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The dissociation of virtual photons, gamma*p -> X(p), in events with a large rapidity gap between X and the outgoing proton, as well as in events in which the leading proton was directly measured, has been studied with the ZEUS detector at HERA. The data cover photon virtualities Q(2) > 2 GeV(2) and gamma*p centre-of-mass energies 40 < W < 240 GeV, with M(X) > 2 GeV, where M(X) is the mass of the hadronic final state, X. Leading protons were detected in the ZEUS leading proton spectrometer. The cross section is presented as a function of t, the squared four-momentum transfer at the proton vertex and Phi. the azimuthal angle between the positron scattering plane and the proton scattering plane. It is also shown as a function of Q(2) and x(P), the fraction of the proton's momentum carried by the diffractive exchange. as well as beta, the Bjorken variable defined with respect to the diffractive exchange. (C) 2009 Elsevier B.V. All rights reserved. RI IBRAHIM, ZAINOL ABIDIN/C-1121-2010; Fazio, Salvatore /G-5156-2010; WAN ABDULLAH, WAN AHMAD TAJUDDIN/B-5439-2010; Doyle, Anthony/C-5889-2009; Ferrando, James/A-9192-2012; Gladilin, Leonid/B-5226-2011
The dissociation of virtual photons, gamma*p -> X(p), in events with a large rapidity gap between X and the outgoing proton, as well as in events in which the leading proton was directly measured, has been studied with the ZEUS detector at HERA. The data cover photon virtualities Q(2) > 2 GeV(2) and gamma*p centre-of-mass energies 40 < W < 240 GeV, with M(X) > 2 GeV, where M(X) is the mass of the hadronic final state, X. Leading protons were detected in the ZEUS leading proton spectrometer. The cross section is presented as a function of t, the squared four-momentum transfer at the proton vertex and Phi. the azimuthal angle between the positron scattering plane and the proton scattering plane. It is also shown as a function of Q(2) and x(P), the fraction of the proton's momentum carried by the diffractive exchange. as well as beta, the Bjorken variable defined with respect to the diffractive exchange. (C) 2009 Elsevier B.V. All rights reserved.
The dissociation of virtual photons, gamma*p -> X(p), in events with a large rapidity gap between X and the outgoing proton, as well as in events in which the leading proton was directly measured, has been studied with the ZEUS detector at HERA. The data cover photon virtualities Q(2) > 2 GeV(2) and gamma*p centre-of-mass energies 40 < W < 240 GeV, with M(X) > 2 GeV, where M(X) is the mass of the hadronic final state, X. Leading protons were detected in the ZEUS leading proton spectrometer. The cross section is presented as a function of t, the squared four-momentum transfer at the proton vertex and Phi. the azimuthal angle between the positron scattering plane and the proton scattering plane. It is also shown as a function of Q(2) and x(P), the fraction of the proton's momentum carried by the diffractive exchange. as well as beta, the Bjorken variable defined with respect to the diffractive exchange. (C) 2009 Elsevier B.V. All rights reserved.
Deep inelastic scattering with leading protons or large rapidity gaps at HERA
