Exclusive J/ψ production and gluonic structure
|
|
- Albert Norman
- 5 years ago
- Views:
Transcription
1 Exclusive J/ψ production and gluonic structure C. Weiss (JLab), Exclusive Meson Production Workshop, JLab, Jan 25 Quarkonium size and structure Parametric: Dynamical scales Numerical: Potential models, Lattice QCD hard x 1 x ? t J /ψ J/ψ photo/electroproduction at W W th FNAL, COMPASS, HERA, EIC Space time picture in rest frame GPD as color dipole moment of nucleon Gluon imaging of nucleon J/ψ photo/electroproduction near threshold Cornell, SLAC, JLab 12 GeV Kinematics of large t min,x Gluonic form factor of nucleon Nuclear targets Connections: Small size configurations, high Q 2 meson production, high t form factors, color transparency...
2 Heavy quarkonium: Scales and size m r Parametric: Non relativistic system Cf. Positronium in QED, v αem m mass mv momentum, inv. size mv 2 binding energy Frankfurt, Koepf, Strikman 98 Effective field theory approach: Non relativistic QCD, mv n expansion Lepage et al 92; Manohar 97; Brambilla 2; Kniehl et al. 22 Numerical: Potential models Eichten et al. 75; Quigg, Rosner 77 Typical c c distances r.2.3 fm 1 fm Transverse size in light cone wave function r 2 T = 2/3 r2 High momentum components with k m account for 3% of R (r = ) Decays J/ψ moderately small, relativistic
3 Heavy quarkonium: Size from lattice QCD γ µ Γ i Γ j Charmonium form factors Separate ground excited states using matrix of correlation functions Dudek et al. 6 Light quarks, hybrid mesons 1.8 temp. p f = () spat. p f = () temp. p f = (1) spat. p f = (1) Artificial J/ψ charge form factor from current with c c coupling G C J/ψ (Q 2 ).6.4 J/ψ charge radius r 2 1/2.26 fm Also η c, radiative transitions.2 J/psi "charge" form factor Dudek, Edwards, Richards Q 2 (GeV 2 )
4 Heavy quarkonium: Probe of color field Q 2 r T Use heavy quarkonium as probe of color fields in light hadrons Fields change with incident energy, size of Q Q configurations Multipole expansion: Dipole +... recoil Exclusive photo/electroproduction Target recoils: Gluonic form factor Q 2 tests/changes mix of Q Q sizes Theoretical challenges! Separate structures of target and probe (factorization), model gluonic structure of target Quarkonium hadron rescattering Theoretically simpler, but difficult to realize at low energies!
5 Photoproduction: Kinematics 11 P + (1 ζ) P, + Τ 11 t Exclusive production γn J/ψ +N Invariant momentum transfer grows near threshold t min,th = 2.2GeV 2 t min [GeV 2 ] Invariant momentum transfer m ψ 2 mn / (m ψ + m N ) Light cone variables ζ Plus momentum transfer, cf. x B large near threshold, but not x 1! T Transverse momentum transfer ζ min Longitudinal momentum transfer m ψ / (m ψ + m N ) t = (ζ 2 m 2 N + 2 T )/(1 ζ) Two regimes W W th t min = 1 2 GeV 2, ζ large cf. nucleon elastic form factors Cornell, SLAC, JLab 12 GeV threshold m ψ 2 /W W [GeV] W W th t min negligible, ζ 1 cf. diffractive processes FNAL, COMPASS, HERA, EIC
6 High W: QCD factorization and dipole picture l coh QCD factorization theorem Collins, Frankfurt, Strikman 96 r T x 1 x 2 N GPD t N Collinear factorization of amplitude GPD Hard scattering Meson dist. amp. GPD as transition matrix element of twist 2 operator: Gluonic form factor of nucleon x 1 = x 2,t = : Usual gluon density Integrand N F +i ()F +i (z ) N z 2 = light like distance Size distribution in integral. McDermott et al. Small sizes ~.1 fm Fixed mass Running mass Space time picture in rest frame Brodsky et al. 94 Coherence length l coh 1fm A = d 2 r T ψ γ (r T ) A Q QN(r T ) }{{} ψ J/ψ (r T ) r 2 T α s GPD(Scale r 2 T ) Distribution of Q Q sizes determined dynamically, changes with energy, electroproduction Q 2 Cf. Color tranparency.2.4 r T (fm) [fm] GPD as transition color dipole moment
