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Diffractive electroproduction of ρ and ϕ mesons at HERA

F. D. AaronNational Institute for Physics and Nuclear Engineering (NIPNE), Bucharest, RomaniaM. Aldaya MartinC. AlexaNational Institute for Physics and Nuclear Engineering (NIPNE), Bucharest, RomaniaV. AndreevLebedev Physical Institute, Moscow, RussiaB. AntunovićA. AsmoneDipartimento di Fisica Universit di Roma Tre and INFN Roma 3, Roma, ItalyS. BackovićFaculty of Science, University of Montenegro, Podgorica, MontenegroA. BaghdasaryanYerevan Physics Institute, Yerevan, ArmeniaE. BarreletLPNHE, Universits Paris VI and VII, CNRS/IN2P3, Paris, FranceW. BartelK. BegzsurenInstitute of Physics and Technology of the Mongolian Academy of Sciences, Ulaanbaatar, MongoliaA. BelousovLebedev Physical Institute, Moscow, RussiaJ.C. BizotLAL, Univ Paris-Sud, CNRS/IN2P3, Orsay, FranceV. BoudryLLR, Ecole Polytechnique, CNRS/IN2P3, Palaiseau, FranceI. Božović-Jelisavc̆ićVinca Institute of Nuclear Sciences, Belgrade, SerbiaJ. BraciníkSchool of Physics and Astronomy, University of Birmingham, Birmingham, UKO. BrandtMartin BrinkmannInstitut fr Experimentalphysik, Universitt Hamburg, Hamburg, GermanyV. BrissonLAL, Univ Paris-Sud, CNRS/IN2P3, Orsay, FranceD. BrunckoInstitute of Experimental Physics, Slovak Academy of Sciences, Koice, Slovak RepublicA. BunyatyanMax-Planck-Institut fr Kernphysik, Heidelberg, GermanyG. BuschhornMax-Planck-Institut fr Physik, Mnchen, GermanyL. BystritskayaInstitute for Theoretical and Experimental Physics, Moscow, RussiaAlan CampbellK. B. Cantun AvilaDepartamento de Fisica Aplicada, CINVESTAV, Mérida, Yucatán, MexicoF. Cassol-BrunnerCPPM, CNRS/IN2P3 -Univ. Mediterranee, Marseille, FranceK. ČernýFaculty of Mathematics and Physics, Charles University, Praha, Czech RepublicV. ČernýAlso at Comenius University, Bratislava, Slovak RepublicV. ChekelianMax-Planck-Institut fr Physik, Mnchen, GermanyA. CholewaJ.G. ContrerasDepartamento de Fisica Aplicada, CINVESTAV, Mrida, Yucatn, MexicoJ. A. CoughlanRutherford Appleton Laboratory, Chilton, Didcot, UKG. CozzikaCEA, DSM/Irfu, CE-Saclay, Gif-sur-Yvette, FranceJ. CvachInstitute of Physics, Academy of Sciences of the Czech Republic, Praha, Czech RepublicJ.B. DaintonDepartment of Physics, University of Liverpool, Liverpool, UKK. DaumAlso at Rechenzentrum, Universitt Wuppertal, Wuppertal, GermanyMichal DeákY. de BoerB. DelcourtLAL, Univ Paris-Sud, CNRS/IN2P3, Orsay, FranceM. Del DeganInstitut für Teilchenphysik, ETH, Zürich, SwitzerlandJ. DelvaxUniversiteit Antwerpen, Antwerpen, BelgiumE. A. De WolfInter-University Institute for High Energies ULB-VUB, Brussels; Universiteit Antwer-pen, Antwerpen; BelgiumC. DiaconuCPPM, CNRS/IN2P3 -Univ. Mediterranee, Marseille, FranceV. DodonovMax-Planck-Institut fr Kernphysik, Heidelberg, GermanyA. DossanovMax-Planck-Institut fr Physik, Mnchen, GermanyA. DubakAlso at Max-Planck-Institut fr Physik, Mnchen, GermanyG. EckerlinV. EfremenkoInstitute for Theoretical and Experimental Physics, Moscow, RussiaS. EgliPaul Scherrer Institut, Villigen, SwitzerlandA. EliseevLebedev Physical Institute, Moscow, RussiaE. ElsenA. FalkiewiczL. FavartUniversiteit Antwerpen, Antwerpen, BelgiumA. FedotovInstitute for Theoretical and Experimental Physics, Moscow, RussiaR. FelstJ. FeltesseAlso at DESY and University Hamburg, Helmholtz Humboldt Research Award 49 Also at Faculty of Physics, University of Bucharest, Bucharest, RomaniaJ. FerenceiInstitute of Experimental Physics, Slovak Academy of Sciences, Koice, Slovak RepublicD.