The JLAB 3D program at 12
GeV (TMDs+GPDs)
Silvia Pisano Laboratori Nazionali di Frascati
INFN
Transversity 2014 β Jun. 9th - 13th 2014.
4th International Workshop on Transverse Polarisation Phenomena in Hard Processes (Transversity 2014)
GPDs&TMDs: 3D reductions of the Wigner functions
Transversity 2014 β Jun. 9th - 13th 2014.
ππ π, π = ππβ
2π 2ππ π, π
Wigner Functions: quantum phase-space quark distributions in the nucleon
integrated over spatial coordinates: Tranverse Momentum Distributions
β accessed through Semi-Inclusive Deep Inelastic Scattering
integrated over momentum space: Generalized Parton Distributions
β measured through exclusive reactions
TMDs: 3D imaging in the momentum space GPDs: 3D imaging in the coordinate space
The 12-GeV upgrade
4 experimental halls with a longitudinally-polarized electron beam of πΈπβ up to 12 GeV.
Transversity 2014 β Jun. 9th - 13th 2014.
Upgraded halls@12 GeV
High Resolution Spectrometer (HRS) pair and specialized large installation experiments
Super High Momentum Spectrometer (SHMS) at high luminosity and forward angles CLAS12: large acceptance, high luminosity
Transversity 2014 β Jun. 9th - 13th 2014.
Hall-A Hall-A - SoLID
Hall-C Hall-B
Deeply-Virtual Compton Scattering & GPD knowledge
Transversity 2014 β Jun. 9th - 13th 2014.
DVCS data in the valence region
Hall-A: unpolarized and beam-polarized cross-section
Hall-B: beam-spin asymmetries, longitudinally-polarized target spin-asymmetries
HERMES: beam-charge, beam-spin and target-spin asymmetries
All included in CFFs extractions β π―π°ππͺππ constrained at the level of 15%
Wanted: 1. more observables 2. more precise data 3. larger phase-space coverage
COMPASS: DVCS program (2016) β 160 GeV muon beam (recoil detector for full exclusivity): π₯π΅ = 0.01 Γ· 0.1 region explored
JLAB12: Hall-A, B, C β high-statistics in a wide kinematics
12-GeV DVCS program
Transversity 2014 β Jun. 9th - 13th 2014.
nucleon polarization
Sensitivity to GPDs
unpolarized
longitudinally-polarized
transversely-polarized
π―,π― , π¬
π― ,π―, π¬
π¬,π―
E12-06-114: Hall-A, p E12-06-119: Hall-B, p E12-11-003: Hall-B, n E12-13-010: Hall-C, p PR12-06-108: Hall-B, p (DVMP - π0, Ξ·)
E12-06-119: Hall-B, p (ππ»3)
LOI12-11-105: Hall-B, p (π»π·)
Good mapping in the π₯π΅, π2, βπ‘ bins β big impact in constraining πΆπΉπΉπ
Deeply-Virtual Compton Scattering@12-GeV JLab
Transversity 2014 β Jun. 9th - 13th 2014.
π = |π΅π»|2 + πΌ π΅π» β π·ππΆπ + |π·ππΆπ|2
π° π©π― β π«π½πͺπΊ gives rise to spin asymmetries, which can be connected to combinations of GPDs
Two processes contribute to the same (π, π, πΎ) final state: Bethe-Heitler and Deeply-Virtual Compton Scattering.
Hall-A@12 GeV: E12-06-114
Beam-polarized and unpolarized cross sections with high precision at three electron-beam energies to get:
increased kinematic coverage Test of scaling β π2
dependence of ππ at fixed π₯π΅
Transversity 2014 β Jun. 9th - 13th 2014.
βππΏπβ sinπ πΌπ πΉ1π+ ΞΎ πΉ1 + πΉ2 π + ππΉ2π ππ
Large πΈπ region explored with high statistics
Hall-B@12 GeV: High-statistics BSA - E12-06-119
Transversity 2014 β Jun. 9th - 13th 2014.
βππΏπβ sinπ πΌπ πΉ1π+ ΞΎ πΉ1 + πΉ2 π + ππΉ2π ππ
Longitudinal Target-Spin Asymmetry: E12-06-119
Transversity 2014 β Jun. 9th - 13th 2014.
Dynamically-polarized π΅π―π target
βπππΏβ sinπ πΌπ πΉ1π + ΞΎ πΉ1 + πΉ2 π+ ππΉ2π ππ
Quark orbital angular momentum & GPD π¬
Transversity 2014 β Jun. 9th - 13th 2014.
