Transversely Polarized Proton Spin Measurements in Polarized p+p Collisions in
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![Page 1: Wooyoung Kim Probing Nuclear Spin Structure with Radioactive Ion Beams and Polarized Target May 28, 2010.](https://reader036.fdocuments.us/reader036/viewer/2022070400/56649eff5503460f94c1417a/html5/thumbnails/1.jpg)
Wooyoung KimWooyoung Kim
Probing Nuclear Spin Structure with Radioactive Ion Beams and Polarized Target
May 28, 2010May 28, 2010
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• Electron Scattering-Kinematics, Spin Structure Function
• GPDs & DVCS
• Polarized Targets with RIB:•
•
Overview
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Ground State Charge Density; Saclay
(e,e’)
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Energy Transfer Dependence of Cross-Section: (e,e’)
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Cross sections and Beam Asymmetries
• Over 31,000 Cross-Sections Measured• Over 4,000 Asymmetries Measured
Q2 = 1.7 – 4.5 GeV2
W = 1.15 – 1.7 GeV
PRC 77, 0152081 (2008)K. Park, W. Kim et al.
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Structure Functions
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Structure Functions
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Electroexcitation of the Roper resonance for 1.7<Q2<4.5 GeV2
Transverse Longitudinal
G. Aznauiy, K. Park, W.Kim PRC 78 (2008),
PRC 80 (2009).
Dispersion Relation
Unitary Isobar Model.
Helicity Amplitude for:
Transition:
A first Radial Excitation of
the 3g Ground State
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2* * ( , )
dh
d d
* * *' ' ' 'cos 2sin cosT T TL TL
L L T T
v R v RA
v R v R
Additional Nuclear Structure Information
0( , ' )p e e p
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Symmetric Detector
Super-Rosenbluth Separation
Simultaneous Measurements of T’ and TL’ asymmetries
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• Formalism for the QCD description of deeply exclusive leptoproduction reactions introduces Generalized Parton Distribution (GPDs)
• Carry new Information about the dynamical degrees of freedom inside the Nucleon
• In the Bjorken scaling regime(Q2→∞, xB finite), the amplitude for exclusive scattering reaction can be factorized into
• A hard scattering part (exactly calcluable in pQCD)
• A nucleon structure part (parameterized via GPDs– handbag approximations)
Generalized Parton Distributions
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Inclusive Scattering Compton Scattering
p
Deeply Virtual Compton Scattering (DVCS)
GPDs depend on 3 variables, e.g. H(x, ξ, t). They probe the quark structure at the amplitude level.
t
Handbag mechanism 2x – longitudinal momentum transfer
real g
p p
q = 0p p
From Inclusive to Exclusive Scattering
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e’
p
e
y
x
z*
plane
ee’* plane
*pep ep
Kinematics
Deeply Virtual Compton Scattering• Virtual Compton Scattering in the Bjorken regime• Virtual Compton Scattering : Electroproduction of photons from
nucleons• The cleanest way of gathering information on nucleon structure• The simplest experiment for studying GPDs (W > 2GeV, Q2 > 1 (GeV/c)2)
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Eo = 11 GeVEo = 6 GeVEo = 4 GeV
BH
DVCS
TBH : given by elastic form factors F1, F2
TDVCS: determined by GPDs
BH-DVCS interference generates beam and target polarization asymmetries that carry the proton structure information.
DVCS
BH
p p
e e
42
2
4 4
2 2
1,1 0,12
| |
Im( )
1 Im sin Im sin 2
DVCS BH
B
DVCS BH
B B
dT T
dQ dx dtd
d dT T
dQ dx dtd dQ dx dtd
a M b M OQ
Accessing GPDs through DVCS
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2-D Scottyz
x
z
y
3-D Scotty
x
1-D Scotty
x
pro
bablit
yCalcium
Water
Carbon
Deep Inelastic Scattering & PDs
Deeply Virtual Exclusive Processes & GPDs
GPDs & PDs
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e.g. H(, t) =Hq(x, , t)dx
x- + i
Hq(x, , t)dx
x-+ iHq(, , t)
cross section difference
H q: Probability amplitude for P to emit a parton q with x+ and P’ to absorb it with x- .
GPDs: H, E unpolarized, H, E polarized~~
g* g
)( xP )( xP
GPD’s
real part imaginary part
=
DVCS and GPDs
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A =
=
Unpolarized beam, transverse target:
UT~ sin{k(F2H – F1E) + …. }d
Kinematically suppressed
H(t), E(t)
Unpolarized beam, longitudinal target:
UL~ sin{F1H+(F1+F2)(H +/(1+)E) -.. }d~
Kinematically suppressed
H(,t)~
LU~ sin{F1H + (F1+F2)H +kF2E}d~
Polarized beam, unpolarized target:
H(,t)
Kinematically suppressed ~ xB/(2-xB)
k = t/4M2 ~
Measuring GPDs through polarization
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• Longitudinal Target-Spin Asymmetry AuL measured for epe'pϒ with 5.72 GeV electron beams
= 0.252 ± 0.042 = -0.022 ± 0.045
First DVCS measurement with spin-aligned target
S. Stepanyan et al.,PRL 87, 182002 (2001)
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• Theoretical calculations in good agreement with the magnitude and kinematic dependence of target-spin asymmetry, which is sensitive to GPDs and H
• Leading term Aulsin
increases with f increasing in agreement with model prediction
DsUL ~ sinfIm{F1H+x(F1+F2)H +… }df
Unpolarized beam, longitudinally spin-aligned target
S. Chen et al.,PRL 97, 072002 (2006)
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Polarized Targets in Radioactive Ion Beams
Polarized Proton Beams Extensively used in nuclear physics experiments.Polarization observables provided us with rich information on spin-dependences of nuclear interactions, nuclear structure, and reaction mechanism.
