Nov. 25-26, 2010 Annual Meeting of GDR Nucleon - K. Park.

Slides:



Advertisements
Similar presentations
Target Fragmentation studies at JLab M.Osipenko in collaboration with L. Trentadue and F. Ceccopieri, May 20,SIR2005, JLab, Newport News, VA CLAS Collaboration.
Advertisements

Workshop on N* excitations at high Q 2 with CLAS12 Page 1 Workshop on N* Excitations at High Q 2 Welcome to Participants in the Workshop on Nucleon Resonance.
 0, ,  + exclusive electroproduction on the proton at CLAS on the proton at CLAS.
M. Ripani INFN Genova Introduction. In less than three years from now, the Jefferson Lab upgrade will be completed, allowing to deliver energies up to.
 photoproduction with linearly polarized photons at SPring-8 SENDAI03 16 th June, 2003 Tsutomu Mibe (Research Center for Nuclear Physics, Osaka univ.,
1 Single  0 Electroproduction in the Resonance Region with CLAS Kyungseon Joo University of Connecticut For the CLAS Collaboration N* 2009 Beijing, China.
Electromagnetic Studies of Pseudoscalar Mesons Dan Dale Idaho State University For the PrimEx Collaboration.
Recent GRAAL Results on Nucleon Spectroscopy at MeV N.V.Rudnev*, A.Lapik, V.G.Nedorezov, A.A.Turinge for \ the GRAAL Collaboration Institute.
Recent Highlights of Physics on the Nucleon with CLAS Volker D. Burkert Jefferson Lab NSTAR 2007 September 5, 2007, Bonn, Germany.
Brahim MorenoStudents' seminar at Bosen Workshop ΔVCS and Generalized Parton Distributions
1 Exclusive electroproduction of the    on the proton at CLAS  Outline: Physics motivations: GPDs CLAS experiment: e1-dvcs Data analysis:   cross.
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.
Study of two pion channel from photoproduction on the deuteron Lewis Graham Proposal Phys 745 Class May 6, 2009.
NUINT11, Dehradun, India March 7-11, 2011 S. Manly, University of Rochester1 eA pion production at CLAS aimed at neutrinos S. Manly & Hyupwoo Lee University.
“Look at the field. They are ripe for harvest.” “ Do you not say, 'Four months more and then the harvest'? I tell you, open your eyes and look at the.
Backward meson production at CLAS Alex Kubarovsky (RPI/Uconn) Kyungseon Joo (Uconn) Valery Kubarovsky (Jlab) Paul Stoler (RPI) Exclusive Meson Production.
T.C. Jude D.I. Glazier, D.P. Watts The University of Edinburgh Strangeness Photoproduction: Polarisation Transfer & Cross-Section Measurements.
Polarisation transfer in hyperon photoproduction near threshold Tom Jude D I Glazier, D P Watts The University of Edinburgh.
T.C. Jude D.I. Glazier, D.P. Watts The University of Edinburgh Strangeness Photoproduction At Threshold Energies.
Valery Kubarovsky Jefferson Lab. Published papers106 Total number of citations Average citations per published paper 74 Renowned papers (500+) 3.
Hard Exclusive Processes at CLAS and CLAS12 Valery Kubarovsky Jefferson Lab Newport News, VA June 28, 2011 The 5th joint International HADRON STRUCTURE.
Eugene Pasyuk DSPIN-09 Dubna, September 1-5, Eugene Pasyuk DSPIN-09 Dubna, September 1-5,
K +  photoproduction with the Crystal Ball at MAMI T.C. Jude The University of Edinburgh New method of K + detection with the Crystal Ball Extraction.
First Results of Curtis A. Meyer GlueX Spokesperson.
Motivation. Why study ground state hyperon electroproduction? CLAS detector and analysis. Analysis results. Current status and future work. M. Gabrielyan.
Probe resolution (GeV) N π,  Q 2 =12 GeV 2 Q 2 =6 GeV 2 The study of nucleon resonance transitions provides a testing ground for our understanding.
Single pion electroproduction at CLAS Kijun Park Univ. of South Carolina Kijun Park Univ. of South Carolina 1 st Student Conference 702D Aug.
Future Physics at JLab Andrew Puckett LANL medium energy physics internal review 12/14/
A Precision Measurement of the Neutral Pion Lifetime: the PRIMEX Experiment Rory Miskimen University of Massachusetts, Amherst and the PRIMEX Collaboration.
A Precision Measurement of the Neutral Pion Lifetime: New Results from the PRIMEX Experiment Rory Miskimen University of Massachusetts, Amherst for the.
Beijing, Sept 2nd 2004 Rachele Di Salvo Beam asymmetry in meson photoproduction on deuteron targets at GRAAL MENU2004 Meson-Nucleon Physics and the Structure.
E02-013: at high Q 2 Status of Analysis Sergey Abrahamyan Yerevan Physics Institute for the E collaboration TexPoint fonts used in EMF. Read the.
