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Titolo:
THRUST JET ANALYSIS OF DEEP-INELASTIC LARGE-RAPIDITY-GAP EVENTS
Autore:
ADLOFF C; AID S; ANDERSON M; ANDREEV V; ANDRIEU B; ARKADOV V; ARNDT C; AYYAZ I; BABAEV A; BAHR J; BAN J; BARANOV P; BARRELET E; BARSCHKE R; BARTEL W; BASSLER U; BECK M; BEHREND HJ; BEIER C; BELOUSOV A; BERGER C; BERNARDI G; BERTRANDCOREMANS G; BEYER R; BIDDULPH P; BIZOT JC; BORRAS K; BOTTERWECK F; BOUDRY V; BOUROV S; BRAEMER A; BRAUNSCHWEIG W; BRISSON V; BROWN DP; BRUCKNER W; BRUEL P; BRUNCKO D; BRUNE C; BURGER J; BUSSER FW; BUNIATIAN A; BURKE S; BUSCHHORN G; CALVET D; CAMPBELL AJ; CARLI T; CHARLET M; CLARKE D; CLERBAUX B; COCKS S; CONTRERAS JG; CORMACK C; COUGHLAN JA; COUSINOU MC; COX BE; COZZIKA G; CUSSANS DG; CVACH J; DAGORET S; DAINTON JB; DAU WD; DAUM K; DAVID M; DAVIS CL; DEROECK A; DEWOLF EA; DELCOURT B; DIRKMANN M; DIXON P; DLUGOSZ W; DONOVAN KT; DOWELL JD; DROUTSKOI A; EBERT J; EBERT TR; ECKERLIN G; EFREMENKO V; EGLI S; EICHLER R; EISELE F; EISENHANDLER E; ELSEN E; ERDMANN M; FAHR AB; FAVART L; FEDOTOV A; FELST R; FELTESSE J; FERENCEI J; FERRAROTTO F; FLAMM K; FLEISCHER M; FLIESER M; FLUGGE G; FOMENKO A; FORMANEK J; FOSTER JM; FRANKE G; GABATHULER E; GABATHULER K; GAEDE F; GARVEY J; GAYLER J; GEBAUER M; GERHARDS R; GLAZOV A; GOERLICH L; GOGITIDZE N; GOLDBERG M; GONZALEZPINEIRO B; GORELOV I; GRAB C; GRASSLER H; GREENSHAW T; GRIFFITHS RK; GRINDHAMMER G; GRUBER A; GRUBER C; HADIG T; HAIDT D; HAJDUK L; HALLER T; HAMPEL M; HAYNES WJ; HEINEMANN B; HEINZELMANN G; HENDERSON RCW; HENGSTMANN S; HENSCHEL H; HERYNEK I; HESS MF; HEWITT K; HILLER KH; HILTON CD; HLADKY J; HOPPNER M; HOFFMANN D; HOLTOM T; HORISBERGER R; HUDGSON VL; HUTTE M; IBBOTSON M; ISSEVER C; ITTERBECK H; JACQUET M; JAFFRE M; JANOTH J; JANSEN DM; JONSSON L; JOHNSON DP; JUNG H; KALMUS PIP; KANDER M; KANT D; KATHAGE U; KATZY J; KAUFMANN HH; KAUFMANN O; KAUSCH M; KAZARIAN S; KENYON IR; KERMICHE S; KEUKER C; KIESLING C; KLEIN M; KLEINWORT C; KNIES G; KOHNE JH; KOLANOSKI H; KOLYA SD; KORBEL V; KOSTKA P; KOTELNIKOV SK; KRAMERKAMPER T; KRASNY MW; KREHBIEL H; KRUCKER D; KUPPER A; KUSTER H; KUHLEN M; KURCA T; LAFORGE B; LAHMANN R; LANDON MPJ; LANGE W; LANGENEGGER U; LEBEDEV A; LEHNER F; LEMAITRE V; LEVONIAN S; LINDSTROEM M; LIPINSKI J; LIST B; LOBO G; LOPEZ GC; LUBIMOV V; LUKE D; LYTKIN L; MAGNUSSEN N; MAHLKEKRUGER H; MALINOVSKI E; MARACEK R; MARAGE P; MARKS J; MARSHALL R; MARTENS J; MARTIN G; MARTIN R; MARTYN HU; MARTYNIAK J; MAVROIDIS T; MAXFIELD SJ; MCMAHON SJ; MEHTA A; MEIER K; MERKEL P; METLICA F; MEYER A; MEYER A; MEYER H; MEYER J; MEYER PO; MIGLIORI A; MIKOCKI S; MILSTEAD D; MOECK J; MOREAU F; MORRIS JV; MROCZKO E; MULLER D; MULLER K; MURIN P; NAGOVIZIN V; NAHNHAUER R; NAROSKA B; NAUMANN T; NEGRI I; NEWMAN PR; NEWTON D; NGUYEN HK; NICHOLLS TC; NIEBERGALL F; NIEBUHR C; NIEDZBALLA C; NIGGLI H; NOWAK G; NUNNEMANN T; OBERLACK