SIDIS @ 12 GeV with polarized target
description
Transcript of SIDIS @ 12 GeV with polarized target
Patrizia RossiLaboratori Nazionali di Frascati- INFN (Italy)
Physics motivations
Experimental Requirements
Measurements
Summary
CLAS12 2nd European Workshop - March 7-11, 2011- Paris, France
SIDIS ProgramSIDIS Program with Longitudinally Polarized with Longitudinally Polarized TargetsTargets
E12-07-107 : E12-07-107 : Studies of Spin-orbit Correlations with Longitudinally Polarized TargetSpokespersons: H. Avakian, P. Bosted, K. Griffioen, K. Hafidi, P. Rossi
E12-09-009 : E12-09-009 : Studies of Spin-Orbit Correlations in Kaon Electroproduction in DIS with polarized hydrogen and deuterium targetsSpokespersons: H. Avakian, E. Cisbani, K. Griffioen, K. Hafidi, P. Rossi
E12-09-007 : E12-09-007 : Studies of partonic distributions using semi-inclusive production of kaonsSpokespersons: K. Hafidi, H. Avakian, F. Benmokhtar, A. EL Alaoui, M. Mirazita
TMDs TMDs with Longitudinally Polarized Targets at l.t.with Longitudinally Polarized Targets at l.t.
Factorization of kT-dependent PDFs proven at low PT of hadrons (Ji et al)
Quark polarization
Nucl
eon
pola
riza
tion
-
Correlation between the transverse momentum and transverse spin of quarks in longitudinally polarized nucleon
Kaon distributions in ep e’KXKaon distributions in ep e’KX
Q2>1GeV2
W2>4 GeV2(10)y<0.85MX>2GeV
SIDIS kinematics
High energy kaons are at small angles (<30o)
forward
Flavor DecompositionFlavor Decomposition
BBS/LSS +OAM
BBS/LSS
H.Avakian,S.Brodsky,A.Deur,F.Yuan (2007)
AA11 – P – PTT dependence dependence
M. Anselmino et al PRD74:074015, 2006
+ A1 suggests broader kT distributions for f1 than for g1
- A1 may require non-Gaussian kT-dependence for different helicities and/or flavors
02=0.25GeV2
D2=0.2GeV2
H. Avakian & CLAS Coll., PRL.105:262002, 2010
0.4<z<0.7
AA11 – P – PTT dependence @ 12 GeV dependence @ 12 GeV
A1 PT-dependence provides access to helicity dependence of kT-distributions of quarks
Deuteron and hydrogen data required for PT-dependent flavor decomposition.
proton
Curves: M. Anselmino et al PRD74:074015, 2006
A1
deuteron
A1
Transverse momentum distributions of Transverse momentum distributions of partons partons
NJL model H. Matevosyan et al. arXiv:1011.1052 [hep-ph]
proton
Transverse momentum distributions in hadronization may be flavor dependent => measurements of different final state hadrons is required
Transverse momentum distributions in hadronization may be flavor dependent => measurements of different final state hadrons is required
Kotzinian-Mulders AsymmetryKotzinian-Mulders Asymmetry
B.Musch arXiv:0907.2381B.Pasquini et al, arXiv:0910.1677
Kotzinian-Mulders Asymmetry for and K provides complimentary information on polarization effects in hadronization
CLAS12 has wide coverage in x and PT, which is crucial for this program
Kotzinian-Mulders AsymmetryKotzinian-Mulders Asymmetry
proton deuteron
Partonic SIDIS: Partonic SIDIS: E12-09-007E12-09-007Complete program for the study of the individual quark
contribution to the nucleon spin
Partonic SIDISPartonic SIDIS
Ke
e’
Sea strange quark polarization
Light quark sea polarization asymmetry
-Most sensitivity to K- (us)
Experimental configurationExperimental configuration
RIC
HRIC
H
CLAS12 + RICH
Target: longitudinally polarized NH3 (P=0.85%) & ND3 (P=0.40%) Luminosity= ∼ 1035 cm−2s−1
Ee = 11GeV
Proposal Physics PAC days Parallel Running
E12-07-107 TMDs 103(50 d, 30 p)
E12-06-109
E12-09-009 TMDs K 103(50 d, 30 p)
E12-06-109, E12-07-107
E12-09-007(b) Partonic SIDIS
103 (50 d, 30 p)
E12-06-109, E12-07-107
Polarized targetPolarized targetDesign Parameters:• L = 2 x 1035 N/cm2 e-/s =>
3.3 cm length, 16 nA beam rastered over 3 cm diameter (anneal once every 1-2 days)
• p and d targets (also C, empty)
• Pt=80(40)% p(d) via DNP
• Horizontal 1 K cryostat (0.8 W), 5 T field from CLAS12 CT solenoid, 140 GHz µwave (1/2 W), irradiated NH3/ND3, NMR to measure Pol.)
Recent Progress:• Funding provided through NSF MRI-R2 grant to ODU
(lead), CNU and UVa (4/’10 - 3/’14)• Refrigerator design led by UVa/Jlab• Development of NMR started at ODU (with help from
UVa and JLab); some equipment purchased• Development of µwave system started at CNU
ConclusionsConclusions
Comprehensive program to study transverse momentum dependence of valence quark transverse and longitudinal spin distributions through measurements of spin-azimuthal asymmetries in SIDIS electroproduction of pions and kaons
Main objectives include studies of correlations of the transverse spin of quarks with their transverse momentum, leading to the sin 2φ azimuthal moment.
The PT dependence of the double spin asymmetry will provide additional information on the flavor and polarization dependence of transverse momentum dependence of helicity distributions of quarks, providing complementary to SSA measurements access to spin-orbit correlations.
11 GeV polarized electron beam, longitudinally polarized proton and deuteron targets and the CLAS12 detector equipped with a RICH detector for kaon studies will be used.
Complete program for the study of the individual quark contribution to the nucleon spin
BACKUP SLIDESBACKUP SLIDES