7 High W: Data and interpretation Q 2 11 hard GPD T J /ψ φ, ρ b x gluons J/ψ photo/electroproduction at high W well understood HERA data, extensive literature Experimental tests of small size regime Universality of t slopes above Q 2 1GeV 2 GPD/dipole calc s describe cross sections Frankfurt et al. 95; Goloskokov, Kroll 8+;... Gluonic radius of nucleon b 2 g [fm 2 ] J/ψ, H1 5 J/ψ, ZEUS 2 µ + µ - J/ψ, ZEUS 2 e + e - J/ψ, FNAL 82 Fits COMPASS J/ψ JLab12 φ x Frankfurt, Strikman, CW 11, Q 2 3GeV 2 Transverse spatial distribution of gluons Fourier T b impact parameter Distribution changes with x and scale Q 2 : Parton diffusion, DGLAP evolution Fundamental gluonic size of nucleon in QCD: Gluon vs. quark radii, non pert. dynamics Input for small x physics: Evolution equations, saturation Needed for pp@lhc: Underlying event, multiparton processes, diffraction
8 Near threshold: Reaction mechanism local x 1 x ? J /ψ Near threshold kinematics Large t min, up to 2.2 GeV 2 Large longit. momentum transfer x 1 x 2 = ζ σ [nb] Slope B [GeV -2 ] threshold t SLAC 75 CERN 87 Cornell W [GeV] FNAL 82 FNAL 93 Reaction mechanism near threshold Strikman, CW, in progress γggj/ψ vertex local on scale R nucl 1fm Amp CF gg (t) local gluonic form factor. Energy dependence through F gg (t min ) Consistent with existing low energy data. Can be tested with JLab 12 GeV! Theoretical questions Matching collinear short distance expansion? Quantum numbers of gluonic operator? Behavior of two gluon form factor? Correlated configurations in nucleon LCWF? Cf. model of Brodsky, Chudakov, Hoyer, Laget
9 Near threshold: Nuclei and ψn interaction W 11 t Kinematics of ψn scattering t accessible at all W > W th Ideal process for probing color fields in hadrons and nuclei! Physics of low energy ψn interaction 2 Operator expansion: Dipole dipole interaction Fuji, Kharzeev 99 Lab momenta p ψ, p N [GeV] Threshold Total J/ψ N Van der Waals force of QCD Brodsky, Miller 97 Nuclear bound states? Brodsky, de Teramond 9; Luke, Manohar, Savage 92 Near threshold γa J/ψ +X p ψ m ψ m ψ 2m N J/ψ fast, relativistic! E γ [GeV] Produced J/ψ is fast How to study bound states?
10 Summary J/ψ as small size probe of color fields in hadrons moderately small, relativistic High W photo/electroproduction at probes gluon GPD Transverse spatial distribution of gluons at fixed x Near threshold photo/electroproduction probes local gluonic form factor Theory/phenomenology developing New physics accessible with JLab 12 GeV! J/ψ fast in photoproduction How to study low energy ψn interaction, bound states? Connections with other JLab 12 GeV experiments Small size q q configurations in high Q 2 meson production High t form factors gluon vs. quark operators? Color transparency different probes Nuclear short range correlations high momentum components in WF
Plans to measure J/ψ photoproduction on the proton with CLAS12
Plans to measure J/ψ photoproduction on the proton with CLAS12 Pawel Nadel-Turonski Jefferson Lab Nuclear Photoproduction with GlueX, April 28-29, 2016, JLab Outline Introduction J/ψ on the proton in CLAS12
More informationProbing Nuclear Color States with J/Ψ and φ
Probing Nuclear Color States with J/Ψ and φ Michael Paolone Temple University Next Generation Nuclear Physics with JLab12 and the EIC FIU - Miami, Florida February 12th 2016 J/Ψ and φ experiments at a
More informationσ tot (J/ψN) 3 4 mb Mark Strikman, PSU Jlab, March 26, 2011
J/ψ exclusive photoproduction off protons and nuclei near threshold Mark Strikman, PSU Application of VDM: σ V DM tot (J/ψN) 1 mb, σtot VDM (Ψ N) m2 (J/ψN) σ VDM tot J/ψ m 2 Ψ though r 2 Ψ r 2 J/ψ 4 QCD:
More informationCoherent and Incoherent Nuclear Exclusive Processes
Coherent and Incoherent Nuclear Exclusive Processes Vadim Guzey Electron-Ion Collider Workshop: Electron-Nucleon Exclusive Reactions Rutgers University, March 14-15, 2010 Outline Coherent and incoherent
More informationPoS(DIS 2010)071. Diffractive electroproduction of ρ and φ mesons at H1. Xavier Janssen Universiteit Antwerpen
Diffractive electroproduction of ρ and φ mesons at Universiteit Antwerpen E-mail: xavier.janssen@ua.ac.be Diffractive electroproduction of ρ and φ mesons is measured at HERA with the detector in the elastic
More informationThreshold Photo-production of J/5 Mesons J. Dunne Jefferson Lab
hreshold Photo-production of J/5 Mesons J. Dunne Jefferson Lab Introduction With the advent of higher energies at Jefferson Lab, the study of charmonium becomes possible. he threshold production of J/5
More informationPhotoproduction of J/ψ on Nuclei
