Deep Inelastic Scattering On Nuclear Targets at
|
|
|
- Phoebe Matthews
- 5 years ago
- Views:
Transcription
1 Deep Inelastic Scattering On Nuclear Targets at Beni Zihlmann NIKHEF NIKHEF Jaarvergadering p./4
2 Deep Inelastic Scattering Electron Scattering on H, H, 3 He, 4 N, Ne, 84 Kr NIKHEF Jaarvergadering p./4
3 Deep Inelastic Scattering Electron Scattering on H, H, 3 He, 4 N, Ne, 84 Kr Inclusive Scattering e(e,)x Nucleon structure in Nucleus Nuclear Dependence R A = R D? NIKHEF Jaarvergadering p./4
4 Deep Inelastic Scattering Electron Scattering on H, H, 3 He, 4 N, Ne, 84 Kr Inclusive Scattering e(e,)x Nucleon structure in Nucleus Nuclear Dependence R A = R D? Semi Inclusive Scattering e(e,h)x Nuclear Attenuation Hadron formation time and energy loss Heavy Ion collisions NIKHEF Jaarvergadering p./4
5 Deep Inelastic Scattering Electron Scattering on H, H, 3 He, 4 N, Ne, 84 Kr Inclusive Scattering e(e,)x Nucleon structure in Nucleus Nuclear Dependence R A = R D? Semi Inclusive Scattering e(e,h)x Nuclear Attenuation Hadron formation time and energy loss Heavy Ion collisions Exclusive Scattering e(e,h)r Coherent, Incoherent ρ production positive slope in Transparency NIKHEF Jaarvergadering p./4
6 Inclusive Scattering Cross Section Ratio on the Born level lepton k k θ γ* q=k-k nucleon p p x NIKHEF Jaarvergadering p.3/4
7 Inclusive Scattering lepton Cross Section Ratio on the Born level k k θ γ* q=k-k Q = q = (k k ) x = q P q = Q Mν y = P q P e = E E E = ν E nucleon p p x NIKHEF Jaarvergadering p.3/4
8 Inclusive Scattering lepton Cross Section Ratio on the Born level k nucleon k θ γ* p q=k-k p x Q = q = (k k ) x = q P q = Q Mν y = P q P e = E E E W = (p + q) = ν E > 4 GeV (DIS) NIKHEF Jaarvergadering p.3/4
9 Inclusive Scattering lepton Cross Section Ratio on the Born level k nucleon k θ γ* p q=k-k p x Q = q = (k k ) x = q P q = Q Mν y = P q P e = E E E W = (p + q) = ν E > 4 GeV (DIS) σ A Born σ D Born = F A F D ( + ɛr A )( + R D ) ( + R A )( + ɛr D ) NIKHEF Jaarvergadering p.3/4
10 Inclusive HERMES Results σ A /σ D HERMES, 84 Kr SLAC, 56 Fe NMC, 9 Sn HERMES, 4 N SLAC, C NMC, C Cross section ratio σ Kr σ D, σ N σd and σ He σ D HERMES data agree within errors with NMC HERMES, 3 He SLAC, 4 He NMC, 4 He - - x NIKHEF Jaarvergadering p.4/4
11 Inclusive HERMES Results σ A /σ D HERMES, 84 Kr SLAC, 56 Fe NMC, 9 Sn HERMES, 4 N SLAC, C NMC, C Cross section ratio σ Kr σ D, σ N σd and σ He σ D HERMES data agree within errors with NMC extend to low Q HERMES, 3 He SLAC, 4 He NMC, 4 He - - x NIKHEF Jaarvergadering p.4/4
12 Inclusive HERMES Results σ A /σ D HERMES, 84 Kr SLAC, 56 Fe NMC, 9 Sn HERMES, 4 N SLAC, C NMC, C Cross section ratio σ Kr σ D, σ N σd and σ He σ D HERMES data agree within errors with NMC extend to low Q extract R A /R D HERMES, 3 He SLAC, 4 He NMC, 4 He - - x NIKHEF Jaarvergadering p.4/4
13 Fit cross section ratio R(ɛ) for fixed x Extraction of R A /R D σ N /σ D. <x> =.5 <x> =.75 <x> =.5. <x> =.35 <x> =.45 <x> =.55.. <x> =.7 <x> =.9 <x> =.5 <x> =.75 <x> =.5 <x> = ε parameter Fit: F A F D solid line, R A R D NIKHEF Jaarvergadering p.5/4
14 Fit cross section ratio R(ɛ) for fixed x Extraction of R A /R D σ N /σ D. <x> =.5 <x> =.75 <x> =.5. <x> =.35 <x> =.45 <x> =.55.. <x> =.7 <x> =.9 <x> =.5 <x> =.75 <x> =.5 <x> = ε parameter Fit: F A F D solid line, R A R D Parameterization of R D for each x bin agrees with NMC F A F D NIKHEF Jaarvergadering p.5/4
15 Fit cross section ratio R(ɛ) for fixed x Extraction of R A /R D σ N /σ D. <x> =.5 <x> =.75 <x> =.5. <x> =.35 <x> =.45 <x> =.55.. <x> =.7 <x> =.9 <x> =.5 <x> =.75 <x> =.5 <x> = ε parameter Fit: F A F D solid line, R A R D Parameterization of R D for each x bin agrees with NMC F A F D parameter Fit: fix F A F D dashed line R A R D for each x bin NIKHEF Jaarvergadering p.5/4
16 New HERMES Results for R A /R D R A /R D < x <.3 HERMES(Kr/D) HERMES(N/D) HERMES( 3 He/D) NMC(C/D) NMC( 4 He/D) NMC(Sn/D) NMC(Ca/D) SLAC(Ca/D).3 < x <.6.6 < x <.5.5 < x < Q (GeV ) HERMES finds R A consistent with R D NIKHEF Jaarvergadering p.6/4