Chekanov S.;Derrick M.;Magill S.;Musgrave B.;Nicholass D.;Repond J.;Yoshida R.;Mattingly M. C. K.;Antonioli P.;Bari G.;Bellagamba L.;Boscherini D.;Bruni A.;Bruni G.;Romeo G. Cara;Cindolo F.;Corradi M.;Iacobucci G.;Margotti A.;Massam T.;Nania R.;Polini A.;Antonelli S.;Basile M.;Bindi M.;Cifarelli L.;Contin A.;Palmonari F.;De Pasquale S.;Sartorelli G.;Zichichi A.;Bartsch D.;Brock I.;Hartmann H.;Hilger E.;Jakob H. P.;Juengst M.;Nuncio Quiroz A. E.;Paul E.;Samson U.;Schoenberg V.;Shehzadi R.;Wlasenko M.;Brook N. H.;Heath G. P.;Morris J. D.;Kaur M.;Kaur P.;Singh I.;CAPUA, Marcella;Fazio S.;MASTROBERARDINO, Anna;Schioppa M.;Susinno G.;TASSI, Enrico;Kim J. Y.;Ibrahim Z. A.;Idris F. Mohamad;Kamaluddin B.;Abdullah W. A. T. Wan;Ning Y.;Ren Z.;Sciulli R.;Chwastowski J.;Eskreys A.;Figiel J.;Galas A.;Olkiewicz K.;Pawlik B.;Stopa P.;Zawiejski L.;Adamczyk L.;Bold T.;Grabowska Bold I.;Kisielewska D.;Lukasik J.;Przybycien M.;Suszycki L.;Kotanski A.;Slominski W.;Behnke O.;Behrens U.;Blohm C.;Bonato A.;Borras K.;Bot D.;Ciesielski R.;Coppola N.;Fang S.;Fourletova J.;Geiser A.;Goettlicher P.;Grebenyuk J.;Gregor I.;Haas T.;Hain W.;Huettmann A.;Januschek F.;Kahle B.;Katkov I. I.;Klein U.;Koetz U.;Kowalski H.;Lisovyi M.;Lobodzinska E.;Loehr B.;Mankel R.;Melzer Pellmann I. A.;Miglioranzi S.;Montanari A.;Namsoo T.;Notz D.;Parenti A.;Rinaldi L.;Roloff P.;Rubinsky I.;Schneekloth U.;Spiridonov A.;Szuba D.;Szuba J.;Theedt T.;Ukleja J.;Wolf G.;Wrona K.;Molina A. G. Yaguees;Youngman C.;Zeuner W.;Drugakov V.;Lohmann W.;Schlenstedt S.;Barbagli G.;Gallo E.;Pelfer P. G.;Bamberger A.;Dobur D.;Karstens F.;Vlasov N. N.;Bussey P. J.;Doyle A. T.;Dunne W.;Forrest M.;Rosin M.;Saxon D. H.;Skillicorn I. O.;Gialas I.;Papageorgiu K.;Holm U.;Klanner R.;Lohrmann E.;Perrey H.;Schleper P.;Schoerner Sadenius T.;Sztuk J.;Stadie H.;Turcato M.;Foudas C.;Fry C.;Long K. R.;Tapper A. D.;Matsumoto T.;Nagano K.;Tokushuku K.;Yamada S.;Yamazaki Y.;Barakbaev A. N.;Boos E. G.;Pokrovskiy N. S.;Zhautykov B. O.;Aushev V.;Bachynska O.;Borodin M.;Kadenko I.;Kozulia A.;Libov V.;Lontkovskyi D.;Makarenko I.;Sorokin I.u.;Verbytskyi A.;Volynets O.;Son D.;de Favereau J.;Piotrzkowski K.;Barreiro F.;Glasman C.;Jimenez M.;Labarga L.;del Peso J.;Ron E.;Soares M.;Terron J.;Uribe Estrada C.;Zambrana M.;Corriveau F.;Liu C.;Schwartz J.;Walsh R.;Zhou C.;Tsurugai T.;Antonov A.;Dolgoshein B. A.;Gladkov D.;Sosnovtsev V.;Stifutkin A.;Suchkov S.;Dementiev R. K.;Ermolov P. F.;Gladilin L. K.;Golubkov Y.u. A.;Khein L. A.;Korzhavina I. A.;Kuzmin V. A.;Levchenko B. B.;Lukina O. Yu;Proskuryakov A. S.;Shcheglova L. M.;Zotkin D. S.;Abt I.;Caldwell A.;Kollar D.;Reisert B.;Schmidke W. B.;Grigorescu G.;Keramidas A.;Koffeman E.;Kooijman P.;Pellegrino A.;Tiecke H.;Vazquez M.;Wiggers L.;Bruemmer N.;Bylsma B.;Durkin L. S.;Lee A.;Ling T. Y.;Allfrey P. D.;Bell M. A.;Cooper Sarkar A. M.;Devenish R. C. E.;Ferrando J.;Foster B.;Gwenlan C.;Horton K.;Oliver K.;Robertson A.;Walczak R.;Bertolin A.;Dal Corso F.;Dusini S.;Longhin A.;Stanco L.;Bellan P.;Brugnera R.;Carlin R.;Garfagnini A.;Limentani S.;Oh B. Y.;Raval A.;Whitmore J. J.;Iga Y.;D'Agostini G.;Marini G.;Nigro A.;Cole J. E.;Hart J. C.;Heusch C.;Sadrozinski H.;Seiden A.;Wichmann R.;Williams D. C.;Abramowicz H.;Ingbir R.;Kananov S.;Levy A.;Stern A.;Kuze M.;Maeda J.;Hori R.;Kagawa S.;Okazaki N.;Shimizu S.;Tawara T.;Hamatsu R.;Kaju H.;Kitamura S.;Ota O.;Ri Y. D.;Cirio R.;Costa M.;Ferrero M. I.;Monaco V.;Peroni C.;Sacchi R.;Sola V.;Solano A.;Cartiglia N.;Maselli S.;Staiano A.;Arneodo M.;Ruspa M.;Fourletov S.;Martin J. F.;Stewart T. P.;Boutle S. K.;Butterworth J. M.;Jones T. W.;Loizides J. H.;Wing M.;Brzozowska B.;Ciborowski J.;Grzelak G.;Kulinski P.;Luzniak P.;Malka J.;Nowak R. J.;Pawlak J. M.;Perlanski W.;Tymieniecka T.;Zarnecki A. F.;Adamus M.;Plucinski P.;Ukleja A.;Eisenberg Y.;Hochman D.;Karshon U.;Brownson E.;Reeder D. D.;Savin A. A.;Smith W. H.;Wolfe H.;Bhadra S.;Catterall C. D.;Cui Y.;Hartner G.;Menary S.;Noor U.;Standage J.;Whyte J.