Outline E.Chudakov SRC Workshop, Jlab 2007 Photoproduction of J/ψ on Nuclei 1 Photoproduction of J/ψ on Nuclei E.Chudakov 1 1 JLab SRC Workshop, Jlab 2007 E.Chudakov SRC Workshop, Jlab 2007 Photoproduction
More informationNuclear GPDs and DVCS in Collider kinematics. Vadim Guzey. Theory Center, Jefferson Lab. Outline
Nuclear GPDs and DVCS in Collider kinematics Vadim Guzey Theory Center, Jefferson Lab Introduction Outline Nuclear PDFs Nuclear GPDs Predictions for DVCS Conclusions Introduction e(k ) Deeply Virtual Compton
More informationHadron Propagation and Color Transparency at 12 GeV
Hadron Propagation and Color Transparency at 12 GeV Dipangkar Dutta Mississippi State University Hall C Users Meeting Jan 21-22, 2016 Hall C meeting Jan 2016 D. Dutta Hadron propagation in nuclear medium
More informationGluons at high x in Nuclei at EIC
Gluons at high x in Nuclei at EIC in collaboration with: E. Chudakov, D. Higinbotham, C. Hyde, C. Weiss Jefferson Lab DNP 2015 Fall meeting, Santa Fe, NM Outline Motivation HERA and ZEUS experience EIC
More informationProposal to Jefferson Lab PAC39 Exclusive Phi Meson Electroproduction with CLAS12
Proposal to Jefferson Lab PAC39 Exclusive Phi Meson Electroproduction with CLAS2 H. Avakian, J. Ball, 2 A. Biselli, 3 V. Burkert, R. Dupr, 2 L. Elouadrhiri, R. Ent, F. X. Girod,, S. Goloskokov, 4 B. Guegan,
More information3-D Imaging and the Generalized Parton Distribution Program at an Electron Ion Collider
Workshop on Precision Radiative Corrections for Next Generation Experiments 6 9 May 6, Jefferson Lab, Newport News VA 3-D Imaging and the Generalized Parton Distribution Program at an Electron Ion Collider
More informationOpportunities in low x physics at a future Electron-Ion Collider (EIC) facility
1 Opportunities in low x physics at a future Electron-Ion Collider (EIC) facility Motivation Quantum Chromo Dynamics Proton=uud Visible Universe Galaxies, stars, people, Silent Partners: Protons & Neutrons
More informationMulti parton interactions B.Blok (Technion)
Multi parton interactions MPI@LHC B.Blok (Technion) Introduction The conventional dijet production in high energy process:. 2 Realistic process however-more than I hard interactions-mpi. Can occur either
More informationJets and Diffraction Results from HERA
Jets and Diffraction Results from HERA A. Buniatyan DESY, Notkestrasse 5, 7 Hamburg, Germany for the H and ZEUS Collaborations he latest results on precision measurements of jet and diffractive cross sections
More informationNuclear shadowing in DIS, diffraction and high energy color transparency. + peek at HERA III at LHC. Mark Strikman, PSU
Nuclear shadowing in DIS, diffraction and high energy color transparency + peek at HERA III at LHC Mark Strikman, PSU EINN05, Milos, September 23, 2005 Outline Nuclear shadowing in DIS - is this obvious?
More informationSt anfo rd L in ear A ccele rat o r Cent e r
SLAC-PUB-7212 July 1996 NUCLEAR EFFECTS AT HERA STANLEY J. BRODSKY St anfo rd L in ear A ccele rat o r Cent e r St anfo rd University, St anfo rd, California 94 309 To appear in the Proceedings of the
More informationGPDs and TMDs at Electron-Ion Collider. Workshop on hadron tomography at J-PARC and KEKB January 6 th, 2017 KEK, Tsukuba, Japan Yuji Goto (RIKEN)
GPDs and TMDs at Electron-Ion Collider Workshop on hadron tomography at J-PARC and KEKB January 6 th, 2017 KEK, Tsukuba, Japan Yuji Goto (RIKEN) Electron-Ion Collider World s first polarized electron +
More information2. HEAVY QUARK PRODUCTION
2. HEAVY QUARK PRODUCTION In this chapter a brief overview of the theoretical and experimental knowledge of heavy quark production is given. In particular the production of open beauty and J/ψ in hadronic
More informationMulti parton interactions in UP collisions
Multi parton interactions in UP collisions B.Blok (Technion) University of Washington at Seattle February 2017 Introduction The conventional dijet production in high energy process:. 2 Realistic process
More informationPolarized deuterium physics with EIC C. Weiss (JLab), Tensor Polarized Solid Target Workshop, JLab, 11 Mar 14