17 New HERMES Results for R A /R D R A /R D < x <.3 HERMES(Kr/D) HERMES(N/D) HERMES( 3 He/D) NMC(C/D) NMC( 4 He/D) NMC(Sn/D) NMC(Ca/D) SLAC(Ca/D) The Future holds.3 < x <.6.6 < x <.5.5 < x < Q (GeV ) HERMES finds R A consistent with R D NIKHEF Jaarvergadering p.6/4
18 New HERMES Results for R A /R D R A /R D < x <.3 HERMES(Kr/D) HERMES(N/D) HERMES( 3 He/D) NMC(C/D) NMC( 4 He/D) NMC(Sn/D) NMC(Ca/D) SLAC(Ca/D) The Future holds σ D σ H at 7 GeV (Jan Visser).3 < x <.6.6 < x <.5.5 < x < Q (GeV ) HERMES finds R A consistent with R D NIKHEF Jaarvergadering p.6/4
19 New HERMES Results for R A /R D R A /R D < x <.3.3 < x <.6.6 < x <.5 HERMES(Kr/D) HERMES(N/D) HERMES( 3 He/D) NMC(C/D) NMC( 4 He/D) NMC(Sn/D) NMC(Ca/D) SLAC(Ca/D) The Future holds σ D σ H at 7 GeV (Jan Visser) Data on Kr, N, H, H at GeV extend to lower Q.5 < x < Q (GeV ) HERMES finds R A consistent with R D NIKHEF Jaarvergadering p.6/4
20 New HERMES Results for R A /R D R A /R D < x <.3.3 < x <.6.6 < x <.5 HERMES(Kr/D) HERMES(N/D) HERMES( 3 He/D) NMC(C/D) NMC( 4 He/D) NMC(Sn/D) NMC(Ca/D) SLAC(Ca/D) The Future holds σ D σ H at 7 GeV (Jan Visser) Data on Kr, N, H, H at GeV extend to lower Q.5 < x < Q (GeV ) HERMES finds R A E99-8(Vladas Tvaskis) direct measurement of R A consistent with R D NIKHEF Jaarvergadering p.6/4
21 Semi Inclusive DIS l lepton k k θ γ* q=k-k h nucleon p p x NIKHEF Jaarvergadering p.7/4
22 Semi Inclusive DIS l Q = q = (k k ) lepton k k θ q=k-k γ* h x = q P q = Q Mν y = P q P e = E E E = ν E nucleon p p x NIKHEF Jaarvergadering p.7/4
23 Semi Inclusive DIS l Q = q = (k k ) lepton k k θ q=k-k γ* h x = q P q = Q Mν y = P q P e = E E E ν = E E = ν E nucleon p p x z = E h ν NIKHEF Jaarvergadering p.7/4
24 Semi Inclusive DIS l Q = q = (k k ) lepton k k θ q=k-k γ* h x = q P q = Q Mν y = P q P e = E E E ν = E E = ν E nucleon p p x z = E h ν R h att(ν, z) = d σ SIDIS σ DIS (ν) dνdz A σ DIS (ν) d σ SIDIS dνdz D RICH identify π ± K ± p ± NIKHEF Jaarvergadering p.7/4
25 Attenuation Ratios multiplicity ratio for 84 Kr / D z ν [GeV] Q [GeV ] multiplicity ratio for 84 Kr / D ν [GeV] z Q [GeV ] NIKHEF Jaarvergadering p.8/4
26 Attenuation Ratios multiplicity ratio for 84 Kr / D z ν [GeV] π + and π consistent Q [GeV ] multiplicity ratio for 84 Kr / D ν [GeV] z Q [GeV ] NIKHEF Jaarvergadering p.8/4
27 Attenuation Ratios multiplicity ratio for 84 Kr / D z ν [GeV] π + and π consistent Q [GeV ] multiplicity ratio for 84 Kr / D ν [GeV] z Q [GeV ] K + larger than K NIKHEF Jaarvergadering p.8/4
28 Attenuation Ratios multiplicity ratio for 84 Kr / D z ν [GeV] π + and π consistent K + larger than K Q [GeV ] multiplicity ratio for 84 Kr / D ν [GeV] p + very different p p + > at low z z Q [GeV ] NIKHEF Jaarvergadering p.8/4
29 Models of Attenuation Hadron Formation Time t Nuclear Absorption formed hadron scatters in nuclear medium A /3 τ f NIKHEF Jaarvergadering p.9/4
30 Models of Attenuation Hadron Formation Time t Nuclear Absorption formed hadron scatters in nuclear medium A /3 Gluon Bremsstrahlung (QCD) multiple parton scattering A /3 τ f NIKHEF Jaarvergadering p.9/4
31 Models of Attenuation Hadron Formation Time t Nuclear Absorption formed hadron scatters in nuclear medium A /3 Gluon Bremsstrahlung (QCD) multiple parton scattering A /3 Combined analysis of Nitrogen and Krypton data Thesis Erika Garutti τ f NIKHEF Jaarvergadering p.9/4
32 Models of Attenuation Hadron Formation Time t Nuclear Absorption formed hadron scatters in nuclear medium A /3 Gluon Bremsstrahlung (QCD) multiple parton scattering A /3 Combined analysis of Nitrogen and Krypton data Thesis Erika Garutti τ f NIKHEF Jaarvergadering p.9/4
33 SIDIS at HERMES Prospects Results on Helium and Neon at 7.5 GeV beam energy NIKHEF Jaarvergadering p./4
34 SIDIS at HERMES Prospects Results on Helium and Neon at 7.5 GeV beam energy Analysis on GeV data (low ν range) Paul van der Nat NIKHEF Jaarvergadering p./4
35 SIDIS at HERMES Prospects Results on Helium and Neon at 7.5 GeV beam energy Analysis on GeV data (low ν range) Paul van der Nat New Data on heavier targets explore A dependence NIKHEF Jaarvergadering p./4
36 Exclusive ρ production lcoh rho N N NIKHEF Jaarvergadering p./4