H; OLSSON JE; OZEROV D; PALMEN P; PANARO E; PANITCH A; PASCAUD C; PASSAGGIO S; PATEL GD; PAWLETTA H; PEPPEL E; PEREZ E; PHILLIPS JP; PIEUCHOT A; PITZL D; POSCHL R; POPE G; POVH B; RABBERTZ K; REIMER P; RICK H; RIESS S; RIZVI E; RIZVI E; ROBMANN P; ROOSEN R; ROSENBAUER K; ROSTOVTSEV A; ROUSE F; ROYON C; RUTER K; RUSAKOV S; RYBICKI K; SANKEY DPC; SCHACHT P; SCHEINS J; SCHIEK S; SCHLEIF S; SCHLEPER P; VONSCHLIPPE W; SCHMIDT D; SCHMIDT G; SCHOEFFEL L; SCHONING A; SCHRODER V; SCHUHMANN E; SCHULTZCOULON HC; SCHWAB B; SEFKOW F; SEMENOV A; SHEKELYAN V; SHEVIAKOV I; SHTARKOV LN; SIEGMON G; SIEWERT U; SIROIS Y; SKILLICORN IO; SLOAN T; SMIRNOV P; SMITH M; SOLOCHENKO V; SOLOVIEV Y; SPECKA A; SPIEKERMANN J; SPIELMAN S; SPITZER H; SQUINABOL F; STEFFEN P; STEINBERG R; STEINHART J; STELLA B; STELLBERGER A; STIEWE J; STOLZE K; STRAUMANN U; STRUCZINSKI W; SUTTON JP; SWART M; TAPPROGGE S; TASEVSKY M; TCHERNYSHOV V; TCHETCHELNITSKI S; THEISSEN J; THOMPSON G; THOMPSON PD; TOBIEN N; TODENHAGEN R; TRUOL P; ZALESAK J; TSIPOLITIS G; TURNAU J; TZAMARIUDAKI E; UELKES P; USIK A; VALKAR S; VALKAROVA A; VALLEE C; VANESCH P; VANMECHELEN P; VANDENPLAS D; VAZDIK Y; VERRECCHIA P; VILLET G; WACKER K; WAGENER A; WAGENER M; WALLNY R; WALTER T; WAUGH B; WEBER G; WEBER M; WEGENER D; WEGNER A; WENGLER T; WERNER M; WEST LR; WIESAND S; WILKSEN T; WILLARD S; WINDE M; WINTER GG; WITTEK C; WOBISCH M; WOLLATZ H; WUNSCH E; ZACEK J; ZARBOCK D; ZHANG Z; ZHOKIN A; ZINI P; ZOMER F; ZSEMBERY J; ZURNEDDEN M;
Indirizzi:
BERG UNIV GESAMTHSCH WUPPERTAL,FACHBEREICH PHYS D-42097 WUPPERTAL GERMANY RHEIN WESTFAL TH AACHEN,INST PHYS 1 D-52074 AACHEN GERMANY RHEIN WESTFAL TH AACHEN,INST PHYS 3 D-52074 AACHEN GERMANY UNIV BIRMINGHAM,SCH PHYS & SPACE RES BIRMINGHAM B15 2TT W MIDLANDS ENGLAND FREE UNIV BRUSSELS,ULB,INTERUNIV INST HIGH ENERGIES BRUSSELS BELGIUM UNIV INSTELLING ANTWERP B-2610 WILRIJK BELGIUM RUTHERFORD APPLETON LAB DIDCOT OX11 0QX OXON ENGLAND INST NUCL PHYS PL-30055 KRAKOW POLAND UNIV CALIF DAVIS,DEPT PHYS DAVIS CA 00000 UNIV CALIF DAVIS,IIRPA DAVIS CA 00000 UNIV DORTMUND,INST PHYS D-44227 DORTMUND GERMANY CEA SACLAY,DSM,DAPNIA F-91191 GIF SUR YVETTE FRANCE UNIV GLASGOW,DEPT PHYS & ASTRON GLASGOW G12 8QQ LANARK SCOTLAND DESY D-22603 HAMBURG GERMANY UNIV HAMBURG,INST EXPT PHYS 1 D-22761 HAMBURG GERMANY UNIV HAMBURG,INST EXPT PHYS 2 D-22761 HAMBURG GERMANY MAX PLANCK INST KERNPHYS D-69029 HEIDELBERG GERMANY UNIV HEIDELBERG,INST PHYS D-69120 HEIDELBERG GERMANY UNIV HEIDELBERG,INST HOCHENERGIEPHYS D-69120 HEIDELBERG GERMANY CHRISTIAN ALBRECHTS UNIV KIEL,INST REINE & ANGEW KERNPHYS D-24118 KIEL GERMANY SLOVAK ACAD SCI,INST EXPT PHYS KOSICE 04353 SLOVAKIA UNIV LANCASTER,SCH PHYS & CHEM LANCASTER LA1 4YB ENGLAND UNIV LIVERPOOL,DEPT PHYS LIVERPOOL L69 3BX MERSEYSIDE ENGLAND UNIV LONDON QUEEN MARY & WESTFIELD COLL LONDON E1 4NS ENGLAND LUND UNIV,DEPT PHYS S-22362 LUND SWEDEN UNIV