2009-01-01
Abstract
The dissociation of virtual photons, gamma*p -> X(p), in events with a large rapidity gap between X and the outgoing proton, as well as in events in which the leading proton was directly measured, has been studied with the ZEUS detector at HERA. The data cover photon virtualities Q(2) > 2 GeV(2) and gamma*p centre-of-mass energies 40 < W < 240 GeV, with M(X) > 2 GeV, where M(X) is the mass of the hadronic final state, X. Leading protons were detected in the ZEUS leading proton spectrometer. The cross section is presented as a function of t, the squared four-momentum transfer at the proton vertex and Phi. the azimuthal angle between the positron scattering plane and the proton scattering plane. It is also shown as a function of Q(2) and x(P), the fraction of the proton's momentum carried by the diffractive exchange. as well as beta, the Bjorken variable defined with respect to the diffractive exchange. (C) 2009 Elsevier B.V. All rights reserved.
The dissociation of virtual photons, gamma*p -> X(p), in events with a large rapidity gap between X and the outgoing proton, as well as in events in which the leading proton was directly measured, has been studied with the ZEUS detector at HERA. The data cover photon virtualities Q(2) > 2 GeV(2) and gamma*p centre-of-mass energies 40 < W < 240 GeV, with M(X) > 2 GeV, where M(X) is the mass of the hadronic final state, X. Leading protons were detected in the ZEUS leading proton spectrometer. The cross section is presented as a function of t, the squared four-momentum transfer at the proton vertex and Phi. the azimuthal angle between the positron scattering plane and the proton scattering plane. It is also shown as a function of Q(2) and x(P), the fraction of the proton's momentum carried by the diffractive exchange. as well as beta, the Bjorken variable defined with respect to the diffractive exchange. (C) 2009 Elsevier B.V. All rights reserved. RI IBRAHIM, ZAINOL ABIDIN/C-1121-2010; Fazio, Salvatore /G-5156-2010; WAN ABDULLAH, WAN AHMAD TAJUDDIN/B-5439-2010; Doyle, Anthony/C-5889-2009; Ferrando, James/A-9192-2012; Gladilin, Leonid/B-5226-2011
The dissociation of virtual photons, gamma*p -> X(p), in events with a large rapidity gap between X and the outgoing proton, as well as in events in which the leading proton was directly measured, has been studied with the ZEUS detector at HERA. The data cover photon virtualities Q(2) > 2 GeV(2) and gamma*p centre-of-mass energies 40 < W < 240 GeV, with M(X) > 2 GeV, where M(X) is the mass of the hadronic final state, X. Leading protons were detected in the ZEUS leading proton spectrometer. The cross section is presented as a function of t, the squared four-momentum transfer at the proton vertex and Phi. the azimuthal angle between the positron scattering plane and the proton scattering plane. It is also shown as a function of Q(2) and x(P), the fraction of the proton's momentum carried by the diffractive exchange. as well as beta, the Bjorken variable defined with respect to the diffractive exchange. (C) 2009 Elsevier B.V. All rights reserved.
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/20.500.11770/126994
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simulazione ASN
Il report seguente simula gli indicatori relativi alla propria produzione scientifica in relazione alle soglie ASN 2023-2025 del proprio SC/SSD. Si ricorda che il superamento dei valori soglia (almeno 2 su 3) è requisito necessario ma non sufficiente al conseguimento dell'abilitazione. La simulazione si basa sui dati IRIS e sugli indicatori bibliometrici alla data indicata e non tiene conto di eventuali periodi di congedo obbligatorio, che in sede di domanda ASN danno diritto a incrementi percentuali dei valori. La simulazione può differire dall'esito di un’eventuale domanda ASN sia per errori di catalogazione e/o dati mancanti in IRIS, sia per la variabilità dei dati bibliometrici nel tempo. Si consideri che Anvur calcola i valori degli indicatori all'ultima data utile per la presentazione delle domande.
La presente simulazione è stata realizzata sulla base delle specifiche raccolte sul tavolo ER del Focus Group IRIS coordinato dall’Università di Modena e Reggio Emilia e delle regole riportate nel DM 589/2018 e allegata Tabella A. Cineca, l’Università di Modena e Reggio Emilia e il Focus Group IRIS non si assumono alcuna responsabilità in merito all’uso che il diretto interessato o terzi faranno della simulazione. Si specifica inoltre che la simulazione contiene calcoli effettuati con dati e algoritmi di pubblico dominio e deve quindi essere considerata come un mero ausilio al calcolo svolgibile manualmente o con strumenti equivalenti.