37 Exclusive ρ production lcoh rho N N Hadronic Structure of virtual photon size of virtual q q-pair NIKHEF Jaarvergadering p./4
38 Exclusive ρ production lcoh rho N N Hadronic Structure of virtual photon size of virtual q q-pair VM interaction in nuclear medium Nuclear transparency NIKHEF Jaarvergadering p./4
39 Exclusive ρ production lcoh rho N N Hadronic Structure of virtual photon size of virtual q q-pair VM interaction in nuclear medium Nuclear transparency Coherence length l c = ν Q +M q q NIKHEF Jaarvergadering p./4
40 Coherent and Incoherent Scattering Transparency Ratios dσ dt e bt NIKHEF Jaarvergadering p./4
41 Coherent and Incoherent Scattering Transparency Ratios dσ dt e bt T coh = σ A coh /Aσp NIKHEF Jaarvergadering p./4
42 Coherent and Incoherent Scattering Transparency Ratios dσ dt e bt T coh = σ A coh /Aσp T incoh = σ A incoh /Aσp NIKHEF Jaarvergadering p./4
43 Coherent and Incoherent Scattering Transparency Ratios dσ dt e bt T coh = σ A coh /Aσp T incoh = σ A incoh /Aσp R = σ A coh /σa incoh NIKHEF Jaarvergadering p./4
44 Coherent and Incoherent Scattering Transparency Ratios dσ dt e bt T coh = σ A coh /Aσp T incoh = σ A incoh /Aσp R = σ A coh /σa incoh T (l c, Q ) and R(l c, Q ) Need to fix l c NIKHEF Jaarvergadering p./4
45 Q [GeV] Coherence length effects 4 4 lcoh [fm] NIKHEF Jaarvergadering p.3/4
46 lcoh =.35 fm lcoh =.45 fm lcoh =.55 fm lcoh =.65 fm lcoh =.75 fm lcoh =.85 fm lcoh =.95 fm lcoh =.5 fm lcoh =.5 fm lcoh =.5 fm lcoh =.35 fm lcoh =.45 fm (lcoh,q ) / A σ p Q [GeV] Coherence length effects N σ coh lcoh [fm] Q [GeV ] NIKHEF Jaarvergadering p.3/4
47 lcoh =.35 fm lcoh =.45 fm lcoh =.55 fm lcoh =.65 fm lcoh =.75 fm lcoh =.85 fm lcoh =.95 fm lcoh =.5 fm lcoh =.5 fm lcoh =.5 fm lcoh =.35 fm lcoh =.45 fm (lcoh,q ) / A σ p Q [GeV] Coherence length effects N σ coh lcoh [fm] 4 4 Q [GeV ] Fit T (Q ) at fixed lc with one slope parameter bcoh =.7 ±.4 bincoh =.89 ±.47 combined: b =.74 ±. positive slope! NIKHEF Jaarvergadering p.3/4
48 Conclusions Extend world data in Q (<GeV ) NIKHEF Jaarvergadering p.4/4
49 Conclusions Extend world data in Q (<GeV ) R A consistent with R D NIKHEF Jaarvergadering p.4/4
50 Conclusions Extend world data in Q (<GeV ) R A consistent with R D Flavor dependence of hadron attenuation NIKHEF Jaarvergadering p.4/4
51 Conclusions Extend world data in Q (<GeV ) R A consistent with R D Flavor dependence of hadron attenuation Formation time of mesons and baryons NIKHEF Jaarvergadering p.4/4
52 Conclusions Extend world data in Q (<GeV ) R A consistent with R D Flavor dependence of hadron attenuation Formation time of mesons and baryons Nuclear Transparency and T (l c, Q ) NIKHEF Jaarvergadering p.4/4
HADRONIZATION IN A NUCLEAR ENVIRONMENT. Nationaal Instituut voor Kernfysica en Hoge-Energiefysica, NIKHEF
98 7 HADRONIZATION IN A NUCLEAR ENVIRONMENT J. J. VAN HUNEN (for the HERMES collaboration) Nationaal Instituut voor Kernfysica en Hoge-Energiefysica, NIKHEF Postbus 41882, 1009 DB Amsterdam, The Netherlands
Studies of hadronization in nuclei at HERMES
Studies of hadronization in nuclei at HERMES H.P. Blok (VU/NIKHEF) (on behalf of the HERMES collaboration) Why? How? What? Next? Hadronization workshop Trento, Oct. 2005 Motivation Hadronization is a non-perturbative
Transport 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
THE NUCLEUS AS A QCD LABORATORY: HADRONIZATION, 3D TOMOGRAPHY, AND MORE
rhtjhtyhy EINN 2017 NOVEMBER 1, 2017 PAPHOS, CYPRUS THE NUCLEUS AS A QCD LABORATORY: HADRONIZATION, 3D TOMOGRAPHY, AND MORE KAWTAR HAFIDI Argonne National Laboratory is a U.S. Department of Energy laboratory
Hadronization 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
Measurements 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.
Description of the HERMES Data on Hadronization in Nuclear Medium in Framework of the String Model
Description of the HERMES Data on Hadronization in Nuclear Medium in Framework of the String Model L.Grigoryan Yerevan Physics Institute ECT*, September 29, 2005 Introduction The TSM and ITSM Q 2 dependence