Polarized deuterium physics with EIC C. Weiss (JLab), Tensor Polarized Solid Target Workshop, JLab, 11 Mar 14 1 e e x, 0000000 1111111 D pol. Q 2 X p, n Electron-Ion Collider overview Design specifications
More informationHeavy quark production and large-x nuclear gluons at EIC
Heavy quark production and large-x nuclear gluons at EIC C. Weiss (JLab), Santa Fe Jets and Heavy Flavor Workshop, -Jan-8 Nuclear partons e x e x B, Q c, b _ c, b _ Nuclear modifications NN interactions
More informationProbing the small-x regime through photonuclear reactions at LHC
Probing the small-x regime through photonuclear reactions at LHC 1/ 26 Probing the small-x regime through photonuclear reactions at LHC G.G. Silveira gustavo.silveira@ufrgs.br High Energy Physics Phenomenology
More informationExclusive VM electroproduction
Exclusive VM electroproduction γ * p V p V γ ρ ϕ ψ =,,, J /, ϒ Aharon Levy Tel Aviv University on behalf of the H and collaborations June, 28 A. Levy: Exclusive VM, GPD8, Trento Why are we measuring σ
More informationDiffractive vector meson leptoproduction and spin effects
Diffractive vector meson leptoproduction and spin effects Bogoliubov Laboratory of Theoretical Physics, Joint Institute for Nuclear Research, Dubna 141980, Moscow region, Russia E-mail: goloskkv@theor.jinr.ru
More informationColor Transparency: past, present and future
Color Transparency: past, present and future D. Dutta, 1 K. Hafidi, 2 M. Strikman 3 1 Mississippi State University, Mississippi State, MS 39762, USA 2 Argonne National Laboratory, Argonne, IL 60439, USA
More informationDiffractive dijet photoproduction in UPCs at the LHC
Diffractive dijet photoproduction in UPCs at the LHC V. Guzey Petersburg Nuclear Physics Institute (PNPI), National Research Center Kurchatov Institute, Gatchina, Russia Outline: l Diffractive dijet photoproduction
More informationExotic and excited-state radiative transitions in charmonium from lattice QCD
Exotic and excited-state radiative transitions in charmonium from lattice QCD Christopher Thomas, Jefferson Lab Hadron Spectroscopy Workshop, INT, November 2009 In collaboration with: Jo Dudek, Robert
More informationTransverse Target Asymmetry in Exclusive Charged Pion Production at 12 GeV
Transverse Target Asymmetry in Exclusive Charged Pion Production at 12 GeV Dipangkar Dutta Mississippi State University (with Dave Gaskell & Garth Huber) Polarized Target Workshop: June 17-18, 2010 Outline
More informationImaging the Proton via Hard Exclusive Production in Diffractive pp Scattering
Exclusive Reactions at High Momentum Transfer Jefferson Lab, Newport News, VA May 21-24, 2007 Imaging the Proton via Hard Exclusive Production in Diffractive pp Scattering Charles Earl Hyde Old Dominion
More informationNuclear Transparency in A(e,e π/k)x Status and Prospects
Nuclear Transparency in A(e,e π/k)x Status and Prospects Tanja Horn Small size configurations at high-t workshop 26 March 2011 1 Nuclear Transparency Color transparency (CT) is a phenomenon predicted by
More informationQCD Collinear Factorization for Single Transverse Spin Asymmetries
INT workshop on 3D parton structure of nucleon encoded in GPD s and TMD s September 14 18, 2009 QCD Collinear Factorization for Single Transverse Spin Asymmetries Iowa State University Based on work with
More informationPhysics at Hadron Colliders Partons and PDFs
Physics at Hadron Colliders Partons and PDFs Marina Cobal Thanks to D. Bettoni Università di Udine 1 2 How to probe the nucleon / quarks? Scatter high-energy lepton off a proton: Deep-Inelastic Scattering
More informationDiffractive rho and phi production in DIS at HERA
Xavier Janssen, on behalf of H and Collaborations. Université Libre de Bruxelles, Belgium. E-mail: xjanssen@ulb.ac.be These proceedings report on H and results on diffractive electroproduction of ρ and
More informationThe Longitudinal Photon, Transverse Nucleon, Single-Spin Asymmetry in Exclusive Pion Production
The Longitudinal Photon, Transverse Nucleon, Single-Spin Asymmetry in Exclusive Pion Production Garth Huber SoLID Collaboration, Jefferson Lab, May 15, 2015. Complementarity of Different Reactions Deep
More informationSingle Spin Asymmetry at large x F and k T