To access πΈπ’&πΈπ both πΈπ&πΈπ are needed.
Proton GPD π¬π: cos π modulation in πππ on proton
Neutron GPD π¬π: π΄πΏπon the neutron
π―,π¬ π π, π, π =πππ π π―, π¬ π π, π, π β π―, π¬ π π, π, π
π―, π¬ π (π, π, π) =πππ π π―, π¬ π π, π, π β π―, π¬ π π, π, π
E12-12-010 π¨πΌπ» on proton
E12-11-003 π¨π³πΌ on neutron
Semi-Inclusive DIS@JLab with 12 GeV
Transversity 2014 β Jun. 9th - 13th 2014.
N/q U L T
U ππ β1β΄
L π π β1πΏβ΄
T π1πβ΄ π1π π‘π, β1π
β΄
Three halls involved ALL Beam/Target
combinations explored Different targets for FLAVOR
SEPARATION multi-D mapping
proton (π―π, π΅π―π, π―π«) deuterium (π«π, π΅π«π) helium ( π―ππ )
E12-06-112: π +, π β, π π E12-09-008: π+, πβ, ππ E12-09-017: π +, π β, π+, πβ C12-11-102: π π
E12-09-08: π +, π β, π π, π+, πβ, ππ E12-09-017: π +, π β, π+, πβ C12-11-102: π π
E12-06-112: π +, π β, π π E12-09-008:π+, πβ, ππ
E07-107: π +, π β, π π E09-009: π+, πβ, ππ
E12-07-007: π +, π β
C12-11-108 (SoLID) PR12-11-111: π +, π β, π π, π+, πβ, ππ PR12-12-009: di-hadron SIDIS
E10-006: π +, π β(SoLID) E12-09-018: π +, π β, π+, πβ(SBS)
Collins@JLab12: Hall-A (neutron) & Hall-B (proton)
Transversity 2014 β Jun. 9th - 13th 2014.
Sivers@JLab12: Hall-A (neutron) & Hall-B (proton)
Transversity 2014 β Jun. 9th - 13th 2014.
π¨πΌπΌ: spin-orbit corr. for pions@Hall-B β E12-06-112
Transversity 2014 β Jun. 9th - 13th 2014.
Tranversely-polarized quark in an unpolarized proton βcos 2πβ modulation Wide π₯&ππ range to map quark 3D momentum phase space
N/q U L T
U ππ β1β΄
L π π β1πΏβ΄
T π1πβ΄ π1π π‘π, β1π
β΄
Transversity 2014 β Jun. 9th - 13th 2014.
Spin-orbit correlations for kaons@Hall-B β E12-09-008
N/q
U L T
U ππ β1β΄
L π π β1πΏβ΄
T π1πβ΄ π1π π‘π, β1π
β΄
Boer-Mulders asymmetry in kaon SIDIS β Collins fragmentation function for kaons β KAON PUZZLE
Transversity through di-hadron β Hall-B&Hall-A (SoLID)
Access through single-hadron
SIDIS: β1π π»1
π β1π π₯, π, π
2 Access through di-hadron SIDIS: π΄ππ β β1π β π»1
β’π β1π π₯, π2
β Complementary measurements on p and n in Hall-A (by SoLID) & Hall-B (C12-12-009)
Transversity 2014 β Jun. 9th - 13th 2014.
πΉπΉ
π
π πβ
π
πβ2
ππ·πΉ
πβ1
Impact of JLab data on the valence region
Transversity 2014 β Jun. 9th - 13th 2014.
Higher-twist PDF: E12-06-112B
Transversity 2014 β Jun. 9th - 13th 2014.
Proposal just submitted to PAC42 β di-hadron SIDIS π΄πΏπ&Multiplicities on hydrogen and deuterium (56 days @ π = 1035ππβ2π β1) β access to the higher-twist PDF π(π₯) Also unpolarized multiplicities will be extracted in 10x10x10x5 π₯π΅, π§,ππ+πβ , π
2 bins
cfr. Marco Radiciβs talk
Summary&Conclusions
Transversity 2014 β Jun. 9th - 13th 2014.
o JLab@12 GeV will perform high-precision measurements in the valence region for both TMDs&GPDs.
o By analyzing all the target/beam polarization combinations on both neutron and proton target, and thanks to a good hadron identification, a huge amount of asymmetries will be extracted and the flavour separation wil be performed
o Many modulations will be extracted in more than one experimental hall, equipped with complementary performing detectors
o Important impact on a wide physics case β spin-orbit correlations, strange quark content in the nucleon, fragmentation, GPDs in the valence region
o JLab 12-GeV operations will start in few months!