Nuclear attenuation 2 dimensional dependences at HERMES
Nuclear attenuation dimensional dependences at HERMES Inti Lemann University of Glasgow for te HERMES Collaboration DIS, Florence, /4/ Experimental Metod Semi-Inclusive DIS (SIDIS) on te Nucleon Access
Experimental 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
Electron-Positron Annihilation
Evidence for Quarks The quark model originally arose from the analysis of symmetry patterns using group theory. The octets, nonets, decuplets etc. could easily be explained with coloured quarks and the
Inelastic scattering
Inelastic scattering When the scattering is not elastic (new particles are produced) the energy and direction of the scattered electron are independent variables, unlike the elastic scattering situation.
Status report of Hermes
Status report of Hermes Delia Hasch Physics Research Committee, DESY Oct 27/28 2004 Spin physics: finalised and new results on: inclusive, semi-inclusive and exclusive measurements nuclear effects data
Study of Strange Quark in the Nucleon with Neutrino Scattering
July 28, 2004 NuFact 04, Osaka Study of Strange Quark in the Nucleon with Neutrino Scattering T.-A. Shibata Tokyo Institute of Technology Contents: 3. Physics Motivation --- Quark Structure of the Nucleon
Deep Inelastic Scattering (DIS) Un-ki Yang Dept. of Physics and Astronomy Seoul National University Un-ki Yang - DIS
Deep Inelastic Scattering (DIS) Un-ki Yang Dept. of Physics and Astronomy Seoul National University ukyang@snu.ac.kr Un-ki Yang - DIS 1 Elastic and Inelastic scattering Electron-Proton Scattering P Electron-proton
Electroproduction of hadrons in nuclei
Electroproduction o hadrons in nuclei Nicola Bianchi Bianchi@ln.inn.it Fragmentation Function modiications in the nuclear medium HERMES recent and new results Expectations rom CLAS Interpretations Workshop
Overview of recent HERMES results
Journal of Physics: Conference Series PAPER OPEN ACCESS Overview of recent HERMES results To cite this article: Hrachya Marukyan and 216 J. Phys.: Conf. Ser. 678 1238 View the article online for updates
Threshold 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
Hadron multiplicities at the HERMES experiment
A. I. Alikhanyan National Science Laboratory, Yerevan, Armenia E-mail: gevkar@mail.desy.de The HERMES collaboration has measured charge-separated pion and kaon multiplicities in semiinclusive deep-inelastic
Quark model. Jan 30, 2006 Lecture 8 1
Quark model Jan 30, 2006 Lecture 8 1 Quark model of hadrons!!!! Developed long before QCD was recognized as the appropriate quantum field theory of the strong interactions Postulate that 1.! All baryons
Photoproduction 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
Physics 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
Nucleon Valence Quark Structure
Nucleon Valence Quark Structure Z.-E. Meziani, S. Kuhn, O. Rondon, W. Melnitchouk Physics Motivation Nucleon spin and flavor structure High-x quark distributions Spin-flavor separation Moments of structure
Nuclear 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
DEEP INELASTIC SCATTERING
DEEP INELASTIC SCATTERING Electron scattering off nucleons (Fig 7.1): 1) Elastic scattering: E = E (θ) 2) Inelastic scattering: No 1-to-1 relationship between E and θ Inelastic scattering: nucleon gets
The Development of Particle Physics. Dr. Vitaly Kudryavtsev E45, Tel.:
The Development of Particle Physics Dr. Vitaly Kudryavtsev E45, Tel.: 0114 4531 v.kudryavtsev@sheffield.ac.uk The structure of the nucleon Electron - nucleon elastic scattering Rutherford, Mott cross-sections
Hadron 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
The Detector Design of the Jefferson Lab EIC
The Detector Design of the Jefferson Lab EIC Jefferson Lab E-mail: mdiefent@jlab.org The Electron-Ion Collider (EIC) is envisioned as the next-generation U.S. facility to study quarks and gluons in strongly
FUTURE SPIN EXPERIMENTS AT SLAC
SLAC-PUB-9658 February 2003 FUTURE SPIN EXPERIMENTS AT SLAC Stephen Rock for the Real Photon Collaboration University of Mass, Amherst MA 01003 Abstract. A series of three photo-production experiments