CLAS12 User’s Activities. CLAS12 Steering Committee Appointed by CLAS Users Coording Committee (Dave Tedeschi, Chair) Function: To assist the CCC and.
E02-013: at high Q 2 Status of Analysis Sergey Abrahamyan Yerevan Physics Institute for the E collaboration.
Harut Avakian (Jlab) DVCS results with unpolarized and polarized target Introduction Event selection MC simulations and radiative corrections DVCS with.
Kijun Park Colloquium γ*γ* Feb. 25, College of William and Mary 02/25/2011 K. Park Universe.
K* photoproduction from g11 K. Hicks Ohio University HSG meeting, 12 June 2009.
TMD flavor decomposition at CLAS12 Patrizia Rossi - Laboratori Nazionali di Frascati, INFN  Introduction  Spin-orbit correlations in kaon production.
Probe resolution (GeV) N π,  Q 2 =12 GeV 2 Q 2 =6 GeV 2 The study of nucleon resonance transitions provides a testing ground for our understanding.
Polarisation transfer in hyperon photoproduction near threshold Tom Jude D I Glazier, D P Watts The University of Edinburgh.
Georgie Mbianda 1 for the Baryon (E01-002) Collaboration 1 University of the Witwatersrand, Johannesburg Exclusive Electroproduction of π + and η mesons.
Simultaneous photo-production measurement of the  and  mesons on the nucleons at the range 680 – 1500 MeV N.Rudnev, V.Nedorezov, A.Turinge for the GRAAL.
Spin Asymmetries of the Nucleon Experiment ( E07-003) Proton Form Factor Ratio G E /G M from Double Spin Asymmetry with Polarized Beam and Target Anusha.
Deeply virtual  0 electroproduction measured with CLAS.
15 cm Plots of missing mass spectrum and 90% interval for width of 0.5 and 10 MeV. Color lines show upper limit, lower limit and sensitivity. Search for.
Transition region (1) Transition region (2) Scaling (s-, Q 2,…) (3) Generalized Parton Distribution (4) Transition Distribution Amplitude (5) …
Double spin asymmetry measurement from SANE-HMS data at Jefferson Lab Hoyoung Kang For SANE collaboration Seoul National University DIS /04/23.
Probe resolution (GeV) N π,  Q 2 =12 GeV 2 Q 2 =6 GeV 2 The study of nucleon resonance transitions provides a testing ground for our understanding.
Exclusive Vector Meson Electroproduction at 12 GeV Paul Stoler Rensselaer Polytechnic Institute.
1 Inclusive B → X c l Decays Moments of hadronic mass and lepton energy PR D69,111103, PR D69, Fits to energy dependence of moments based on HQE.
Overview of recent photon beam runs at CLAS CLAS12 European Workshop, Feb , Genoa, Italy Ken Livingston, University of Glasgow Tagged photons.
1 Kinematics Plots Single event : electron, positive charged pion Under Condition : W ≥ 2GeV, Reaction : ep→e’π + ( X ) Scaling Update Report Apr.09,’07.
Envisioned PbWO4 detector Wide-Angle Compton Scattering at JLab-12 GeV with a neutral-particle detector With much input from B. Wojtsekhowski and P. Kroll.
1 FAIR SIMULATION ACTIVITIES AND PHENOMENOLOGICAL STUDIES AT IPN ORSAY PANDA Collaboration Meeting, GSI, Sep. 5, 2011 Béatrice Ramstein for the.
Spin Asymmetries of the Nucleon Experiment ( E07-003) Anusha Liyanage Advisor : Dr. Michael Kohl  Introduction  Physics Motivation  Detector Setup &
Status Report of Single Pion Electroproduction in the Deep Inelastic Scattering Region Kijun Park Univ. of South Carolina Kijun Park Univ. of South Carolina.
Top 3 European countries? 1.England/Britain 2.France 3.Spain.
Kijun Park Univ. of South Carolina Kijun Park Univ. of South Carolina Axial Form Factor Physics at CLAS May. 30, 2008 HSWG meeting Electroproduction of.
Kijun Park Univ. of South Carolina Kijun Park Univ. of South Carolina Aug. 30, 2008 Hadron Spectroscopy Physics Working Group Meeting Electroproduction.
Proton Form Factor Ratio GE/GM from Double Spin Asymmetry with
EM channels with reduced luminosity and aceptance: preliminary results
into three pions Opportunities in p pbar annihilation S. Ong IPN Orsay
Recent GRAAL Results on Nucleon Spectroscopy at MeV
Pion Photoproduction from the Nucleon and Scaling
Exclusive electroproduction of the r+ on the proton at CLAS
October 12, Tallahassee, FL
Selected Physics Topics at the Electron-Ion-Collider
Experiment (Jlab Exp : CLAS eg3)
Update of RG-A Hadron Structure Analyses
GEp-2γ experiment (E04-019) UPDATE
Presentation transcript:

Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

Pert. hard part soft part Successful Q2  ∞, t << fixed Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

Pert. hard part soft part What about u <<, DVCS ? Non-pert. Part does not describe the Hadron  Hadron transition Need a Transition DA (TDAs) ??? Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

Non-pertubative transition between pion and baryon in backward angle Investigation of Transition Distribution Amplitude B. Pire, L. Szymanowski PRD71, (2005) Pert. Amplitude = Correlation between meson →  transition Mesonic TDA pp     GSI e+e- B-factories       Large Q2 would provide hard scale with pert. expansion pp  J/  GSI pp     t GSI Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

Non-pertubative transition between pion and baryon in backward angle Investigation of Transition Distribution Amplitude B. Pire, L. Szymanowski PRD71, (2005) Pert. Amplitude = Correlation between meson →  transition Mesonic TDA pp     GSI e+e- B-factories       Large Q2 would provide hard scale with pert. expansion pp  J/  GSI pp     t GSI Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

Non-pertubative transition between pion and baryon in backward angle Investigation of Transition Distribution Amplitude J.P. Lansberg, B. Pire, PRD75, (2007) GPD can not describe Non-perturbative part Baryon → π transition Pert. Amplitude = Meson almost stay at rest in the target(baryon) rest frame Pert. Baryonic TDA e’   n u CLAS   at 180 Hall-C e’p  e’p  CLAS JLAB 12GeV  *p  pJ/ COMPASS Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

The kinematics imposes the exchange of 3 quarks in the u -channel Factorization in the generalized Bjorken limit: The object factorized from the hard part is a Transition Distribution Amplitude Interpretation at the amplitude Amplitude of probability to find a meson within the proton Baryonic TDA Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

Kinematical variables Unpol. CRS w/ one-photon exchange approx. Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

The CLAS Collaboration Old Dominion University, Norfolk, VA Rensselaer Polytechnic Institute, Troy, NY Rice University, Houston, TX University of Richmond, Richmond, VA University of Rome Tor Vergata, Italy University of South Carolina, Columbia, SC Thomas Jefferson National Accelerator Facility, Newport News, VA Union College, Schenectady, NY Virginia Polytechnic Institute, Blacksburg, VA University of Virginia, Charlottesville, VA College of William and Mary, Williamsburg, VA Yerevan Institute of Physics, Yerevan, Armenia Brazil, Germany, Morocco and Ukraine,, have individuals or groups involved with CLAS, but with no formal collaboration at this stage. Arizona State University, Tempe, AZ University Bari, Bari, Italy University of California, Los Angeles, CA California State University, Dominguez Hills, CA Carnegie Mellon University, Pittsburgh, PA Catholic University of America CEA-Saclay, Gif-sur-Yvette, France Christopher Newport University, Newport News, VA University of Connecticut, Storrs, CT Edinburgh University, Edinburgh, UK University Ferrara, Ferrara, Italy Florida International University, Miami, FL Florida State University, Tallahassee, FL George Washington University, Washington, DC University of Glasgow, Glasgow, UK University of Grenoble, Grenoble, France Idaho State University, Pocatello, Idaho INFN, Laboratori Nazionali di Frascati, Frascati, Italy INFN, Sezione di Genova, Genova, Italy Institut de Physique Nucléaire, Orsay, France ITEP, Moscow, Russia James Madison University, Harrisonburg, VA Kyungpook University, Daegu, South Korea University of Massachusetts, Amherst, MA Moscow State University, Moscow, Russia University of New Hampshire, Durham, NH Norfolk State University, Norfolk, VA Ohio University, Athens, OH Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