Physics Program@Hall-B in the 12-GeV era
Transversity 2014 β Jun. 9th - 13th 2014.
π¨πΌπ³&π¨π³π³for pions on proton@Hall-B β E12-07-107
Transversity 2014 β Jun. 9th - 13th 2014.
N/q U L T
U ππ β1β΄
L π π β1πΏβ΄
T π1πβ΄ π1π π‘π, β1π
β΄
Longitudinal Target-Spin Asymmetry: Kotzinian-Mulder function β tranversely-polarized quark in a longitudinally-polarized proton
Longitudinal Double-Spin Asymmetry: difference in the ππ» distribution of quark with spin || or anti-|| to the proton spin
Transversity 2014 β Jun. 9th - 13th 2014.
π¨πΌπ³&π¨π³π³for pions on π―ππ @Hall-A (SoLID) β E12-11-007
Measurement on NEUTRON β Can be combined with the Hall-B measurement on proton Measurement on longitudinally and
transversely polarized π»π3 target. Combining the π΄πΏπΏ on neutron β constrain the flavour decomposition of the quark helicity distribution 4D binning in π₯, π§, πβ₯, π
2
N/q U L T
U ππ β1β΄
L π π β1πΏβ΄
T π1πβ΄ π1π π‘π, β1π
β΄
π¨πΌπ³ for kaons@Hall-B - E12-09-009
Transversity 2014 β Jun. 9th - 13th 2014.
test of the fragmentation mechanism in the presence of a π -quark
distribution of the sea quarks on the nucleon
Collins fragmentations of kaons
85 days of beam time ππ‘πππππ‘ = 85% (ππ»3),
40%(ππ·3) π = 1035ππβ2π β1
Semi-Inclusive DIS and Tranverse Momentum PDFs
Transversity 2014 β Jun. 9th - 13th 2014.
During the 6-GeV era JLab provided a large amount of data on the unpolarized and longitudinally-polarized modulations. β at 12 GeV the use of a polarized target will open the access to the transversely-polarized sector.
o Tranversity π΄ππsin(π+ππ)β β1π»1
β₯
o Sivers function π΄ππsin(πβππ)β f1TD1
o Pretzelosity π΄ππsin(3πβππ)β β1Tπ»1
β₯
o Worm-gear π΄πΏππππ (πβππ)β π1TD1
CLAS12 phase-space coverage
N/q U L T
U ππ β1β΄
L π π β1πΏβ΄
T π1πβ΄ π1π π‘π, β1π
β΄
Observables accessible through 2h Single-Spin Asymmetries
A longitudinally polarized beam scattering off an unpolarized/longitudinally-polarized target will allow to access the higher-twist PDF π x and βπΏ(π₯) that appears coupled to the Interference Fragmentation
Function π»1β’π
. π΄πΏπ & π΄ππΏ are indeed proportional to the Structure Functions
ππ+
ππβ
π π
π
πβ²
Parton Distribution
Function
Fragmentation Function
π»1β’π extraction ((PRD 85, 114023 (2012)) from Belle π+πβ data (A.Vossen et al.,
PRL107, 072004 (2011))
π―πβ’π
/π«ππ
π x and βπΏ π₯ will provide:
1. insights into the physics of the quarkβgluon correlations 2. π π , ππ³(π) xβintegral β related to the marginally known
scalar(/tensor)βcharge of the nucleon
Transversity 2014 β Jun. 9th - 13th 2014.
Beam-Spin Asymmetries on π―π
Unpolarized π―π target
Longitudinally-polarized π΅π―π target
β Significantly non-zero asymmetries β Good agreement among the two datasets β no alteration from nuclear
background on π¨π³πΌsin ππ
The two analyses performed on CLAS on π»2 and ππ»3 show consistent results. The Beam-Spin Asymmetries extracted through these data sets have been binned in π₯π΅, π§, ππ+πβ .
βππΏπβ [π π₯ π»1β’π+ π π₯ πΊ 1
β’π] π ππ ππ
Transversity 2014 β Jun. 9th - 13th 2014.