Nuclear effects in deep-inelastic scattering
Nuclear effects in deep-inelastic scattering Sergei Kulagin (INR, Moscow) Talk at JLab Theory Center October 8, 200 Typeset by FoilTEX Outline Brief summary of experimental evidence of nuclear effects
GENERALIZED PARTON DISTRIBUTIONS
Exploring fundamental questions of NUCLEON STRUCTURE with GENERALIZED PARTON DISTRIBUTIONS Florian Herrmann 16.9.2012 Corfu Summer School LHC COMPASS SPS Versatile facility for hadron structure studies
Hadron Production Generators: Progress
Rakitha S. Beminiwattha SoLID Collaboration Meeting January 12 th, 2016 1/19 Hadron Production Generators: Progress Rakitha S. Beminiwattha Department of Physics, Syracuse University January 12 th, 2016
COMPASS results on inclusive and semi inclusive polarised DIS
COMPASS results on inclusive and semi inclusive polarised DIS Helena Santos LIP - Lisboa on behalf of the COMPASS Collaboration The nucleon spin The COMPASS experiment Longitudinal spin structure functions
PHY357 Lecture 14. Applications of QCD. Varying coupling constant. Jets and Gluons. Quark-Gluon plasma. Colour counting
PHY357 Lecture 14 Applications of QCD Varying coupling constant Jets and Gluons Quark-Gluon plasma Colour counting The proton structure function (not all of section 5.8!) Variable Coupling Constants! At
Single 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,
High Energy Physics. Lecture 9. Deep Inelastic Scattering Scaling Violation. HEP Lecture 9 1
High Energy Physics Lecture 9 Deep Inelastic Scattering Scaling Violation HEP Lecture 9 1 Deep Inelastic Scattering: The reaction equation of DIS is written e+ p e+ X where X is a system of outgoing hadrons
Probing 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
Standard Model of Particle Physics SS 2013
Lecture: Standard Model of Particle Physics Heidelberg SS 013 Weak Interactions II 1 Important Experiments Wu-Experiment (1957): radioactive decay of Co60 Goldhaber-Experiment (1958): radioactive decay
Experimental Program of the Future COMPASS-II Experiment at CERN
Experimental Program of the Future COMPASS-II Experiment at CERN Luís Silva LIP Lisbon lsilva@lip.pt 24 Aug 2012 On behalf of the COMPASS Collaboration co-financed by THE COMPASS EXPERIMENT Common Muon
Subleading-twist effects in single-spin asymmetries in semi-inclusive DIS on a longitudinally polarized hydrogen target
Subleading-twist effects in single-spin asymmetries in semi-inclusive DIS on a longitudinally polarized hydrogen target G Schnell, H Ohsuga, H Tanaka, T Hasegawa, T Kobayashi, Y Miyachi, T-A Shibata Tokyo
Evidence for the Strong Interaction
Evidence for the Strong Interaction Scott Wilbur Scott Wilbur Evidence for the Strong Interaction 1 Overview Continuing search inside fundamental particles Scott Wilbur Evidence for the Strong Interaction
Diffraction at HERA. On behalf of H1 and ZEUS collaboations. Laurent Schoeffel CEA Saclay, Irfu/SPP. Paris 2011
Diffraction at HERA On behalf of H1 and ZEUS collaboations Laurent Schoeffel CEA Saclay, Irfu/SPP Paris 2011 1 1 st part: Inclusive diffraction at HERA and the dynamical structure of the proton at low
Electron-Ion Collider Taking us to the next QCD Frontier
QCD Evolution 2014 Workshop at Santa Fe, NM (May 12 16, 2014) Electron-Ion Collider Taking us to the next QCD Frontier Jianwei Qiu Brookhaven National Laboratory Acknowledgement: Much of the physics presented
GlueX Capabilities for Nuclear Photoproduction
GlueX Capabilities for Nuclear Photoproduction A. Somov, Jefferson Lab Nuclear Photoproduction with GlueX April 28 29, 2016 Physics Topics with Nuclear Targets Considered for GlueX Photoproduction of vector
Zhong-Bo Kang Los Alamos National Laboratory
Introduction to pqcd and Jets: lecture 1 Zhong-Bo Kang Los Alamos National Laboratory Jet Collaboration Summer School University of California, Davis July 19 1, 014 Selected references on QCD! QCD and
Overview of Elementary Particle Physics
Overview of Elementary Particle Physics Michael Gold Physics 330 May 3, 2006 Overview of Elementary Particle Physics Rutherford e p elastic elastic scattering e p inelastic scattering zeus Parton model
