DIS off Pions Bogdan Povh

Slides:



Advertisements
Similar presentations
Max-Planck-Institut für Kernphysik, Heidelberg Two scales of the hadronic structure Search for clean signatures in the data Bogdan Povh.
Advertisements

Target Fragmentation studies at JLab M.Osipenko in collaboration with L. Trentadue and F. Ceccopieri, May 20,SIR2005, JLab, Newport News, VA CLAS Collaboration.
Measurement of F 2 and F L at low Q 2 in ep Interactions at HERA  H1 and ZEUS analyses at low Q 2  Extraction of F L  Summary and Outlook Tomáš Laštovička.
The Hadronic Final State at HERA Rainer Mankel DESY for the ZEUS & H1 collaborations C2CR Conference Prague 9-Sep Sep-2005 (Some Highlights from)
Measurements of F 2 and R=σ L /σ T on Deuterium and Nuclei in the Nucleon Resonance Region Ya Li November 3, 2009 Jlab E02-109/E (Jan05)
Experimental requirements for GPD measurements at JLab energies. Detector that ensures exclusivity of process, measurement of complete final state Measure.
PION STRUCTURE FUNCTION AND MORE. Pion signature in experiment: Forward neutrons in DIS Gottfried Sum rule.
Working Group on e-p Physics A. Bruell, E. Sichtermann, W. Vogelsang, C. Weiss Antje Bruell, JLab EIC meeting, Hampton, May Goals of this parallel.
11 Primakoff Experiments with EIC A. Gasparian NC A&T State University, Greensboro, NC For the PrimEx Collaboration Outline  Physics motivation:  The.
Measurements of F 2 and R=σ L /σ T on Deuteron and Nuclei in the Nucleon Resonance Region Ya Li January 31, 2009 Jlab E02-109/E (Jan05)
Recoil Polarimetry in Meson Photoproduction at MAMI Mark Sikora, Derek Glazier, Dan Watts School of Physics, University of Edinburgh, UK Introduction The.
Shibata lab. Ogoshi Shun P. Amaudruz et al., New Muon Collaboration Phys. Rev. Lett. 66 (1991) 2712 [Contents] 1.Introduction 2.Deep inelastic scattering.
Crossed Channel Compton Scattering Michael Düren and George Serbanut, II. Phys. Institut, - some remarks on cross sections and background processes  
Prague 05-10/07/2004Marialaura Colantoni1 Advance Study Institute SYMMETRY and SPIN Marialaura Colantoni* on behalf of the COMPASS coll. *Universita’ del.
Parton Model & Parton Dynamics Huan Z Huang Department of Physics and Astronomy University of California, Los Angeles Department of Engineering Physics.
Electron Deuteron Scattering with H1 at HERA ■ Introduction ■ Physics with deuterons ■ H1 upgrade for ed running ■ Possible further studies and the necessary.
Particle Physics Chris Parkes Experimental QCD Kinematics Deep Inelastic Scattering Structure Functions Observation of Partons Scaling Violations Jets.
Single-spin asymmetries in two hadron production of polarized deep inelastic scattering at HERMES Tomohiro Kobayashi Tokyo Institute of Technology for.
Measurement of F 2 and R=σ L /σ T in Nuclei at Low Q 2 Phase I Ya Li Hampton University January 18, 2008.
Spin physics at the SMC Spin Muon Collaboration A. Magnon (CEA-Saclay/IRFU & COMPASS)
Jim Stewart DESY Measurement of Quark Polarizations in Transversely and Longitudinally Polarized Nucleons at HERMES for the Hermes collaboration Introduction.
Heuijin LimICHEP04, Beijing, Aug. 1 Leading Baryons at HERA Introduction Diffractive structure function measured in events with a leading proton.
Lattice /Detector Integration for Target Fragmentation, Diffraction, and other Low-t Processes Charles Hyde-Wright Old Dominion University
The Quark Structure of the Nucleon Inti Lehmann & Ralf Kaiser University of Glasgow Cosener’s House Meeting 23/05/2007 Nucleon Structure Generalised Parton.
Measurements with Polarized Hadrons T.-A. Shibata Tokyo Institute of Technology Aug 15, 2003 Lepton-Photon 2003.
Measuring the Spin Structure of 3 He and the Neutron at Low Q 2 Timothy Holmstrom College of William and Mary For the Jefferson Lab Hall A Collaboration.
Thomas Jefferson National Accelerator Facility PAC-25, January 17, 2004, 1 Baldin Sum Rule Hall C: E Q 2 -evolution of GDH integral Hall A: E94-010,
Inclusive Measurements of inelastic electron/positron scattering on unpolarized H and D targets at Lara De Nardo for the HERMES COLLABORATION.
Lara De Nardo DIS 2007 Measurement of the spin structure functions g 1 and g 1 at HERMES Lara De Nardo TRIUMF/DESY pd.
Measurement of Flavor Separated Quark Polarizations at HERMES Polina Kravchenko (DESY) for the collaboration  Motivation of this work  HERMES experiment.
K 0 S and  production at ZEUS, A. Savin, University of Wisconsin DIS 2006, April 22, K 0 S and  production at ZEUS Alexander A. Savin University.
Isabell-A. Melzer-Pellmann DIS 2007 Charm production in diffractive DIS and PHP at ZEUS Charm production in diffractive DIS and PHP at ZEUS Isabell-Alissandra.
Polarised DIS Experiment Gerhard Mallot. G. Mallot/CERN Spin Summer School, BNL, 2004 Plan Lecture I –introduction –kinematics –the cross section –structure.
A. Bertolin on behalf of the H1 and ZEUS collaborations Charm (and beauty) production in DIS at HERA (Sezione di Padova) Outline: HERA, H1 and ZEUS heavy.
JLab, October 31, 2008 WACS in 12 GeV era 1 GPDs Wide-Angle Compton Scattering pi-0 photo-production in 12 GeV era B. Wojtsekhowski Outline WACS and other.
Abstract Deep inelastic scattering (DIS) and diffractive scattering are used to probe the internal structure of hadrons in accelerator physics. During.
1 Exotic States 2005 E.C. Aschenauer The search for Pentaquarks at on behalf of the HERMES Collaboration E.C. Aschenauer DESY.
Measurements of Generalized Parton Distributions with COMPASS at CERN (CERN-SPSC , SPSC-EoI-005) Letter of Intent, in framework of the theme /2008.
Mesons in ep missing spectra G. M. Urciuoli. Meson photoproduction provide a good tool to study nucleon resonances. For example, a large number of resonances.
Timelike Compton Scattering at JLab
F2bb from muon+jet final states at ZEUS
Lecture 18 - Detectors Detector systems
COMPASS results on inclusive and semi–inclusive polarised DIS
Multilepton production at HERA
Explore the new QCD frontier: strong color fields in nuclei
Small-x Physics and Diffraction: HERA Results
PHYS 3446 – Lecture #14 Energy Deposition in Media Particle Detection
HERA p e± 920 GeV 27.6 GeV √s = 319 GeV ep Collider
Luciano Pappalardo for the collaboration
Deeply Virtual Compton Scattering at HERMES
Wide Angle Compton Scattering
Future physics at nuSTORM
F2/FL with HERA III/eRHIC A. Caldwell, Max-Planck-Institut f. Physik
Particle Physics WS 2012/13 ( )
Study of Strange Quark in the Nucleon with Neutrino Scattering
B2B hadron production in SIDIS
PHENIX Transverse-Spin Physics
Measurement of the spin structure functions g1 and g1 at HERMES
K0S and L production at ZEUS
B. Povh, MPIK Heidelberg Th. Walcher, Uni Mainz
PIONS in DIS Bogdan Povh Max-Planck-Institut fuer Kernphysik.
Diffraction at HERA Alice Valkárová Charles University, Prague
Searches and EW physics at HERA
MAID and the GDH sum rule in the resonance region
Overview on hard exclusive production at HERMES
Helicity dependence of g n ® Nπ(π) and the GDH integral on the neutrom
XIII LNF Spring school, May 2008, Frascati.
Measurement of the spin structure functions g1 and g1 at HERMES
PHYS 3446 – Lecture #14 Energy Deposition in Media Particle Detection
Search for X - - Pentaquark in COMPASS
Presentation transcript:

DIS off Pions Bogdan Povh Max-Planck-Institut fuer Kernphysik, Heidelberg

Pion signature in experiment: Gottfried Sum rule Polarized structure function Forward neutrons in DIS

DIS on Proton and Deuteron Gottfried sum rule Spin structure function

Pion signature NMC detector at CERN Deep inelastic scattering of muons off protons and deuterons

Pion signature Gottfried sum rule for flavour symmetric sea

Pion signature

Pion signature Toy model

Forward Neutron Calorimeters at H1 and ZEUS at DESY

FNC – design specifications The size and weight of FNC is defined by the space available in HERA tunnel position– 105m from the interaction point, size ~ 70 x 70 x 200cm3 , weight <10t geometrical acceptance is limited by beam-line elements <0.8mrad should work in high radiation environment A.Bunyatyan “Physics with FNC”

Pion signature H1 detector at HERA collider

A.Bunyatyan “Physics with FNC”

The H1-FNC energy response CERN test-beam Ebeam=120-350 GeV A.Bunyatyan “Physics with FNC”

Neutron and photon energy spectrum measured in H1 -cluster in Preshower = photon, -cluster in main calorimeter and/or Preshower = neutron A.Bunyatyan “Physics with FNC”

Different pion fluxes used in analysis (different form factors)

Rapgap-MC after tuning Data Acceptance determined by MC A.Bunyatyan “Physics with FNC”

“Measurement of leading proton and neutron production in DIS at HERA” H1 Publications: “Measurement of leading proton and neutron production in DIS at HERA” DESY-98-169 “Measurement of dijet cross sections in ep interactions with a leading neutron “, DESY-04-247 ZEUS Publications: “Study of the pion trajectory in the photoproduction of leading neutrons at HERA” DESY-04-037 “Photoproduction of D* mesons associated with a leading neutron”” DESY-03-221 “Leading neutron production in ep collisions at HERA” DESY-02-039 “Measurement of dijet cross sections for events with a leading neutron in photoproduction at HERA” DESY 00-142 “Observation of events with an energetic forward neutron in DIS at HERA” DESY 96-093 A.Bunyatyan “Physics with FNC”

F2p from ZEUS

F2LN(3) (z=0.7) Gp Xp Data show sensitivity to the parameterizations of the pion structure function (constrained for x (=b)>0.1 from the fixed target experiments). A.Bunyatyan “Physics with FNC”

e.g. rgp < rjj < rD* ≤ rDIS Comparison of LN production rate for different processes (ZEUS) e.g. rgp < rjj < rD* ≤ rDIS Absorption - ratio depends on the transverse size of virtual photon A.Bunyatyan “Physics with FNC”

Pion signature Estimation of the probability of the p→n+p+ in DIS from the neutron rate in DIS extrapolating to the full energy range (for three different pion fluxes}

SU(2) chiral model

Conclusions

Conclusions

Conclusions The constituent quarks are a superposition of the massive quarks and pions

Conclusions Gluonic structure of the nucleon- resolution on the order of 0.3 fm