Target-Spin Asymmetry on π΅π―π
βπππΏβ [βπΏ π₯ π»1β’π+ π1 π₯ πΊ 1
β’π] π ππ ππ
β Significantly non-zero asymmetries β further modulations under investigation
Transversity 2014 β Jun. 9th - 13th 2014.
Other di-hadron observables
Unpolarized terms β π1(π₯)π·1(π§, πππ ππ , πβ) (leading-twist) and π· 1(π§, πππ ππ , πβ) (higher-twist) 1. π1(π₯) is well-known
2. good description of detector acceptance and
efficiences is needed
π΄πΏπΏ numerator (cross-section differences) β π1(π₯)π·1(π§, cos ππ , πβ) 1. π1(π₯) is well-known
2. good description of detector acceptance and
efficiences is needed
Transversity 2014 β Jun. 9th - 13th 2014.
Hall-C@12 GeV: E12-13-010
1. Energy separation of the DVCS cross section
2. Low-π₯π΅ extension thanks to sweeping magnet
Shaded area β resonance region π > 2 πΊππ
Physical region accessible with a max beam energy πΈππππ = 11 πΊππ
Transversity 2014 β Jun. 9th - 13th 2014.
JLab12 impact on π°π β &πΉπ(β)
Transversity 2014 β Jun. 9th - 13th 2014.
M. Guidal, H. Moutarde, M. Vanderhaeghen: hep-ph > arXiv:1303.6600
Hall-B@12 GeV: π¨πΌπ» on a polarized proton β PR12-12-010
Transversity 2014 β Jun. 9th - 13th 2014.
π΄ππ provides access to the GPD π β sensible to the π-quark contribution to the proton spin
βπππ β πΌπ(π»π, πΈπ) βππΏπ β πΌπ(π»π, πΈπ)
100 days of beam time ππ‘πππππ‘(π»π·) = 60%, π = 1033ππβ2π β1
1 < π2 < 10 πΊππ2, 0.06 < π₯π΅ < 0.66, βπ‘πππ < π‘ < 1.5 πΊππ2
Hall-B@12 GeV: DVCS on the neutron β PR12-11-003
π―,π¬ π π, π, π =πππ π π―,π¬ π π, π, π β π―, π¬ π π, π, π
π―,π¬ π (π, π, π) =πππ π π―,π¬ π π, π, π β π―, π¬ π π, π, π
π¨ππ³πΌ is the most sensitive observables to the GPD E
π¨π³πΌ
80 days of beam time πππππ = 85%, π = 1035ππβ2π β1
β Flavor separation of GPDs
Transversity 2014 β Jun. 9th - 13th 2014.
Impact on quark total OAM
Deeply-Virtual π π, Ξ· Production β PR12-06-108
Transversity 2014 β Jun. 9th - 13th 2014.
1. explore the transition from hadronic to partonic regime
2. chiral-odd GPDs in the proton
Collins&Sivers on p@Hall-B β 80 days@π = ππππππβππβπ
Indiana-Illinois Workshop on FF 2013 β Dec. 13th, 2013.
Sivers@CLAS12 Collins@CLAS12
Collins&Sivers on n@Hall-A β C12-09-018
Indiana-Illinois Workshop on FF 2013 β Dec. 13th, 2013.
Both pions and kaons considered High-luminosity polarized π―ππ target SuperBiBite Spectrometerβ hadron arm BiBite β electron arm Two beam-energies used β evaluation of πΈπ dependence
80 days@π = ππππππβππβπ
SoLID
Transversity 2014 β Jun. 9th - 13th 2014.
1. Scattering electron identified both in the forward and in the large angle part Large-& Forward-angle
electromagnetic calorimeter
2. SIDIS hadrons will be detected in the forward part β 8Γ·15Β° through
Cherenkov counters
MRPC for Time-Of-Flight
Forward-Angle EC
GEM for tracking
Hall-A setup: SBS (hadrons) & BB (electron)
Transversity 2014 β Jun. 9th - 13th 2014.
π»π3 β 60-cm long target Projected luminosity: 2π₯1037πππππ‘πππ β ππ’πππππ ππβ2π β1 (2π₯1036πππππ‘πππ β πππππππ§ππ πππ’π‘πππ ππβ2π β1)
BigBite
Transversity 2014 β Jun. 9th - 13th 2014.
1. tracker 2. gas Cherenkov
counter 3. two-layer
electromagnetic calorimeter
4. scintillator hodoscope