MANCHESTER,DEPT PHYS MANCHESTER M13 9PL LANCS ENGLAND UNIV AIX MARSEILLE 2,CPPM,IN2P3,CNRS F-13288 MARSEILLE FRANCE INST THEORET & EXPT PHYS RU-117924 MOSCOW RUSSIA PN LEBEDEV PHYS INST RU-117924 MOSCOW RUSSIA MAX PLANCK INST PHYS & ASTROPHYS D-80805 MUNICH GERMANY UNIV PARIS 11,IN2P3,CNRS,LAL F-91405 ORSAY FRANCE ECOLE POLYTECH,IN2P3,CNRS,LPNHE F-91128 PALAISEAU FRANCE UNIV PARIS 06,LPNHE,IN2P3,CNRS F-75252 PARIS FRANCE UNIV PARIS 07,LPNHE,IN2P3,CNRS F-75252 PARIS FRANCE ACAD SCI CZECH REPUBL,INST PHYS CZ-18040 PRAGUE CZECH REPUBLIC CHARLES UNIV,NUCL CTR CZ-18000 PRAGUE CZECH REPUBLIC INFN ROMA 1 I-00146 ROME ITALY UNIV ROMA 3,DIPARTIMENTO FIS I-00146 ROME ITALY PAUL SCHERRER INST CH-5232 VILLIGEN SWITZERLAND INST HOCHENERGIEPHYS,DESY D-15738 ZEUTHEN GERMANY ETH ZURICH,INST TEILCHENPHYS CH-8093 ZURICH SWITZERLAND UNIV ZURICH,INST PHYS CH-8001 ZURICH SWITZERLAND HUMBOLDT UNIV BERLIN,INST PHYS D-10115 BERLIN GERMANY BERG UNIV GESAMTHSCH WUPPERTAL,RECHENZENTRUM D-42097 WUPPERTAL GERMANY
Titolo Testata:
EUROPEAN PHYSICAL JOURNAL C-PARTICLES AND FIELDS
fascicolo: 3-4, volume: 1, anno: 1998,
pagine: 495 - 507
SICI:
1434-6044(1998)1:3-4<495:TJAODL>2.0.ZU;2-Q
Fonte:
ISI
Lingua:
ENG
Soggetto:
E+E-ANNIHILATION; DIFFRACTION DISSOCIATION; POWER CORRECTIONS; QCD CASCADES; CM ENERGIES; SCATTERING; MODEL; HERA; PREDICTIONS; COLLISIONS;
Tipo documento:
Article
Natura:
Periodico
Settore Disciplinare:
Science Citation Index Expanded
Citazioni:
66
Recensione:
Indirizzi per estratti:
Citazione:
C. Adloff et al., "THRUST JET ANALYSIS OF DEEP-INELASTIC LARGE-RAPIDITY-GAP EVENTS", EUROPEAN PHYSICAL JOURNAL C-PARTICLES AND FIELDS, 1(3-4), 1998, pp. 495-507

Abstract

A thrust analysis of Large-Rapidity-Gap events in deep-inelastic cp collisions is presented, using data taken with the H1 detector at HERA in 1994. The average thrust of the final states X, which emerge from the dissociation of virtual photons in the range 10 < Q(2) < 100 GeV2 grows with hadronic mass nr, and implies a dominant 2-jet topology. Thrust is found to decrease with growing P-t, the thrust jet momentum transverse to the photon-proton collision axis. Distributions of P-t(2) are consistent with being independent of M-x. They show a strong alignment of the thrust axis with the photon-proton collision axis. and havea large high-P-t tail. Tile correlation of thrust with M-x is similarto that ill e(+)e(-) annihilation at root s(ee) = M-x but with lower values of thrust in the ep data. The data cannot be described by interpreting the dissociated system X as a q (q) over bar state but inclusion of a substantial fraction of q (q) over bar q parton configurationsleads naturally to the observed properties. The soft colour exchange interaction model does not describe the data.

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Documento generato il 04/12/20 alle ore 09:00:09