology · Physics 2020-06-11 Hao Yang , Zi-Qiang Chen , Cong-Feng Qiao

We report the results of a next-to-leading order event generator of purely gluonic jet production. This calculation is the first step in the construction of a full next-to-leading order calculation of three jet production at hadron…

High Energy Physics - Phenomenology · Physics 2009-10-30 William B. Kilgore , W. T. Giele

The properties of three-jet events with total transverse energy greater than 320 GeV and individual jet energy greater than 20 GeV have been analyzed and compared to absolute predictions from a next-to-leading order (NLO) perturbative QCD…

High Energy Physics - Experiment · Physics 2010-05-12 D. Acosta , T. Affolder , M. G. Albrow , D. Ambrose , D. Amidei , K. Anikeev , J. Antos , G. Apollinari , T. Arisawa , A. Artikov , W. Ashmanskas , F. Azfar , P. Azzi-Bacchetta , N. Bacchetta , H. Bachacou , W. Badgett , A. Barbaro-Galtieri , V. E. Barnes , B. A. Barnett , S. Baroiant , M. Barone , G. Bauer , F. Bedeschi , S. Behari , S. Belforte , W. H. Bell , G. Bellettini , J. Bellinger , D. Benjamin , A. Beretvas , A. Bhatti , M. Binkley , D. Bisello , M. Bishai , R. E. Blair , C. Blocker , K. Bloom , B. Blumenfeld , A. Bocci , A. Bodek , G. Bolla , A. Bolshov , D. Bortoletto , J. Boudreau , C. Bromberg , E. Brubaker , J. Budagov , H. S. Budd , K. Burkett , G. Busetto , K. L. Byrum , S. Cabrera , M. Campbell , W. Carithers , D. Carlsmith , A. Castro , D. Cauz , A. Cerri , L. Cerrito , J. Chapman , C. Chen , Y. C. Chen , M. Chertok , G. Chiarelli , G. Chlachidze , F. Chlebana , M. L. Chu , J. Y. Chung , W. -H. Chung , Y. S. Chung , C. I. Ciobanu , A. G. Clark , M. Coca , A. Connolly , M. Convery , J. Conway , M. Cordelli , J. Cranshaw , R. Culbertson , D. Dagenhart , S. D'Auria , P. de Barbaro , S. De Cecco , S. Dell'Agnello , M. Dell'Orso , S. Demers , L. Demortier , M. Deninno , D. De Pedis , P. F. Derwent , C. Dionisi , J. R. Dittmann , A. Dominguez , S. Donati , M. D'Onofrio , T. Dorigo , N. Eddy , R. Erbacher , D. Errede , S. Errede , R. Eusebi , S. Farrington , R. G. Feild , J. P. Fernandez , C. Ferretti , R. D. Field , I. Fiori , B. Flaugher , L. R. Flores-Castillo , G. W. Foster , M. Franklin , J. Friedman , I. Furic , M. Gallinaro , A. F. Garfinkel , C. Gay , D. W. Gerdes , E. Gerstein , S. Giagu , P. Giannetti , K. Giolo , M. Giordani , P. Giromini , V. Glagolev , D. Glenzinski , M. Gold , N. Goldschmidt , J. Goldstein , G. Gomez , M. Goncharov , I. Gorelov , A. T. Goshaw , Y. Gotra , K. Goulianos , A. Gresele , C. Grosso-Pilcher , M. Guenther , J. Guimaraes da Costa , C. Haber , S. R. Hahn , E. Halkiadakis , R. Handler , F. Happacher , K. Hara , R. M. Harris , F. Hartmann , K. Hatakeyama , J. Hauser , J. Heinrich , M. Hennecke , M. Herndon , C. Hill , A. Hocker , K. D. Hoffman , S. Hou , B. T. Huffman , R. Hughes , J. Huston , C. Issever , J. Incandela , G. Introzzi , M. Iori , A. Ivanov , Y. Iwata , B. Iyutin , E. James , M. Jones , T. Kamon , J. Kang , M. Karagoz Unel , S. Kartal , H. Kasha , Y. Kato , R. D. Kennedy , R. Kephart , B. Kilminster , D. H. Kim , H. S. Kim , M. J. Kim , S. B. Kim , S. H. Kim , T. H. Kim , Y. K. Kim , M. Kirby , L. Kirsch , S. Klimenko , P. Koehn , K. Kondo , J. Konigsberg , A. Korn , A. Korytov , J. Kroll , M. Kruse , V. Krutelyov , S. E. Kuhlmann , N. Kuznetsova , A. T. Laasanen , S. Lami , S. Lammel , J. Lancaster , K. Lannon , M. Lancaster , R. Lander , A. Lath , G. Latino , T. LeCompte , Y. Le , J. Lee , S. W. Lee , N. Leonardo , S. Leone , J. D. Lewis , K. Li , C. S. Lin , M. Lindgren , T. M. Liss , T. Liu , D. O. Litvintsev , N. S. Lockyer , A. Loginov , M. Loreti , D. Lucchesi , P. Lukens , L. Lyons , J. Lys , R. Madrak , K. Maeshima , P. Maksimovic , L. Malferrari , M. Mangano , G. Manca , M. Mariotti , M. Martin , A. Martin , V. Martin , M. Martinez , P. Mazzanti , K. S. McFarland , P. McIntyre , M. Menguzzato , A. Menzione , P. Merkel , C. Mesropian , A. Meyer , T. Miao , R. Miller , J. S. Miller , S. Miscetti , G. Mitselmakher , N. Moggi , R. Moore , T. Moulik , M. Mulhearn , A. Mukherjee , T. Muller , A. Munar , P. Murat , J. Nachtman , S. Nahn , I. Nakano , R. Napora , F. Niell , C. Nelson , T. Nelson , C. Neu , M. S. Neubauer , C. Newman-Holmes , T. Nigmanov , L. Nodulman , S. H. Oh , Y. D. Oh , T. Ohsugi , T. Okusawa , W. Orejudos , C. Pagliarone , F. Palmonari , R. Paoletti , V. Papadimitriou , J. Patrick , G. Pauletta , M. Paulini , T. Pauly , C. Paus , D. Pellett , A. Penzo , T. J. Phillips , G. Piacentino , J. Piedra , K. T. Pitts , A. Pompos , L. Pondrom , G. Pope , T. Pratt , F. Prokoshin , J. Proudfoot , F. Ptohos , O. Poukhov , G. Punzi , J. Rademacker , A. Rakitine , F. Ratnikov , H. Ray , A. Reichold , P. Renton , M. Rescigno , F. Rimondi , L. Ristori , W. J. Robertson , T. Rodrigo , S. Rolli , L. Rosenson , R. Roser , R. Rossin , C. Rott , A. Roy , A. Ruiz , D. Ryan , A. Safonov , R. St. Denis , W. K. Sakumoto , D. Saltzberg , C. Sanchez , A. Sansoni , L. Santi , S. Sarkar , P. Savard , A. Savoy-Navarro , P. Schlabach , E. E. Schmidt , M. P. Schmidt , M. Schmitt , L. Scodellaro , A. Scribano , A. Sedov , S. Seidel , Y. Seiya , A. Semenov , F. Semeria , M. D. Shapiro , P. F. Shepard , T. Shibayama , M. Shimojima , M. Shochet , A. Sidoti , A. Sill , P. Sinervo , A. J. Slaughter , K. Sliwa , F. D. Snider , R. Snihur , M. Spezziga , F. Spinella , M. Spiropulu , L. Spiegel , A. Stefanini , J. Strologas , D. Stuart , A. Sukhanov , K. Sumorok , T. Suzuki , R. Takashima , K. Takikawa , M. Tanaka , M. Tecchio , R. J. Tesarek , P. K. Teng , K. Terashi , S. Tether , J. Thom , T. L. Thomas , A. S. Thompson , E. Thomson , P. Tipton , S. Tkaczyk , D. Toback , K. Tollefson , D. Tonelli , M. Toennesmann , H. Toyoda , W. Trischuk , J. Tseng , D. Tsybychev , N. Turini , F. Ukegawa , T. Unverhau , T. Vaiciulis , A. Varganov , E. Vataga , S. Vejcik , G. Velev , G. Veramendi , R. Vidal , I. Vila , R. Vilar , I. Volobouev , M. von der Mey , R. G. Wagner , R. L. Wagner , W. Wagner , Z. Wan , C. Wang , M. J. Wang , S. M. Wang , B. Ward , S. Waschke , D. Waters , T. Watts , M. Weber , W. C. Wester , B. Whitehouse , A. B. Wicklund , E. Wicklund , H. H. Williams

