Multijet production at low xBj in deep inelastic scattering at HERA

S. Chekanov,M. Derrick,S. Magill,B. Musgrave,D. Nicholass,J. Repond,R. Yoshida, M.C.K. Mattingly, M. Jechow,N. Pavel,A.G. Yagües Molina,S. Antonelli, P. Antonioli,G. Bari,M. Basile,L. Bellagamba,M. Bindi, D. Boscherini,A. Bruni,G. Bruni, L. Cifarelli,F. Cindolo,A. Contin,M. Corradi,S. De Pasquale,G. Iacobucci, A. Margotti,R. Nania,A. Polini,G. Sartorelli, A. Zichichi,D. Bartsch, I. Brock,S. Goers,H. Hartmann,E. Hilger,H.-P. Jakob,M. Jüngst,O.M. Kind,A.E. Nuncio-Quiroz,E S Paul,Renato Renner,U. Samson,V. Schönberg,R. Shehzadi,M. Wlasenko,N.H. Brook,Greg P Heath,J.D. Morris,T. Namsoo,M. Capua,S. Fazio,A. Mastroberardino,M. Schioppa,G. Susinno,E. Tassi,J.Y. Kim,K.J. Ma,Z.A. Ibrahim,B. Kamaluddin,W.A.T. Wan Abdullah,Y. Ning,Zhongliang Ren,F. Sciulli,J. Chwastowski,A. Eskreys,J. Figiel,A. Galas,M. Gil,K. Olkiewicz,P. Stopa,L. Zawiejski,L. Adamczyk,T. Bołd,I. Grabowska-Bołd, D. Kisielewska,J. Łukasik,M. Przybycień,L. Suszycki,A. Kotański,W. Słomiński,Volker Adler, U. Behrens,I. Bloch,C. Blohm,Alessio Bonato,K. Borras,R. Ciesielski,N. Coppola,A. Dossanov,V. Drugakov,J. Fourletova, A. Geiser,D. Gladkov,P. Göttlicher,J. Grebenyuk,Ingridmaria Gregor,T. Haas, W. Hain,Claus Horn,A. Hüttmann,B. Kahle,I.I. Katkov,U. Klein,U. Kötz,H. Kowalski,E. Lobodzinska,B. Löhr, R. Mankel,I.-A. Melzer-Pellmann,S. Miglioranzi,A. Montanari,D. Notz,Lorenzo Rinaldi,P. Roloff,I. Rubinsky,R. Santamarta,U. Schneekloth, A. Spiridonov, H. Stadie,D. Szuba,J. Szuba,T. Theedt,G. Wolf,K. Wrona,C. Youngman, W. Zeuner,W. Lohmann,S. Schlenstedt, G. Barbagli,E. Gallo,P.G. Pelfer,A. Bamberger, D. Dobur,F. Karstens,N.N. Vlasov,P.J. Bussey,A.T. Doyle,W. Dunne,J. Ferrando,M J Forrest,D.H. Saxon,I.O. Skillicorn,I. Gialas,K. Papageorgiu,T. Gosau,U. Holm,R. Klanner,E. Lohrmann,H. Salehi, P. Schleper,T. Schörner-Sadenius,J. Sztuk,K. Wichmann,K. Wick, C. Foudas,C. Fry,K.R. Long,Alexander Tapper,Mayuko Kataoka,Takuya Matsumoto,K. Nagano,K. Tokushuku, S. Yamada,Y. Yamazaki,A.N. Barakbaev,E.G. Boos,N.S. Pokrovskiy,B.O. Zhautykov,V. Aushev,D. Son,J. de Favereau,Krzysztof Piotrzkowski,F. Barreiro,C. Glasman,M L Jimenez, L. Labarga,J. del Peso,Elias Ron,Mara Senghi Soares,J. Terrón,M. Zambrana,F. Corriveau,Cunjia Liu,Roberval Walsh,Chan Zhou,T. Tsurugai,A. Antonov,B.A. Dolgoshein,V. Sosnovtsev,A. Stifutkin,S. Suchkov,R.K. Dementiev,P.F. Ermolov, L.K. Gladilin,L.A. Khein,I.A. Korzhavina,V.A. Kuzmin,B.B. Levchenko,O.Yu. Lukina, A.S. Proskuryakov,L.M. Shcheglova, D.S. Zotkin,S.A. Zotkin,I. Abt,C. Büttner,A. Caldwell,D. Kollar,W.B. Schmidke,J. Sutiak,G. Grigorescu,A. Keramidas, E. Koffeman,P. Kooijman,A. Pellegrino,H. Tiecke,M. Vázquez,L. Wiggers,N. Brümmer, B. Bylsma,L.S. Durkin,A. Lee,T.Y. Ling,P.D. Allfrey,M.A. Bell,A.M. Cooper-Sarkar,A. Cottrell,R.C.E. Devenish,B. Foster,K. Korcsak-Gorzo,S. Patel,V. Roberfroid,A I Robertson,P.B. Straub,C. Uribe-Estrada, R. Walczak, P. Bellan,A. Bertolin,R. Brugnera,Roberto Carlin,F. Dal Corso,S. Dusini,A. Garfagnini,S. Limentani,A. Longhin,L. Stanco,M. Turcato,B.Y. Oh,Amita Raval,J. Ukleja,J.J. Whitmore,Y. Iga,G. D'Agostini,G. Marini,A. Nigro,J.E. Cole,J.C. Hart, H. Abramowicz,A M Gabareen,R. Ingbir,S. Kananov,A. Levy, M. Kuze,J. Maeda,R. Hori,S. Kagawa,Naoaki Okazaki, S. Shimizu,T. Tawara,R. Hamatsu,H. Kaji,S. Kitamura,O. Ota,Y.D. Ri,M.I. Ferrero,Vincenzo Monaco, R. Sacchi,Ada Solano,M. Arneodo, M. Ruspa,S. Fourletov,J.F. Martin,Sarah Boutle,J.M. Butterworth,C. Gwenlan,T.W. Jones,J.H. Loizides,M.R. Sutton, M. Wing,B. Brzozowska, J. Ciborowski,G. Grzelak,P. Kulinski,P. Łużniak,J. Malka,R.J. Nowak,J.M. Pawlak,T. Tymieniecka,A. Ukleja,A.F. Żarnecki,M. Adamus,Pawel Plucinski,Y. Eisenberg,I. Giller,D. Hochman,U. Karshon,M. Rosin, E. Brownson,T. Danielson,Adam Everett,D. Kçira,D.D. Reeder,P. Ryan,A.A. Savin,W.H. Smith,H. Wolfe,S. Bhadra,C.D. Catterall,Yang Cui,G F Hartner,S. Menary,U. Noor,J. Standage,J. Whyte