1 Single Spin Asymmetry at large x F and k T Paul Hoyer University of Helsinki Workshop on Transverse momentum, spin, and position distributions of partons in hadrons ECT*, 11-15 June 2007 PH and M. Järvinen,
More informationThe nucleon is an excitation of 3 quarks in the QCD vacuum. Understanding the vacuum structure and its properties, such as color confinement, is
The nucleon is an excitation of 3 quarks in the QCD vacuum. Understanding the vacuum structure and its properties, such as color confinement, is essential. Light quarks (up and down) are nearly massless,
More informationProbing nucleon structure by using a polarized proton beam
Workshop on Hadron Physics in China and Opportunities with 12 GeV Jlab July 31 August 1, 2009 Physics Department, Lanzhou University, Lanzhou, China Probing nucleon structure by using a polarized proton
More informationSearch for φ-n Bound State in Jefferson Lab Hall B
Search for φ-n Bound State in Jefferson Lab Hall B Haiyan Gao ( 高海燕 ) Duke University Jefferson Lab Theory Seminar, Oct. 20, 2008 1 QCD: still unsolved in non-perturbative region Gauge bosons: gluons (8)
More informationLattice QCD study of Radiative Transitions in Charmonium
Lattice QCD study of Radiative Transitions in Charmonium (with a little help from the quark model) Jo Dudek, Jefferson Lab with Robert Edwards & David Richards Charmonium spectrum & radiative transitions
More informationHigh-energy ea scattering. Spectator nucleon tagging. Future facilities. Energy, luminosity, polarization. Physics objectives with light nuclei
High-energy nuclear physics with spectator tagging A. Deshpande, D. Higinbotham, Ch. Hyde, S. Kuhn, M. Sargsian, C. Weiss Topical Workshop, Old Dominion U., 9 11 March 015 High-energy ea scattering e e
More informationColor dipoles: from HERA to EIC
Université de Moncton INT workshop: Gluons and the quark sea at high energies,distributions, polarisation, tomography September 29, 2010 based on work done with J. R. Forshaw, G.Shaw and B. E. Cox (Manchester
More informationMeson Radiative Transitions on the Lattice hybrids and charmonium. Jo Dudek, Robert Edwards, David Richards & Nilmani Mathur Jefferson Lab
Meson Radiative Transitions on the Lattice hybrids and charmonium Jo Dudek, Robert Edwards, David Richards & Nilmani Mathur Jefferson Lab 1 JLab, GlueX and photocouplings GlueX plans to photoproduce mesons
More informationMark Strikman PSU. for Boris Blok
Open charm production in Double Parton Scattering processes in forward kinematics Mark Strikman PSU for oris lok.lok M.Strikman MPI 16 arxiv:168.14; arxiv:1611.3649 in press Hard interaction ~ 1 ~ geometrical
More informationCharmonium Transitions
Hans Kuipers & Maikel de Vries Student Seminar on Subatomic Physics October 14, 2009 Outline n 2S+1 L J J PC Aspects of charmonium Charmonium is a mesonic bound state of c c. Charmonium produced in e e
More informationerhic: Science and Perspective
erhic: Science and Perspective Study of the Fundamental Structure of Matter with an Electron-Ion Collider A. Deshpande, R. Milner, R. Venugopalan, W. Vogelsang hep-ph/0506148, Ann. Rev. Nucl. Part. Sci.
More informationPerturbative Pion Wave function in Coherent Pion-Nucleon. Di-Jet Production
NT@UW-99-25 Perturbative Pion Wave function in Coherent Pion-Nucleon Di-Jet Production L. Frankfurt School of Physics and Astronomy, Tel Aviv University, 69978 Tel Aviv, Israel G. A. Miller Department
More informationGPDs. -- status of measurements -- a very brief introduction prerequisites and methods DVCS & DVMP: selected results on the way to an EIC
Delia Hasch GPDs -- status of measurements -- a very brief introduction prerequisites and methods & DVMP: selected results on the way to an EIC see additional slides for results not covered POETIC 01,
More informationIntroduction to High Energy Nuclear Collisions I (QCD at high gluon density) Jamal Jalilian-Marian Baruch College, City University of New York
Introduction to High Energy Nuclear Collisions I (QCD at high gluon density) Jamal Jalilian-Marian Baruch College, City University of New York Many thanks to my colleagues, A. Deshpande, F. Gelis, B. Surrow
More informationExciting opportunities at JLab GeV!