Polarized Proton in RIB Experimentswill bring stiffer understanding of structure of unstable nuclei
Polarized d and 3He Target with RIBwill bring us similar contribution in spin physics
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Why do we need polarized proton target? (I)
Spin-dependent Interactions Origin of fundamental properties of nuclei – Saturation, Shell,
Cluster structure
Spin-orbit Couplings Phenomenologically modelled by spin-orbit potential.
Spin-orbit potential Localized at the nuclear surface
where ρ(r) : density distribution
Will be modified in neutron rich nuclei. Should be composed of two parts localized at different positions
if p and n have different distributions. Would have extended shape correspondingly if n have
extended distribution in skin or halo nuclei.
dr
rd
rVLS
)(1~
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Why do we need polarized proton target? (II)
Measurement of Spin-dependent Asymmetry, Vector Analyzing Power: Direct approach to investigate modifications of spin-orbit potential in neutron rich nuclei.
Ex 1 : Determination of a spin-orbit term in optical potential from vector analyzing power for p elastic scattering from a nucleus.
Ex 2 : Spin-orbit splitting, energy difference between
single particle states determined from vector
analyzing power for transfer or p induced nuclear-knockout
reactions.
2
1lj
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Polarized Proton Target with RIB Need Solid Hydrogen target with high density for low RIB current
Use single crystal of Naphthalene (C10H8) doped with a small amount of
Pentacene (C22H14)
Proton polarization produced at high temperature of 100K and in low magnetic field of 0.1 T allowing a detection of low-energy recoiled proton
Use an electron alignment on the photo-excited triplet state of aromatic molecules
A pulsed laser light with a wavelength of 532 nm from Ar-ion laser are used to induce an electron alignment in the triplet state of pentacene.
The population difference in Zeeman sublevels of the triplet state is transferred to proton polarization by means of a cross polarization method.
Proton polarization of about 20 % has been achieved.
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1 Optical Excitation Electron Alignment
2 Cross Polarization Polarization Transfer
3 Decay to the Ground State
4 Diffuse the Polarization to Protons in Host Molecules by Dipolar Interaction
Repeating 1 4
T1
Triplet state
S0
S1
Singlet state
laser
+1
0
-1
S2
① ②③
④
Protons are polarized
100 s
Excitation Scheme of Pentacene Molecules
ms12%
76%
12%
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Complete Target System of RIKEN Polzrized p
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Present status: RIKEN
Radial dependence of spin-orbit potentials between a proton and helium isotopes.
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6He-p Cross-section & Analyzing Power Results
M. Hatao et al., Eur. Phys. J. AS01, 255 (2005)
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p – 6He , p – 8He Elastic Scattering in 71 MeV/A
Hep 6
Hep 8
S. Sakaguchi Ph.D. Thesis Univesity of Tokyo(2008)
t-matrix folding calculation. S. P. Weppner et al., PRC 61, 044601 (2000)
Non-local g-matrix folding calculation.K. Amos et al., Adv. in N. P.A 25, 275 (2000)
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• t-matrix : Effective Two-body Interaction in free space
• g-matrix : Complicated Medium Effects are taken into account.
• Full treatment of Exchange Amplitudes is important to describe the proton elastic scattering.
• As an effective interaction the Melbourne g-matrix was used.
• Contains Density-dependent Spin-orbit Interaction
g-matrix as an Effective Interaction
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•Microscopic calculation was carried out
•Reduction of the spin-orbit potential in 6He was found to be due to the diffuseness of the density.
•The spin-orbit potential in 6He is dominated by the contribution of the core.
A-dependence & Correlation between point proton radius and LS
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Measurement of Spin Observables Using a Storage Ring with Polarized Beam and Polarized Internal Gas Target
IUCF K. Lee et al., PRL 70, 738 (1993)
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Polarization Correlation Coefficient
T. Uesaka et al.,PL B 467 (1999)
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Physics Motivation with Polarized 3He and RIB
Study of unstable nuclei by performing (3He, α) scattering experiments with RI beams
Analyzing Power Ay in (3He, α) Reaction becomes in PWIA
1
11
lAY
)( slJ
)( slJ
Measure Ay and assign Jπ
Ex. Perform 34Si(3He, Alpha)33Si and study the excited state of 33Si
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Optical Pumping and Spin Exchange
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cell
optics
Diode Laser
Oven (160 oC)
pickup coil
e- beam
B ~ 30 Gauss
main coilsrf drive coils
Instrument Control
Polarized 3He Setup with Electron Beams
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Optics system
Oven, coils and heaters
Ion pump and gas panel
5000C Oven tobake cell assembly
Laser
Experimental Setup
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Results : Polarized 3He
3He NMR Signal
Polarization Dependence on time
Exponential Decay of polarization
2007.9.5 Polarized 3He achieved in Korea for the first time
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Summary
RIB Accelerator will provide us with world's forefront Physics in unstable nuclei
Demonstrated the effectiveness of polarized p, d, 3He in exploring new aspects of nuclei far from the stability line
RI beam experiment with polarized p, d, 3He targets will be a powerful tool to shed a light on the spin-orbit coupling in unstable nuclei