-J. FischerM. FleischerA. FomenkoLebedev Physical Institute, Moscow, RussiaE. GabathulerDepartment of Physics, University of Liverpool, Liverpool, UKJ. GaylerS. GhazaryanYerevan Physics Institute, Yerevan, ArmeniaA. GlazovI. GlushkovDESY, Zeuthen, GermanyL. GoerlichN. GogitidzeLebedev Physical Institute, Moscow, RussiaM. GouzevitchC. GrabInstitut fr Teilchenphysik, ETH, Zrich, SwitzerlandT. GreenshawDepartment of Physics, University of Liverpool, Liverpool, UKB.R. GrellG. GrindhammerMax-Planck-Institut fr Physik, Mnchen, GermanyS. HabibInstitut fr Experimentalphysik, Universitt Hamburg, Hamburg, GermanyD. HaidtC. HelebrantR. C. W. HendersonDepartment of Physics, University of Lancaster, Lancaster, UKE. HennekemperKirchhoff-Institut fr Physik, Universitt Heidelberg, Heidelberg, GermanyH. HenschelDESY, Zeuthen, GermanyM. HerbstKirchhoff-Institut fr Physik, Universitt Heidelberg, Heidelberg, GermanyG. HerreraDepartamento de Fisica, CINVESTAV, MexicoM. HildebrandtPaul Scherrer Institut, Villigen, SwitzerlandK. H. HillerDESY, Zeuthen, GermanyD. HoffmannCPPM, CNRS/IN2P3 -Univ. Mediterranee, Marseille, FranceR. HorisbergerPaul Scherrer Institut, Villigen, SwitzerlandT. HreusAlso at University of P.J. afrik, Koice, Slovak RepublicM. JacquetLAL, Univ Paris-Sud, CNRS/IN2P3, Orsay, FranceM.E. JanssenX. JanssenInter-University Institute for High Energies ULB-VUB, Brussels; Universiteit Antwer-pen, Antwerpen; BelgiumL. JönssonPhysics Department, University of Lund, Lund, SwedenA. JungKirchhoff-Institut fr Physik, Universitt Heidelberg, Heidelberg, GermanyH. JungM. KapichineJoint Institute for Nuclear Research, Dubna, RussiaJ. KatzyI. R. KenyonSchool of Physics and Astronomy, University of Birmingham, Birmingham, UKC. KieslingMax-Planck-Institut fr Physik, Mnchen, GermanyM. KleinDepartment of Physics, University of Liverpool, Liverpool, UKC. KleinwortT. KlugeDepartment of Physics, University of Liverpool, Liverpool, UKA. KnutssonR. KoglerMax-Planck-Institut fr Physik, Mnchen, Germany
2010en
ABI

Annotatsiya

Diffractive electroproduction of and mesons is measured at HERA with the H1 detector in the elastic and proton dissociative channels. The data correspond to an integrated luminosity of 51 pb -1 . About 10500 and 2000 events are analysed in the kinematic range of squared photon virtuality 2.5 Q 2 60 GeV 2 , photon-proton centre of mass energy 35 W 180 GeV and squared four-momentum transfer to the proton |t| 3 GeV 2 . The total, longitudinal and transverse cross sections are measured as a function of Q 2 , W and |t|. The measurements show a transition to a dominantly "hard" behaviour, typical of high gluon densities and small q q dipoles, for Q 2 larger than 10 to 20 GeV 2 . They support flavour independence of the diffractive exchange, expressed in terms of the scaling variable (Q 2 +M 2 V )/4, and proton vertex factorisation. The spin density matrix elements are measured as a function of kinematic variables. The ratio of the longitudinal to transverse cross sections, the ratio of the helicity amplitudes and their relative phases are extracted. Several of these measurements have not been performed before and bring new information on the dynamics of diffraction in a QCD framework. The measurements are discussed in the context of models using generalised parton distributions or universal dipole cross sections.

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