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Three-jet event-shape distributions can be exploited to investigate the dependence of hadronisation effects on the colour and the geometry of the underlying hard event. We present here the first comparison of data in e+e- annihilation and…

High Energy Physics - Phenomenology · Physics 2007-06-20 Andrea Banfi

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

This talk discusses recent results for next-to-next-to-leading order (NNLO) QCD corrections to jet cross sections and transverse momentum distributions. The results are obtained in the NNLOJET code framework, which provides an…

We compute the next-to-next-to-leading order (NNLO) QCD corrections to the first five moments of six event shape variables related to three-particle final states in electron-positron annihilation; the thrust, the heavy jet mass, the…

High Energy Physics - Phenomenology · Physics 2009-06-11 A. Gehrmann-De Ridder , T. Gehrmann , E. W. N. Glover , G. Heinrich

The next-to-leading order three-jet cross section in hadron collisions is calculated in the simplified case when the matrix elements of all QCD subprocesses are approximated by the pure gluon matrix element. The longitudinally-invariant…

High Energy Physics - Phenomenology · Physics 2009-10-30 Zoltán Trócsányi

We present next-to-leading order corrections in the leading colour approximation for jet rates in electron-positron annihilation up to seven jets. The results for the two-, three-, and four-jet rates agree with known results. The NLO jet…

High Energy Physics - Phenomenology · Physics 2013-05-30 Sebastian Becker , Daniel Goetz , Christian Reuschle , Christopher Schwan , Stefan Weinzierl

This article gives the perturbative NNLO results for the most commonly used event shape variables associated to three-jet events in electron-positron annihilation: Thrust, heavy jet mass, wide jet broadening, total jet broadening, C…

High Energy Physics - Phenomenology · Physics 2009-10-16 Stefan Weinzierl

The N-jettiness event shape divides phase space into N+2 regions, each containing one jet or beam. Using a geometric measure these regions correspond to jets with circular boundaries. We give a factorization theorem for the cross section…

High Energy Physics - Phenomenology · Physics 2011-06-21 Teppo T. Jouttenus , Iain W. Stewart , Frank J. Tackmann , Wouter J. Waalewijn

We give a brief overview of our calculation of the next-to-next-to-leading order (NNLO) QCD corrections to Z+jet production in hadronic collisions. Phenomenological results are presented which comprise various differential distributions for…

High Energy Physics - Phenomenology · Physics 2016-07-07 A. Gehrmann-De Ridder , T. Gehrmann , E. W. N. Glover , A. Huss , T. A. Morgan

We present results of a next-to-leading order calculation of three jet production at hadron colliders. This calculation will have many applications. In addition to computing such three-jet observables as spectra, mass distributions, this…

High Energy Physics - Phenomenology · Physics 2007-05-23 William B. Kilgore , Walter T. Giele

We compute the electroweak ${\cal O}(\alpha^3\alpha_s)$ corrections to three-jet production and related event-shape observables at electron-positron colliders. We properly account for the experimental photon isolation criteria and for the…

High Energy Physics - Phenomenology · Physics 2009-09-28 Ansgar Denner , Stefan Dittmaier , Thomas Gehrmann , Christian Kurz

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

In this article we illustrate how event weights for jet events can be calculated efficiently at next-to-leading order (NLO) accuracy in QCD. This is a crucial prerequisite for the application of the Matrix Element Method in NLO. We modify…

High Energy Physics - Phenomenology · Physics 2015-09-18 Till Martini , Peter Uwer

The N-jettiness event shape divides phase space into N+2 regions, each containing one jet or beam. These jet regions are insensitive to the distribution of soft radiation and, with a geometric measure for N-jettiness, have circular…

High Energy Physics - Phenomenology · Physics 2015-05-30 Teppo T. Jouttenus , Iain W. Stewart , Frank J. Tackmann , Wouter J. Waalewijn

We discuss next-to-next-to-leading order QCD results for Higgs, W-boson and Z-boson production in association with a jet in hadronic collisions, obtained using the recently developed N-jettiness subtraction method.

High Energy Physics - Phenomenology · Physics 2016-01-22 Radja Boughezal

We present the computation of next-to-leading order (NLO) QCD corrections to di-photon production in association with two or three hard jets in pp collisions at a center-of-mass energy of 8 TeV. The inclusion of NLO corrections is shown to…

High Energy Physics - Phenomenology · Physics 2015-06-18 Simon Badger , Alberto Guffanti , Valery Yundin

We introduce a set of correlations between energy flow and event shapes that are sensitive to the flow of color at short distances in jet events. These correlations are formulated for a general set of event shapes, which includes jet…

High Energy Physics - Phenomenology · Physics 2014-11-17 Carola F. Berger , Tibor Kucs , George Sterman

We consider QCD radiative corrections to vector-boson production in hadron collisions. We present the next-to-next-to-leading order (NNLO) result of the hard-collinear coefficient function for the all-order resummation of…

High Energy Physics - Phenomenology · Physics 2015-06-11 S. Catani , L. Cieri , D. de Florian , G. Ferrera , M. Grazzini

The production of two jets is the simplest exclusive quantum chromodynamics process in electron-positron annihilation. Using this process, we examine the structure of next-to-next-to-leading order (NNLO) corrections to jet production…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. Gehrmann-De Ridder , T. Gehrmann , E. W. N. Glover

We study three and four jet production in hadronic collisions at next-to-leading order accuracy in massless QCD. We cross check results previously obtained by the BlackHat collaboration for the LHC with a centre-of-mass energy of sqrt(s)=7…

High Energy Physics - Phenomenology · Physics 2015-06-11 Simon Badger , Benedikt Biedermann , Peter Uwer , Valery Yundin