NUCLEAR PHYSICS B(2007)

引用 31|浏览128
暂无评分
摘要
Dijet and trijet production in deep inelastic ep scattering has been measured in the phase space region 10 < Q(2) < 100 GeV2 and 10(-4) < x(Bj) < 10(-2) using an integrated luminosity of 82 pb(-1) collected by the ZEUS experiment. The high statistics have made possible detailed studies of multijet production at low xBj. The dependence of dijet and trijet production on the kinematic variables Q(2) and x(Bj) and on the jet variables E-T,HCM(jet) and eta(jet)(LAB) is well described by perturbative QCD calculations which include NLO corrections. To investigate possible deviations with respect to the collinear factorisation approximation used in the standard pQCD approach, measurements of the correlations between the two jets with highest E-T,HCM(jet) have been made. At low x(Bj), measurements of dijet production with low azimuthal separation are reproduced by the perturbative QCD calculations provided that higher-order terms (O(alpha(3)(s))) are accounted for. Such terms increase the predictions of pQCD calculations by up to one order of magnitude when the two jets with the highest E-T,HCM(jet1,2) are not balanced in transverse momentum. This demonstrates the importance of higher-order corrections in the low-x(Bj) region.
更多
查看译文
关键词
perturbation theory,high energy physics
AI 理解论文
溯源树
样例
生成溯源树,研究论文发展脉络
Chat Paper
正在生成论文摘要