Exciting opportunities at JLab 25-75 GeV! JLab users town meeting, Newport News! March 16 2012! Kawtar Hafidi! Develop a common vision for the future! The future starts today! 40 - Today (2012), we are
More informationHadronization with JLab 6/12 GeV
Hadronization with JLab 6/12 GeV Next generation nuclear physics with JLab12 and EIC Florida International University February 10-13th, 2016 Lamiaa El Fassi (On behalf of EG2 and CLAS Collaborations) Outline
More informationPhotodisintegration of Light Nuclei
Photodisintegration of Light Nuclei Yordanka Ilieva for the CLAS Collaboration Motivation Two-body photodisintegration of deuteron Two-body photodisintegration of 3 He The 7th International Workshop on
More informationPANDA. antiproton Annihilation at DArmstadt
antiproton Annihilation at DArmstadt Physics programme Quark confinement: Charmonium spectroscopy Excited gluons: Exotic hybrid mesons & glueballs Nucleon spin puzzle: transverse quark spin distribution
More informationQuarkonium Production at J-PARC
Quarkonium Production at J-PARC Jen-Chieh Peng University of Illinois at Urbana-Champaign J-PARC Meeting for Spin and Hadron Physics RIKEN, April 7-8, 008 Outline Quarkonium Production at J-PARC with Unpolarized
More informationExperimental Aspects of Deep-Inelastic Scattering. Kinematics, Techniques and Detectors
1 Experimental Aspects of Deep-Inelastic Scattering Kinematics, Techniques and Detectors 2 Outline DIS Structure Function Measurements DIS Kinematics DIS Collider Detectors DIS process description Dirac
More informationALICE results on vector meson photoproduction in ultraperipheral p-pb and Pb-Pb collisions
ALICE results on vector meson photoproduction in ultraperipheral p-pb and Pb-Pb collisions Evgeny Kryshen (Petersburg Nuclear Physics Institute, Russia) for the ALICE collaboration INT workshop INT-17-65W
More informationNext-generation nuclear physics with JLab12 and EIC
Next-generation nuclear physics with JLab12 and EIC Topical Workshop, Florida International University, 10 13 Feb 2016 W. Brooks, R. Dupre, Ch. Hyde, M. Sargsian, C. Weiss (Organizers) Welcome! Physics
More informationarxiv: v1 [nucl-th] 17 Aug 2012
Color Transparency Gerald A. Miller Physics Department, Univ. of Washington, Seattle, Wa. 98195-1560, USA arxiv:1208.3668v1 [nucl-th] 17 Aug 2012 Abstract. Color transparency is the vanishing of nuclear
More informationDIFFRACTIVE DIJET PHOTOPRODUCTION AND THE OFF-DIAGONAL GLUON DISTRIBUTION a
DIFFRACTIVE DIJET PHOTOPRODUCTION AND THE OFF-DIAGONAL GLUON DISTRIBUTION a K. GOLEC BIERNAT,,J.KWIECIŃSKI, A.D.MARTIN Department of Physics, University of Durham, Durham DH LE, England H. Niewodniczański
More informationShape and Structure of the Nucleon
Shape and Structure of the Nucleon Volker D. Burkert Jefferson Lab Science & Technology Peer Review June 25-27, 2003 8/7/2003June 25, 2003 Science & Technology Review 1 Outline: From form factors & quark
More informationThe Structure of Hadrons
1 The Structure of Hadrons Paul Hoyer University of Helsinki CP 3 Inauguration 24 November 2009 What are Hadrons? Strongly interacting elementary particles 2 Hadrons are extended objects and can be classified
More informationSeeking the Shadowing in ea Processes. M. B. Gay Ducati. V. P. Gonçalves
Seeking the Shadowing in ea Processes M. B. Gay Ducati and V. P. Gonçalves InstitutodeFísica, Univ. Federal do Rio Grande do Sul Caixa Postal 15051, 91501-970 Porto Alegre, RS, BRAZIL Abstract: We consider
More informationFrom JLab12 to EIC: QCD in nuclei
The EIC Science case: a report on the joint BL/IT/JLab program Gluons and the quark sea at high energies: distributions, polarization, tomography Institute for uclear Theory, University of Washington,
More informationCGC effects on J/ψ production
CGC effects on J/ψ production Kirill Tuchin based on work with D. Kharzeev, G. Levin and M. Nardi 6th Winter Workshop on Nuclear Dynamics Jan.-9 Ocho Rios, Jamaica Introduction I Inclusive light hadron
More informationarxiv:hep-ph/ v1 4 Nov 1998
Gluon- vs. Sea quark-shadowing N. Hammon, H. Stöcker, W. Greiner 1 arxiv:hep-ph/9811242v1 4 Nov 1998 Institut Für Theoretische Physik Robert-Mayer Str. 10 Johann Wolfgang Goethe-Universität 60054 Frankfurt
More informationComplex Systems of Hadrons and Nuclei
1 European Graduate School Complex Systems of Hadrons and Nuclei Copenhagen - Giessen - Helsinki - Jyväskylä -Torino Measuring transverse size with virtual photons In-Medium Effects in Hadronic and Partonic
