isospin diffusion experiment(s) at riken
DESCRIPTION
Isospin Diffusion Experiment(s) at RIKEN. Betty Tsang August 22, 2012. O utline. Introduction – MSU expeirment Experimental Setup in RIKEN Status of RIKEN isospin expeirments Proposed reaction 132Sn+112Sn, 124Sn. HIC constraints on symmetry energy. - PowerPoint PPT PresentationTRANSCRIPT
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Isospin Diffusion Experiment(s) at RIKEN
Betty TsangAugust 22, 2012
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Outline
• Introduction – MSU expeirment• Experimental Setup in RIKEN• Status of RIKEN isospin expeirments• Proposed reaction 132Sn+112Sn, 124Sn
HIC constraints on symmetry energy
Current constraints from HIC weigh heavily on isospin diffusion. (The n/p ratios are more for consistency checks due to large error bars at high nucleon energy.
Isospin Diffusion with Neck Fragments
This can be described by the isoscaling parameters and :
)ZNexp(C
Z,NYZ,NY
1
2
Liu et al.PRC 76, 034603 (2007).
Ri(α)=Ri(d) assuming d=mα+bd (residue asymmetry)α (isoscaling parameter)
BBAA
BBAAABi xx
xxxR
2/)(2
Confirm the assumed Linearity of α on δ
• α depends linearly on the asymmetry according to statistical and dynamic models.
• Experimentally verified in central collisions.
• Measure 118Sn on 118Sn to add a data point to 112Sn + 112Sn and 124Sn + 124Sn.
BBAA
BBAAABi xx
xxxR
2/)(2
Ri(α)=Ri(d) assuming d=mα+bd (residue asymmetry, BUU)α (isoscaling parameter, expt)
Isospin Transport in Residues
• Different amount of isospin diffusion for heavy residues.
• provide another isospin observable and impact parameter selection
iiksym SSE
0
3/2
0)(
Experiment 07038: Precision Measurement of Isospin Diffusion
• Investigates the density-dependence of the nuclear symmetry energy• 112,118,124Sn+ 112,118,124Sn Collisions• Combines the MSU Miniball, the LASSA Array, and the S800 Spectrograph
Incoming Beam, 70 MeV/u
Beam-like fragments 10<Z<50
J.R. Winkelbauer,7
Experiment 07038: Precision Measurement of Isospin Diffusion
Motions:1. Targets2. Downstream
scintillator/degrader (deflect beam away from focal plane)
Detectors3. miniball—b selection4. LASSA – detect Z<85. S800 – detect
residues 20<Z<45
J.R. Winkelbauer,8
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1. Introduction1.1 Data taken at MSU (Ex07038)
• 112,118,124Sn + 112,118,124Sn • ~5 mg/cm2 Targets• 70 MeV/u beam energy• Event rates 200-300/s• Beam Rate 2*107/s to 6*107/s• Millions of events:
BeamTarget
112Sn 118Sn 124Sn
112Sn / 43hr 11.4M/11.2hr x 8.7M/11.3hr118Sn / 43hr 3.8M/2.8hr 10.7M/8.4hr x124Sn / 43 hr 12.3M/10.6hr 10.1M/9.5hr 15.2M/10hr
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1.2 RIKEN Experiment
• 108Sn + 112Sn • 108Sn + 124Sn • 112Sn + 112Sn (referenced to MSU) • 112Sn + 124Sn (referenced to MSU)
Primary beam: 124Xe (10-30 pnA)No 124Sn beam because there is no 132Xe primary beam124Sn Beam is not availableProposed beams : 108Sn and 112SnProposed reactions:
Calculations use beam intensities in the proposal based on 100 pnA of 124Xe beams
Microball from WU
2. Proposed Experimental Set up
Chamber from RIKEN
Scintillator & degrader foil ladder
12Fast Plastic Scintillator with a hole in the center: Polystyrene ,C8H8, 1.06g/cm3, 125 micron
Target Thickness ( mg/cm2)
112Sn 50124Sn 50
Beam Energy ( MeV/u)
Intensity (pps)
108Sn 73 6e+5112Sn 73 1e+6124Sn 73 6e+5
Experimental Setup
BigRIPSZero Degree Spectrometer
TargetSlits
(It turns out that the beam intensity is only 20% of what is written in the proposal and here)
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6. Beam Charge States Measurement
Beam Brho(Tm) F9 slit (mm) Charge states
108Sn 2.64 -75 ~ 75 50+ , 49+ , 48+
112Sn 2.74 -75 ~ 75 50+ , 49+ , 48+
(With target, With Fast Plastic hole)
108Sn: 112Sn:
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3. Brho “Safe” Region
(In current setting, the same fragments from different reactions have the similar Brho. )
I. Avoid the beamII. Consider different reactions at the same time.
beam target Brho without plastic
Brho with plastic
108Sn 112Sn <2.58 <2.52124Sn <2.58 <2.52
112Sn 112Sn <2.68 <2.62124Sn <2.68 <2.62
124Sn 112Sn <2.995 <2.935124Sn <2.995 <2.935
Conclusion: choose the Brho region smaller than 2.58.
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7. Al Degrader (For Plan A)
Use the Al to replace the target to tune the beam into the fragments Brho region.
Beam Brho(Tm) F9 slit (mm) Al thickness (mg/cm2)
108Sn 2.505 -75 ~ 75 70.7 (7 layer)
112Sn 2.505 -75 ~ 75 101 ( 10 layer)
108Sn: 112Sn:
(No target, No Fast Plastic)
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5.2* Summary of the measured isotopes (for Plan B)
Zn(Z=30) Br(Z=35) Zr(Z=40) Rh(Z=45)
108Sn+112Sn (62?),63,64 73,74,75 83,84,85,86 93,94,95,96,97
108Sn+124Sn (62?),63,64 73,74,75 83,84,85,86 93,94,95,96,97
112Sn+112Sn (62?),63,64 73,74,75 83,84,85,86 93,94,95,96,97,98
112Sn+124Sn (62?),63,64 73,74,75 83,84,85,86 93,94,95,96,97,98
112Sn+112Sn(MSU)
61 ~ 66 72 ~ 77 83 ~ 89 93 ~ 101
112Sn+124Sn(MSU)
61 ~ 66 71 ~ 77 82 ~ 89 93 ~ 101
Press here to directly go back to Slide 16
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Status• Xe beam cancelled for December, 2012• Rachel Hodges will travel to RIKEN in week of Sept 10
and work on the chamber design & beam calculations.• Transport microball to RIKEN in Dec (Betty?)• Pursuing a separate set of electronics (loan from ORNL?)• Propose 132Sn+ 112, 124Sn; 124Sn+124Sn (match to MSU) to
Dec PAC• Run the proposed experiment as a campaign to the
108,112Sn + 112, 124Sn isospin diffusion expt.