First Experiments with The SpRIT-TPC at SAMURAI in RIKEN-RIBF
Mizuki Kurata-Nishimura
For SπRIT-TPC collaboration
- :EOS(symmetry energy
First Experiments with The SpRIT-TPC at SAMURAI in RIKEN-RIBF - - PowerPoint PPT Presentation
First Experiments with The SpRIT-TPC at SAMURAI in RIKEN-RIBF : EOS(symmetry energy Mizuki Kurata-Nishimura For S RIT-TPC collaboration
For SπRIT-TPC collaboration
132Sn + 124Sn108Sn + 112Sn124Sn + 112Sn112Sn + 124Sn300MeV/u
l 荷電粒子が通る l ガスがイオン化され電子が飛跡に沿って弾き飛ばされる。 l 電子を電場によってドリフトさせる。 l ドリフトしてきた電子を強い電場で増幅する。 l 検出した電荷をパッドの位置から2次元分布に変換。 l 到達した時間から3次元情報を算出
E field 135V/cm B field 0.5T Beam: 132Sn, 108Sn, 124Sn, 112Sn Target:112Sn, 124Sn Position in vertical drift direction from time
AsAd Boards 2D-motion target system
constructed at NSCL/MSU to be used in SAMURAI magnet chamber.
n π+, p, d, t…..
NeuLAND
2m
Sn ~300MeV/u SAMURAI dipole magnet
Beam 10Gb network CoBo CoBo CoBo CoBo
SpiRITROOT analysis Semi-online Analysis xrootd Disk DAQ Disk DAQ
48 AsAds in total 4 AsAds into
12 Cobos
AsAd <= 4 AGET (63 pads)
Issue 2, pp 144–151(2016)
AsAd
AGET AGET AGET AGET
AsAd
AGET AGET AGET AGET
AsAd
AGET AGET AGET AGET
AsAd
AGET AGET AGET AGET
Air cooling Assembling AsAds
–
– NIM paper is accepted
Detector Location In trigger Purpose SBT: Start Counters After STQ mag. Hitting Count number of beam and determine start timing Active Collimator In front
target No hit Reject beam passing through
target. KATANA- Veto After the exit window Pulse Height <=
eject beam-like residues with Z greater than 20 passing through the TPC Kyoto Array Left and Right side Multiplic ity >= 4 Trigger central collision events BDC: Beam Drift Chamber In beam line after S.C. not included Reconstruct a beam track NeuLAND 8.5m, 30deg not included Detect neutron and charged light particles
Active Collimator (no hit)
Beam
NeuLAND : Neutron detection SBT:Start Counter (hitting) Beam Drift Chamber(BDC)
1. Put reflecting point stickers on the measuring surface 2. Take pictures from several angles. 3. Analyze picture data. 4. The absolute position of point is reconstructed. 5. Absolute position determined with ~0.2mm. 6. This results will be submitted soon!
132Sn (49%) 108Sn (56%) 134Sb (10%) 110Sb (1.5%)
Beam Purity Energy [MeV/u] Target Purposeδ=(N-Z)/A Periods Time [h] Triggered Commissioning I
79Se
50% ~200 Al Full readout check
29‘15 Commissioning II
132Sn
50% ~300
Trigger system check inside the magnet
Xe
108Sn
49% 268.9
112Sn
neutron deficient δ = 0.09
64 10M Xe
112Sn
44% 270.2
124Sn
reference δ = 0.15
38 5.9M U
132Sn
57% 268.9
124Sn
neutron rich δ = 0.22
57 9.5M U
124Sn
10% 270.2
112Sn
reference δ = 0.15 May 30 – Jun. 1 ‘16 30 4.6M U (Z=1,2,3 A/Z=2) d, , 6Li ~300 Empty Gain Calibration
2.5 0.28M ~100 4.4 a
Top View
Side View
124Sn + 112Sn
1. Track separation 2. Riemann fit: 2D 3. Helix fit: 3D 4. Clustering 5. Initialize GENFIT parameters
t0: time at 5% of h
f: Fixed shape
Cosmic event
Reaction at target
Active target Before target
Target Ladder Entrance window
Background can be eliminated
Nice correlation indicates the successful operation of DAQ synchronization and vertex reconstruction Intrinsic spatial resolution is estimated to be ~ 1mm.
X Y
Two drift chambers provide us beam position at the target Each track extrapolated onto the target
URQMD+G4 132Sn(300MeV/u) + 124Sn
Impact Parameter [fm]
30 30 Central Peripheral Peripheral Central
KATANA_M
10%.
~10% inefficiency
1
>95% Efficiency
PID by TPC (132Sn + 124Sn @E/A=280MeV)