Introduction to Neutrino Interaction Physics NUFACT08 Summer School June 2008 Benasque, Spain Paul Soler
Introduction to NUCT08 Summer School -3 June 008 Benasque, Spain Paul Soler 4. uasi-elastic, resonant, coherent and diffractive scattering 4. Motivation 4. Charged current quasi-elastic scattering 4.3
Physics at LHC. lecture one. Sven-Olaf Moch. DESY, Zeuthen. in collaboration with Martin zur Nedden
Physics at LHC lecture one Sven-Olaf Moch Sven-Olaf.Moch@desy.de DESY, Zeuthen in collaboration with Martin zur Nedden Humboldt-Universität, October 22, 2007, Berlin Sven-Olaf Moch Physics at LHC p.1 LHC
Exclusive J/ψ production and gluonic structure
Exclusive J/ψ production and gluonic structure C. Weiss (JLab), Exclusive Meson Production Workshop, JLab, 22 24 Jan 25 Quarkonium size and structure Parametric: Dynamical scales Numerical: Potential models,
Nuclear 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
Subatomic Physics: Particle Physics Study Guide
Subatomic Physics: Particle Physics Study Guide This is a guide of what to revise for the exam. The other material we covered in the course may appear in uestions but it will always be provided if reuired.
Physics at HERA. Summer Student Lectures August Katja Krüger Kirchhoff Institut für Physik H1 Collaboration
Physics at HERA Summer Student Lectures 10 13 August 009 Kirchhoff Institut für Physik H1 Collaboration email: katja.krueger@desy.de Overview Introduction to HERA Inclusive DIS & Structure Functions formalism
Color 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
M.Battaglieri Istituto Nazionale di Fisica Nucleare Genova - Italy. A Forward Photon Tagging Facility for CLAS12
A Forward Photon Tagging Facility for CLAS12 M.Battaglieri Istituto Nazionale di Fisica Nucleare Genova - Italy 1) From CEBAF at 6 GeV 2) From CEBAF at 6 GeV to CEBAF at 12 GeV add Hall D (and beam line)
Studying Nuclear Structure
Microscope for the Studying Nuclear Structure with s School of Physics Seoul National University November 15, 2004 Outline s Microscope for the s Smaller, smaller Quest for basic building blocks of the
Nucleons in the Nuclear Environment
Nucleons in the Nuclear Environment "The next seven years..." John Arrington Argonne National Lab Topic: Study of nucleons (hadrons, quarks) in nuclei 1 - The EMC effect and related measurements 2 - Color
Hadron 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
Nuclear aspects of neutrino energy reconstruction in current oscillation experiments
Nuclear aspects of neutrino energy reconstruction in current oscillation experiments Tina Leitner Oliver Buss, Luis Alvarez-Ruso, and Ulrich Mosel Institut für Theoretische Physik Universität Gießen, Germany
Seeking 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
Experimental 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
SEARCH FOR THE ONSET OF COLOR TRANSPARENCY ELECTROPRODUCTION ON NUCLEI. Outline
SEARCH FOR THE ONSET OF COLOR TRANSPARENCY THROUGH ρ 0 ELECTROPRODUCTION ON NUCLEI Outline 1 introduction 2 Theoretical introduction 3 Experiments 4 CLAS EG2 5 Results 6 Future ρ 0 measurements at JLAB
The Role of Heavy Quarks in Light Hadron Fragmentation. HUGS Manuel Epele Instituto de Física La Plata
The Role of Heavy Quarks in Light Hadron Fragmentation. In collaboration with C. A. Garcia Canal and R. Sassot HUGS 2016 Jefferson Lab, Newport News, Virginia June, 2016 Outline Fragmentation Functions
arxiv: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
St 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
Probing the Atomic Nucleus at Jefferson Lab
Probing the Atomic Nucleus at Jefferson Lab (a glimpse ) Fatiha Benmokhtar Duquesne University. *Thanks to R. Ent for some of the material 1 Building Blocks of Matter Electrons Atom Nucleus -Most of the
Calculation of the Gluon Distribution Function Using Alternative Method for the Proton Structure Function
Commun. Theor. Phys. (Beijing, China 40 (2003 pp. 551 557 c International Academic Publishers Vol. 40, No. 5, November 15, 2003 Calculation of the Gluon Distribution Function Using Alternative Method for