CLAS E max 6 GeV I max 200  A Duty Factor 100%  E /E Beam P ~ 85% E g (tagged) ~ GeV

e-e- π+π+ e-e- Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

Kinematical variables Unpol. CRS w/ one-photon exchange approx. Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

Particle Identification Acceptance Calculation Radiative Correction Background Subtraction Kinematical Correction Extract CRS & structure functions Acceptance cross check after more simulation in backward angle with Modification of GENEV vs. FSGEN Bin corrections Systematic error studies E1-6 data set was used.E 0 =5.754GeV, B =3375A, LH2 ……. Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

1.No (s-) resonance access (= no event below 2GeV of W) 2.No missing mass cut Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

1.No (s-) resonance access (= no event below 2GeV of W) 2.No missing mass cut 3.Automatically, accessible small -u large –t u t Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

Requirement W>2GeV Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

Requirement W>2GeV cos  * <0.0  T 2 <0.5GeV 2 Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

Requirement W>2GeV cos  * <0.0  T 2 <0.5GeV 2 TOF mass 3sigma cut Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

Requirement W>2GeV cos  * <0.0  T 2 <0.5GeV 2 TOF mass 3sigma cut  : 2sigma cut Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

Blue bullets :  _T2 < 0.5GeV2 cut Red hist. :  _T2 < 1.0GeV2 cut u t cos  * Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

Black bullets : exp. Data before BG subtraction Red bullets : exp. Data before BG subtraction Blue solid lines : nominal MMx 3  cut Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

Blue bullets : exp. Data after BG subtraction Red hist. : GPP + w/o (left) & with (right) correction applied MC Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

1.Two event generators were tested 2.cos  cut was applied on top of  T 2 cut Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

1.Two event generators were tested 2.cos  cut was applied on top of  T 2 cut Nov. 12, 2010 DPWG K. Park

W>2GeV MMx cut cos  * <0.0  T 2 <0.5GeV 2 Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

W>2GeV  T 2 <1.0GeV 2 + GPP+corr.  T 2 <0.5GeV 2 MMx cut Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

Blue square : data with stat. err. only Red triangle : fit with cos2  Average Chi2 ~ 1.74 except last Q 2 bin Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

σ T +εσ L Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

σ T +εσ L Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

σ T +εσ L Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

σ T +εσ L J.P. Lansberg, B. Pire, PRD75, (2007) But  0 – calculation for  =0.8,  =180 o Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

σ T +εσ L < 1/2 ~1  - range is about Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

Hard exclusive process of meson in the backward angle opens a new window in the understand of hadronic physics in the framework of the collinear-factorization approach of QCD. Measurement of cross sections and asymmetries are crucial to develop a realistic model for the TDAs. Careful study has been performed by communicating with theory group (kinematic binning, corrections, acceptance(GENEV/FSGEN), cuts, etc.) We measured the differential cross sections on backward angle in the kinematic range of W > 2GeV, high “t” and low “u”. We extracted the structure functions from differential cross sections,  TT has a similar amplitude of  LT  T +  L is ~2x larger than  TT and  LT.  Open questions ? Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

Thank you ! Questions/comments ? Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

Black bullets : exp. Data before BG subtraction Red bullets : exp. Data before BG subtraction Blue solid lines : nominal MMx 3sigma cut Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

Black bullets : exp. Data before BG subtraction Red bullets : exp. Data before BG subtraction Blue solid lines : nominal MMx 3sigma cut Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

Black bullets : exp. Data before BG subtraction Red bullets : exp. Data before BG subtraction Blue solid lines : nominal MMx 3sigma cut Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

Black bullets : exp. Data before BG subtraction Red bullets : exp. Data before BG subtraction Blue solid lines : nominal MMx 3sigma cut Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

Black bullets : exp. Data before BG subtraction Red bullets : exp. Data before BG subtraction Blue solid lines : nominal MMx 3sigma cut Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

W>2GeV  T 2 <0.5GeV bins of  MMx cut  T 2 <0.5GeV bins of  Nov , 2010 Annual Meeting of GDR Nucleon - K. Park

W>2GeV  T 2 <0.5GeV 2 MMx : +/- 4  cut MMx : +/- 2  cut Nov , 2010 Annual Meeting of GDR Nucleon - K. Park