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We considered the three jet production processes in the region of the incident lepton, photon, quark or gluon fragmentation. The fourth jet is created by the recoil proton. The kinematics of jet production is discussed in jets production in…

High Energy Physics - Phenomenology · Physics 2015-06-18 Azad I. Ahmadov , Eduard A. Kuraev

A comprehensive overview of the latest aspects of jet physics in proton-antiproton collisions at $\sqrt{s}=$1.96 TeV is presented. In particular, measurements of the inclusive jet production, dijet and multi-jet production, and jet…

High Energy Physics - Experiment · Physics 2011-06-17 Christina Mesropian

Dijet production in DIS is an important laboratory for testing our understanding of perturbative QCD. Flexible NLO Monte Carlo programs allow to investigate general jet definition schemes. For forward jet production at $p_{Tj} \approx Q$…

High Energy Physics - Phenomenology · Physics 2009-10-30 Erwin Mirkes , Dieter Zeppenfeld

The kernel of the BFKL equation for non-zero momentum transfer is found at next-to-leading order. It is presented in various forms depending on the regularization of the infrared singularities in "virtual" and "real" parts of the kernel.…

High Energy Physics - Phenomenology · Physics 2010-11-05 V. S. Fadin , R. Fiore

The inclusive cross-section for production of a jet with a given transverse momentum off a heavy nucleus is derived in the BFKL framework with a running coupling on the basis of the bootstrap relation. The cross-section depends on the same…

High Energy Physics - Phenomenology · Physics 2015-05-19 M. A. Braun

Annihilation process of proton and antiproton to guark antiquark pair accompanied by emission of two additional gluon jets with intermediate state of vector meson is considered.Strong azimuthal correlation is revealed of two gluonic…

High Energy Physics - Phenomenology · Physics 2011-08-11 E. A. Kuraev , V. V. Bytev , E. S. Kokoulina

Diffractive vector meson photoproduction accompanied by proton dissociation is studied for large momentum transfer. The process is described by the non-forward BFKL equation, for which an analytical solution is found for all conformal…

High Energy Physics - Phenomenology · Physics 2007-05-23 R. Enberg , L. Motyka , G. Poludniowski

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

Identifying jets in heavy ion collisions is of significant interest since the properties of jets are expected to get modified because of the formation of quark gluon plasma. The detection of jets is, however, difficult because of large…

Nuclear Theory · Physics 2008-09-17 Sadhana Dash , Dipak K. Mishra , S. C. Phatak , P. K. Sahu

We propose a phenomenological study of the Balitsky-Fadin-Kuraev-Lipatov (BFKL) approach applied to the data on the proton structure function F_2 measured at HERA in the small-x_{Bjorken} region. In a first part we use a simplified…

High Energy Physics - Phenomenology · Physics 2008-11-26 R. Peschanski , C. Royon , L. Schoeffel

A study of dijet production in proton-proton collisions was performed at sqrt(s) = 7 TeV for jets with pt > 35 GeV and abs(y) < 4.7 using data collected with the CMS detector at the LHC in 2010. Events with at least one pair of jets are…

High Energy Physics - Experiment · Physics 2013-01-24 CMS Collaboration

We study the efficiency of a neural-net filter and deconvolution method for estimating jet energies and spectra in high-background reactions such as nuclear collisions at the relativistic heavy-ion collider and the large hadron collider.…

Nuclear Theory · Physics 2009-10-22 Dawei W Dong , Miklos Gyulassy

Diffractive vector meson photoproduction accompanied by proton dissociation is studied for large momentum transfer. The process is described by the non-forward BFKL equation which we use to compare to data collected at the HERA collider.

High Energy Physics - Phenomenology · Physics 2009-11-10 G. G. Poludniowski , R. Enberg , J. R. Forshaw , L. Motyka

We propose the study of new observables in LHC inclusive events with three tagged jets, one in the forward direction, one in the backward direction and both well-separated in rapidity from the each other (Mueller-Navelet jets), together…

High Energy Physics - Phenomenology · Physics 2018-02-14 F. Caporale , F. G. Celiberto , G. Chachamis , D. Gordo Gomez , A. Sabio Vera

We compute the cross-section of the hadronic jets arising from the quark antiquark pair which are produced from a hard photons (of 4-momentum $q$) in the plasma, predominantly consisting of thermalised quarks and gluons. The quark antiquark…

High Energy Physics - Phenomenology · Physics 2007-05-23 Krishnendu Mukherjee

Dilepton production in proton-proton collision through $\gamma\gamma$-fusion with one proton scattered elastically while the second produces a hadron jet is considered. Semi-analytical formulas describing the cross section of a muon pair…

High Energy Physics - Phenomenology · Physics 2022-01-26 S. I. Godunov , E. K. Karkaryan , V. A. Novikov , A. N. Rozanov , M. I. Vysotsky , E. V. Zhemchugov

We investigate different final state features in Mueller-Navelet jets events at hadron colliders. The focus lies on the average rapidity ratio between subsequent minijet emissions which has been investigated in previous works but now is…

High Energy Physics - Phenomenology · Physics 2021-12-08 Nauzet Bethencourt de León , Grigorios Chachamis , Agustín Sabio Vera

The aim of this study is to set a baseline for the jet quenching measurements of the Quark Gluon Plasma (QGP) formed in the large system size Nucleus-Nucleus (A-A) at top central collisions, via studying simulated small system size,…

High Energy Physics - Experiment · Physics 2020-01-29 M. T. AlFiky , O. T. ElSherif , A. M. Hamed

Collisions of heavy ion nuclei at relativistic speeds (close to the speed of light) creates a high temperature and very dense form of matter, now known to consist of de-confined quarks and gluons, named the quark gluon plasma (QGP). In this…

High Energy Physics - Experiment · Physics 2018-03-13 Raghav Kunnawalkam Elayavalli

The most extreme deformations that can be explored in heavy-ion collisions at Fermi-energies are collimated flows of nuclear matter which recall jet dynamics. From microphysics to the cosmological scale, jets are rather common topologies.…

Nuclear Theory · Physics 2019-05-06 P. Napolitani , M. Colonna
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