3-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
SPIN STRUCTURE OF THE NUCLEON AND POLARIZATION. Charles Y. Prescott Stanford Linear Accelerator Center Stanford University, Stanford CA 94309
SLAC-PUB-662 September 1994 (TE) SPIN STRUCTURE OF THE NUCLEON AND POLARIZATION Charles Y. Prescott Stanford Linear Accelerator Center Stanford University, Stanford CA 9439 Work supported by Department
Spin Structure of the Deuteron from the CLAS/EG1b Data
Spin Structure of the Deuteron from the CLAS/EGb Data Nevzat Guler (the CLAS Collaboration) Old Dominion University OUTLINE Formalism Experimental setup Data analysis Results Parameterizations Conclusion
Helicity: Experimental Status. Matthias Grosse Perdekamp, University of Illinois
Helicity: Experimental Status Matthias Grosse Perdekamp, University of Illinois Content o The Experimental Effort o Quark and Sea Quark Helicity è DIS, SIDIS, pp è new FFs for global analysis è results
Physics Prospects with the JLab 12 GeV Upgrade
Physics Prospects with the JLab 12 GeV Upgrade Gluonic Excitations 3-dim view of the Nucleon Valence Structure of the Nucleon Elton S. Smith Jefferson Lab PANIC02 Osaka 1 CEBAF @ JLab Today Main physics
CHAPTER 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
Measuring Form Factors and Structure Functions With CLAS
Measuring Form Factors and Structure Functions With CLAS Jerry Gilfoyle for the CLAS Collaboration Physics Department, University of Richmond, Virginia Outline: 1. Jefferson Lab and the CLAS Detector..
Results on the proton structure from HERA
Results on the proton structure from HERA Shima Shimizu (Univ. of Tokyo) Introduction HERA physics Proton structure The world only e-p collider: HERA electron proton A unique collider at DESY, Hamburg
erhic: 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.
Probing 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
Quark-Hadron Duality in Structure Functions
Approaches to QCD, Oberwoelz, Austria September 10, 2008 Quark-Hadron Duality in Structure Functions Wally Melnitchouk Outline Bloom-Gilman duality Duality in QCD OPE & higher twists Resonances & local
Ulrich Mosel TexPoint fonts used in EMF. Read the TexPoint manual before you delete this box.: AAAAAAA
Ulrich Mosel General Motivation: Interactions n Pions (from resonances and DIS) are the most dominant background to QE GiBUU : Theory and Event Simulation based on a BM solution of Kadanoff-Baym equations
Nuclear Parton Distribution Functions
Nuclear Parton Distribution Functions Lessons Learned from Global Fitting J.F. Owens Physics Department, Florida State University DNP Long Range Plan QCD Town Meeting Rutgers University January 12, 2007
Jet Evolution in Hot and Cold Matter
Jet Evolution in Hot and Cold Matter Hans J. Pirner (September 2010, Heidelberg) with S. Domdey, B. Kopeliovich, K. Zapp, J. Stachel, G. Ingelman. J. Rathsman, A. Accardi, D. Gruenewald, V. Muccifora Outline
Nucleon Spin. Tyler Corbett
Nucleon Spin Tyler Corbett Abstract: In 1988 the European Muon Collaboration showed that the quark contribution to spin only accounts for 20-30 percent of the nucleon spin; The "naive quark parton model
Coherent Neutrino Nucleus Scattering
1 Coherent Neutrino Nucleus Scattering E.A. Paschos a and A. Kartavtsev b (presented by E.A. Paschos) a Universität Dortmund, D 441 Dortmund, Germany b Rostov State University, Rostov on Don, Russia We
Flavor Asymmetry of the Nucleon Sea and W-Boson Production*
Flavor Asymmetry of the Nucleon Sea and W-Boson Production* Department of Physics University of Illinois 7 December 2012 *R. Yang, J.C. Peng, M. Grosse-Perdekamp, Phys. Lett. B 680 (2009) 231-234 What
Extraction of Quark Distributions on Transverse Spin of the Nucleon at the HERMES Experiment. Hidekazu Tanaka
Extraction of Quark Distributions on Transverse Spin of the Nucleon at the HERMES Experiment A Dissertation By Hidekazu Tanaka February 25 Department of Physics Tokyo Institute of Technology Abstract
Opportunities 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