More informationAsmita Mukherjee Indian Institute of Technology Bombay, Mumbai, India
. p.1/26 Sivers Asymmetry in e + p e + J/ψ + X Asmita Mukherjee Indian Institute of Technology Bombay, Mumbai, India Single spin asymmetry Model for J/ψ production Formalism for calculating the asymmetry
More informationExperimental results on nucleon structure Lecture I. National Nuclear Physics Summer School 2013
Experimental results on nucleon structure Lecture I Barbara Badelek University of Warsaw National Nuclear Physics Summer School 2013 Stony Brook University, July 15 26, 2013 Barbara Badelek (Univ. of Warsaw
More informationCHAPTER 2 ELECTRON-PROTON COLLISION
CHAPTER ELECTRON-PROTON COLLISION.1 Electron-proton collision at HERA The collision between electron and proton at HERA is useful to obtain the kinematical values of particle diffraction and interaction
More informationThe Jefferson Lab 12 GeV Program
The Jefferson Lab 12 GeV Program The Jefferson Lab facilities have undergone a substantial upgrade, both of accelerator, CEBAF, and of the experimental installations. We will discuss the progress to completion
More informationDi-muon electroproduction with CLAS12
Di-muon electroproduction with CLAS1 S. Stepanyan (JLAB) CLAS collaboration meeting, June 16-18, 016 Ø Physics motivation for LOI: Double DVCS J/ψ-electroproduction Ø Detector configuration Background
More informationHadron-hadron Interactions
116 PN12 Nov, 2004 Hadron-hadron Interactions general considerations effective approaches microscopic approaches OPE methods Dyson-Schwinger constituent quark model chiral symmetry issues Eric Swanson
More informationMultiple hard scattering and parton correlations in the proton
Multiple hard scattering and parton correlations in the proton M. Diehl Deutsches Elektronen-Synchroton DESY QCD Evolution Workshop, Santa Fe, 12 May 2014 DESY Hadron-hadron collisions standard description
More informationThe 2011 Europhysics Conference on High Energy Physics Grenoble, July Riccardo Brugnera Padova University and INFN
The 2011 Europhysics Conference on High Energy Physics Grenoble, 21-27 July 2011 Riccardo Brugnera Padova University and INFN on behalf of the ZEUS Collaboration J/ J/ photo photoproduction production
More informationMultiple Parton Interactions Physics
Some entertaining aspects of Multiple Parton Interactions Physics Yuri Dokshitzer LPTHE, Jussieu, Paris & PNPI, St Petersburg GGI 13.09 2011 Multi-Parton Interactions work in collaboration with B.Blok,
More informationarxiv:hep-ph/ v2 24 Dec 1997
Proton-Proton Spin Correlations at Charm Threshold and Quarkonium Bound to Nuclei hep-ph/9708202 Guy F. de Téramond and Randall Espinoza Escuela de Física, Universidad de Costa Rica, San José, Costa Rica
More informationExclusive processes at Jefferson Lab
PRAMANA cfl Indian Academy of Sciences Vol. 61, No. 5 journal of November 2003 physics pp. 837 846 Exclusive processes at Jefferson Lab HAIYAN GAO 1;2 1 Department of Physics, Duke University, Durham,
More informationSummary of subtopic Imaging QCD Matter : Generalized parton distributions and exclusive reactions
Summary of subtopic Imaging QCD Matter : Generalized parton distributions and exclusive reactions of weeks 8 and 9 of the INT program Gluons and the quark sea at high energy: distributions, polarization,
More informationTransport Theoretical Studies of Hadron Attenuation in Nuclear DIS. Model Results Summary & Outlook
Transport Theoretical Studies of Hadron Attenuation in Nuclear DIS T. Falter, W. Cassing,, K. Gallmeister,, U. Mosel Contents: Motivation Model Results Summary & Outlook Motivation elementary en reaction
More informationHadron Physics with Real and Virtual Photons at JLab
Hadron Physics with Real and Virtual Photons at JLab Elton S. Smith Jefferson Lab Virtual photons shape of the nucleon Elastic scattering (form factors) Inelastic scattering (uark distributions) Exclusive
More informationStudy of Dimensional Scaling in Two- Body Photodisintegration of 3 He
Study of Dimensional Scaling in Two- Body Photodisintegration of 3 He Yordanka Ilieva CLAS Collaboration 2011 Fall Meeting of the APS Division on Nuclear Physics Meeting Michigan State University October
More informationMeasurements with Polarized Hadrons
Aug 15, 003 Lepton-Photon 003 Measurements with Polarized Hadrons T.-A. Shibata Tokyo Institute of Technology Contents: Introduction: Spin of Proton Polarized Deep Inelastic Lepton-Nucleon Scattering 1.