In these proceedings we present results from a recent calculation for the production of a W boson in conjunction with five jets at next-to-leading order in perturbative QCD. We also use results at lower multiplicities to extrapolate the…

High Energy Physics - Phenomenology · Physics 2013-08-20 Z. Bern , L. J. Dixon , F. Febres Cordero , S. Höche , H. Ita , D. A. Kosower , K. J. Ozeren , D. Maître

We compute the next-to-next-to-leading order (NNLO) QCD correction to the total cross-section for the reaction gg \to t\bar t + X. Together with the partonic channels we computed previously, the result derived in this letter completes the…

High Energy Physics - Phenomenology · Physics 2013-08-06 Michal Czakon , Paul Fiedler , Alexander Mitov

We calculate the production of a W boson in association with up to two jets including at least one b-jet to next-to-leading order (NLO) in QCD at the CERN Large Hadron Collider with 7 TeV center-of-mass energy. Both exclusive and inclusive…

High Energy Physics - Phenomenology · Physics 2013-03-20 F. Caola , J. M. Campbell , F. Febres Cordero , L. Reina , D. Wackeroth

We report on the first calculation of next-to-next-to-leading order (NNLO) QCD corrections to the inclusive production of ZZ pairs at hadron colliders. Numerical results are presented for pp collisions with centre-of-mass energy…

High Energy Physics - Phenomenology · Physics 2015-06-19 F. Cascioli , T. Gehrmann , M. Grazzini , S. Kallweit , P. Maierhöfer , A. von Manteuffel , S. Pozzorini , D. Rathlev , L. Tancredi , E. Weihs

We report next-to-leading order perturbative QCD predictions of 4 jet event shape variables for the process e+e- \to 4 jets obtained using the general purpose Monte Carlo EERAD2. This program is based on the known `squared' one loop matrix…

High Energy Physics - Phenomenology · Physics 2008-11-26 J. M. Campbell , M. A. Cullen , E. W. N. Glover

The inclusive one- and two-jet cross-sections are measured in collisions of quasi-real photons at e+e- centre-of-mass energies of 130 and 136 GeV using the OPAL detector at LEP. Jets are reconstructed with a cone jet finding algorithm. The…

High Energy Physics - Experiment · Physics 2007-05-23 Stefan Soldner-Rembold

Several important processes and analyses at the LHC are sensitive to higher-order perturbative corrections beyond what can currently be calculated at fixed order. One important class of logarithmic corrections are those which appear when…

High Energy Physics - Phenomenology · Physics 2022-02-04 Emmet P. Byrne

We present the next-to-next-to-leading order (NNLO) QCD corrections to dijet production in the purely gluonic channel retaining the full dependence on the number of colours. The sub-leading colour contribution in this channel first appears…

High Energy Physics - Phenomenology · Physics 2015-06-17 James Currie , Aude Gehrmann-De Ridder , E. W. N. Glover , Joao Pires

In quark-antiquark pair production at LEP, many features of the hadronic final state can be predicted by QCD. Using data collected by the OPAL experiment, we present the statistical distributions of fourteen "event shape observables," which…

High Energy Physics - Experiment · Physics 2009-09-29 Matthew Ford

We compute next-to-next-to-leading order (NNLO) QCD corrections to neutral vector boson production in association with a charm jet at the LHC. This process is studied in the forward kinematics at $\sqrt{s}=13$ TeV, which may provide…

High Energy Physics - Phenomenology · Physics 2023-05-31 R. Gauld , A. Gehrmann-De Ridder , E. W. N. Glover , A. Huss , A. Rodriguez Garcia , G. Stagnitto
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