Hadron Formation Lengths: QCD Confinement in Forming Systems
Hadron Formation Lengths: QCD Confinement in Forming Systems Will Brooks Jefferson Lab Workshop on Intersections of Nuclear Physics with Neutrinos and Electrons May 5, 2006 Main Focus Space-time characteristics
Lepton and gamma nuclear reactions. J.P. Wellisch, CERN/EP, Geant4 Users Workshop, SLAC, Feb 2002
Lepton and gamma nuclear reactions J.P. Wellisch, CERN/EP, Geant4 Users Workshop, SLAC, Feb 00 Outline Partices treated Cross-section calculations The modeling Classes exposed to users Restrictions of
HERMES status and future running
HERMES status and future running Benedikt Zihlmann University of Gent on behalf of the collaboration DESY PRC Mai 24 p.1/18 Access to Transversity Single spin azimuthal asymmetries on a transverse polarized
Drell-Yan experiments at Fermilab/RHIC/J-PARC. QCD Frontier 2013 Jefferson Lab October 21, 2013 Yuji Goto (RIKEN)
Drell-Yan experiments at Fermilab/RHIC/J-PARC QCD Frontier 2013 Jefferson Lab October 21, 2013 Yuji Goto (RIKEN) Outline Fermilab Drell-Yan experiments Unpolarized program Flavor asymmetry of sea-quark
Strong Interactions and QCD
Strong Interactions and QCD Sourendu Gupta DTP: TIFR DIM 2009 TIFR, Mumbai November 4, 2009 SG (DTP: TIFR) Strong Interactions DIM 09 1 / 14 The experimental context of strong interactions 1 Thomson and
Vector meson photoproduction in ultra-peripheral p-pb collisions measured using the ALICE detector
Vector meson photoproduction in ultra-peripheral p-pb collisions measured using the ALICE detector Jaroslav Adam On behalf of the ALICE Collaboration Faculty of Nuclear Sciences and Physical Engineering
Coherent 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
Nucleon Spin Structure: Overview
Nucleon Spin Structure: Overview Jen-Chieh Peng University of Illinois at Urbana-Champaign Workshop on Spin Structure of Nucleons and Nuclei from Low to High Energy Scales EINN2015, Paphos, Cyprus, Nov.
Introduction to Quantum Chromodynamics (QCD)
Introduction to Quantum Chromodynamics (QCD) Jianwei Qiu Theory Center, Jefferson Lab May 29 June 15, 2018 Lecture One The plan for my four lectures q The Goal: To understand the strong interaction dynamics
Experimental investigation of the nucleon transverse structure
Electron-Nucleus Scattering XIII Experimental investigation of the nucleon transverse structure Silvia Pisano Laboratori Nazionali di Frascati INFN. The unsolved proton How do the lagrangian degrees of
The strange asymmetry of the proton sea
The strange asymmetry of the proton sea J. Magnin CBPF Brazilian Center for Research in Physics XII Mexican Workshop on Particles and Fields Mazatlán, Mexico Outline Introduction The structure of the proton
The measurement of non-photonic electrons in STAR
The measurement of non-photonic electrons in STAR Czech Technical University in Prague, Faculty of Nuclear Sciences and Physical Engineering, Břehová 7, 11519, Prague 1, Czech Republic E-mail: olga.hajkova@fjfi.cvut.cz
Hadron Mass Effects on Kaon Multiplicities: HERMES vs. COMPASS
Hadron Mass Effects on Kaon Multiplicities: HERMES vs. COMPASS Juan Guerrero Hampton University & Jefferson Lab QCD evolution 2017 May 26, 2017 Based on: J. G., J. Ethier, A. Accardi, S. Casper,W. Melnitchouk,
Summary talk. Paul Hoyer University of Helsinki. First Workshop on Quark-Hadron Duality and the Transition to pqcd
Summary talk 1 Paul Hoyer University of Helsinki First Workshop on Quark-Hadron Duality and the Transition to pqcd Laboratori Nazionali di Frascati June 6-8 2005 Amor Sacro e Amor Profano Quark and Hadron
Physic 492 Lecture 16
Physic 492 Lecture 16 Main points of last lecture: Angular momentum dependence. Structure dependence. Nuclear reactions Q-values Kinematics for two body reactions. Main points of today s lecture: Measured
Structure Functions at Very High Q 2 From HERA
Structure Functions at Very High Q 2 From HERA Christopher M. Cormack For the H1 and ZEUS Collaborations Rutherford Appleton Laboratory, Chilton, Didcot, Oxford, OX11 0QX, United Kingdom Abstract. Measurements