More informationarxiv:nucl-th/ v1 5 Sep 2000
Suppression of Quarkonium Production in Heavy Ion Collisions at RHIC and LHC arxiv:nucl-th/0009008v1 5 Sep 000 1. Introduction L. Gerland, L. Frankfurt, M. Strikman, H. Stöcker, W. Greiner Institut für
More informationMeasuring the gluon Sivers function at a future Electron-Ion Collider
Measuring the gluon Sivers function at a future Electron-Ion Collider Speaker: Liang Zheng Central China Normal University In collaboration with: E.C. Aschenauer (BNL) J.H.Lee (BNL) Bo-wen Xiao (CCNU)
More informationStudies of the hadronic component of the photon light-cone wave function using exclusive di-pion events at HERA
Submitted to the International Conference on High Energy Physics 6-22 August 2004, Beijing, China Abstract: 6-0250 Parallel Session: QCD soft interactions Studies of the hadronic component of the photon
More informationIntroduction to particle physics Lecture 7
Introduction to particle physics Lecture 7 Frank Krauss IPPP Durham U Durham, Epiphany term 2009 Outline 1 Deep-inelastic scattering and the structure of protons 2 Elastic scattering Scattering on extended
More informationMeasuring transverse size with virtual photons
Measuring transverse size with virtual photons 1 Paul Hoyer University of Helsinki Work done with Samu Kurki arxiv:0911.3011 arxiv:1101.4810 How to determine the size of the interaction region in electroproduction
More informationOpportunities with diffraction
Opportunities with diffraction Krzysztof Golec-Biernat Institute of Nuclear Physics in Kraków IWHSS17, Cortona, 2 5 April 2017 Krzysztof Golec-Biernat Opportunities with diffraction 1 / 29 Plan Diffraction
More informationElectron-Ion Collider for Nuclear and Particle Physics. Hugh Montgomery Jefferson Lab
Electron-Ion Collider for Nuclear and Particle Physics Hugh Montgomery Jefferson Lab Input to this Talk Abhay Deshpande's EICAC talk to Jefferson Lab Users http://www.jlab.org/conferences/ugm/talks/monday/deshpande.pdf
More informationUpdate on the Hadron Structure Explored at Current and Future Facilities
3D Nucleon Tomography Workshop Modeling and Extracting Methodology Update on the Hadron Structure Explored at Current and Future Facilities Jianwei Qiu September 25-29, 2017 Salamanca, Spin Atomic Structure
More informationEffective Field Theory for Nuclear Physics! Akshay Vaghani! Mississippi State University!
Effective Field Theory for Nuclear Physics! Akshay Vaghani! Mississippi State University! Overview! Introduction! Basic ideas of EFT! Basic Examples of EFT! Algorithm of EFT! Review NN scattering! NN scattering
More informationQCD Factorization Approach to Cold Nuclear Matter Effect
Physics Division Seminar April 25, 2016 Mini-symposium on Cold Nuclear Matter from Fixed-Target Energies to the LHC SCGP: Small Auditorium Rm 102, October 9-10, 2016 QCD Factorization Approach to Cold
More informationFactorisation in diffractive ep interactions. Alice Valkárová Charles University, Prague
Factorisation in diffractive ep interactions Alice Valkárová Charles University, Prague 8th International Workshop on Multiple Partonic Interactions at the LHC, San Cristóbal de las Casas, 2016 HERA collider
More informationCentral Questions in Nucleon Structure
Central Questions in Nucleon Structure Werner Vogelsang BNL Nuclear Theory QCD and Hadron Physics Town Meeting, 01/13/2007 Exploring the nucleon: Of fundamental importance in science Know what we are made
More informationSmall angle (Low Q 2 ) GDH sum rule experiments
Small angle (Low Q 2 ) GDH sum rule experiments A. Deur Jefferson Lab. Outline: Sum rules, GDH, Bjorken, spin polarizability sum rules; Usefulness and context; Measurements (published, being analyzed,
More informationSpin Physics Experiments at SLAC
SLAC-PUB-9269 June, 2002 Spin Physics Experiments at SLAC P. Bosted, for the E155/E155x Collaborations 1 Stanford Linear Accelerator Center, Stanford CA 94309 and Physics Dept., University of Massachusetts,
More informationMEIC Physics. Tanja Horn for the MEIC group. Jlab Users Meeting
MEIC Physics Tanja Horn for the MEIC group Jlab Users Meeting The Structure of the Proton Naïve Quark Model: proton = uud (valence quarks) QCD: proton = uud + uu + dd + ss + The proton sea has a non-trivial
More informationStrong interaction physics with an Electron Ion Collider
Strong interaction physics with an Electron Ion Collider C. Weiss (JLab), UNAM, Mexico City, 03 April 17 [E-mail] Internal structure of nucleon Quantum Chromodynamics Concepts and methods for structure
More informationNeutron structure with spectator tagging at MEIC
Neutron structure with spectator tagging at MEIC C. Weiss (JLab), Users Group Workshop 2014, JLab, 03 Jun 14 Light ion physics with EIC e D pol. e p, n High energy process Forward spectators detected Physics
More informationHigher Fock states and power counting in exclusive charmonium decays
Higher Fock states and power counting in exclusive charmonium decays WU B 98-15 hep-ph/9807470 P. Kroll 1 arxiv:hep-ph/9807470v1 23 Jul 1998 Fachbereich Physik, Universität Wuppertal Gaußstrasse 20, D-42097
More information