![Page 1: HypTPC for high-rate beamslambda.phys.tohoku.ac.jp/nstar/content/files/detectorWS...HypTPC for high-rate beams 佐甲博之(原子力機構) 新学術領域「中性子星核物質」](https://reader036.vdocuments.pub/reader036/viewer/2022062607/603f5fe5d9554514e75fce8b/html5/thumbnails/1.jpg)
HypTPC for high-rate beams
佐甲博之(原子力機構)
新学術領域「中性子星核物質」
第2回検出器ワークショップ
2017/3/4, 東工大
1
![Page 2: HypTPC for high-rate beamslambda.phys.tohoku.ac.jp/nstar/content/files/detectorWS...HypTPC for high-rate beams 佐甲博之(原子力機構) 新学術領域「中性子星核物質」](https://reader036.vdocuments.pub/reader036/viewer/2022062607/603f5fe5d9554514e75fce8b/html5/thumbnails/2.jpg)
Outline
• HypTPCの設計
– The TPC vs HypTPC
• High rateへの対応
• Field cageの帯電対策
• HypTPC,TPCの応用
2
![Page 3: HypTPC for high-rate beamslambda.phys.tohoku.ac.jp/nstar/content/files/detectorWS...HypTPC for high-rate beams 佐甲博之(原子力機構) 新学術領域「中性子星核物質」](https://reader036.vdocuments.pub/reader036/viewer/2022062607/603f5fe5d9554514e75fce8b/html5/thumbnails/3.jpg)
TPC • The best three-dimensional imaging tracker
– Pad position (x,z) and drift time (y)
– Easy for 3-d pattern recognition
– dE/dx can be measured with large number of
layers
– Big detector possible
• Disadvantage: high-rate capability
– Limited primarily by electron drift time
• e.g. Drift length(L)=50cm, Drift velocity(v)=5cm/ms
• t = 10ms (105Hz)
• If the rate is higher, events overlap
– Field distortion due to positive ions 3
![Page 4: HypTPC for high-rate beamslambda.phys.tohoku.ac.jp/nstar/content/files/detectorWS...HypTPC for high-rate beams 佐甲博之(原子力機構) 新学術領域「中性子星核物質」](https://reader036.vdocuments.pub/reader036/viewer/2022062607/603f5fe5d9554514e75fce8b/html5/thumbnails/4.jpg)
4
• Drift volume : uniform E
• End cap chamber for signal amplification
• B parallel to E
– Smaller diffusion size higher resolution
The PEP-4 TPC
G. D. Cowan, LBL-24715 (1988)
at PEP storage ring (SLAC)
End cap chamber
Cathode
![Page 5: HypTPC for high-rate beamslambda.phys.tohoku.ac.jp/nstar/content/files/detectorWS...HypTPC for high-rate beams 佐甲博之(原子力機構) 新学術領域「中性子星核物質」](https://reader036.vdocuments.pub/reader036/viewer/2022062607/603f5fe5d9554514e75fce8b/html5/thumbnails/5.jpg)
• Gating grid
• Amplification
with anode
wires
– Ion backflow
~ 100%
5
The PEP-4 TPC
![Page 6: HypTPC for high-rate beamslambda.phys.tohoku.ac.jp/nstar/content/files/detectorWS...HypTPC for high-rate beams 佐甲博之(原子力機構) 新学術領域「中性子星核物質」](https://reader036.vdocuments.pub/reader036/viewer/2022062607/603f5fe5d9554514e75fce8b/html5/thumbnails/6.jpg)
• Large acceptance
– Target “inside” drift volume
• Good position and decay vertex resolution
– B//E
– Solenoid: poor momentum resolution in the forward direction
Vertical B field (good resolution in the forward direction)
HypTPC design
6
PEP-4/LEPS like TPC
B E Opening
for beam &
produced
particle
Helmholtz magnet Hole for beampipe/target
Coil and Yoke
(Solenoid)
TPC
B
E
Target holder
Beam Beam
![Page 7: HypTPC for high-rate beamslambda.phys.tohoku.ac.jp/nstar/content/files/detectorWS...HypTPC for high-rate beams 佐甲博之(原子力機構) 新学術領域「中性子星核物質」](https://reader036.vdocuments.pub/reader036/viewer/2022062607/603f5fe5d9554514e75fce8b/html5/thumbnails/7.jpg)
7
HypTPC
Design for high-rate capability
Double suppression of ion backflow
• Gating Grid
• GEM(Gas Electron Multiplier)
Suppression of positive-ion backflow causing field distortion
• Mask GEM
• Exchange of the target holder possible for various targets
p- beam ~
550
Gating grid wires GEMs (electron amplification)
Pad plane
Target holder (E45)
500φ 70φ
B=1.5T
E=180V/cm
P-10 gas
target
ionization
Electron
drift
p-
p+
n e-
Gas vessel
Field cage (sensitive volume)
![Page 8: HypTPC for high-rate beamslambda.phys.tohoku.ac.jp/nstar/content/files/detectorWS...HypTPC for high-rate beams 佐甲博之(原子力機構) 新学術領域「中性子星核物質」](https://reader036.vdocuments.pub/reader036/viewer/2022062607/603f5fe5d9554514e75fce8b/html5/thumbnails/8.jpg)
J-PARC E42 setup
8
• 1.8 GeV/c K- beam at 106 / spill on a diamond target
• (K-,K+) tagged by KURAMA Spectrometer
• Search for H→LL→p-p-pp , H→Lp-p→ p-p-pp in HypTPC (Hyperon-TPC)
Drawn by S.H. Kim
H→ΛΛ
H→Λpπ-
1.0 μb/sr
0.2 μb/sr
11000 LL events
and 1440 H-dibaryons in 33-day experiment
LL invariant mass resolution
=1.5 MeV/c2
![Page 9: HypTPC for high-rate beamslambda.phys.tohoku.ac.jp/nstar/content/files/detectorWS...HypTPC for high-rate beams 佐甲博之(原子力機構) 新学術領域「中性子星核物質」](https://reader036.vdocuments.pub/reader036/viewer/2022062607/603f5fe5d9554514e75fce8b/html5/thumbnails/9.jpg)
Measure (p,2p) in HypTPC p-p→p+p-n, p0p-p 2 charged particles + 1 neutral particle
p+p→p0p+p, p+p+n →missing mass
p+- beam at 106 / spill
on liquid-H target
(p=0.73 – 2.0 GeV/c)
E45 : 30M events in 15 days
Enhance statistics of world’s
data by factor of 130 LH target
9
E45 setup
Hyp-TPC Helmholtz
Dipole magnet
Trigger with hodoscope
p+- beam
![Page 10: HypTPC for high-rate beamslambda.phys.tohoku.ac.jp/nstar/content/files/detectorWS...HypTPC for high-rate beams 佐甲博之(原子力機構) 新学術領域「中性子星核物質」](https://reader036.vdocuments.pub/reader036/viewer/2022062607/603f5fe5d9554514e75fce8b/html5/thumbnails/10.jpg)
10
Readout pads
Pad size
2.4 x 9 mm2 (inner layer)
2.4 x 13 mm2 (outer layer)
32 pad rows (rings)
No. of pads = 5768 520
215
520 Position resolution <300mm
(L>10cm)
Dp/p=1-3% (p,p)
![Page 11: HypTPC for high-rate beamslambda.phys.tohoku.ac.jp/nstar/content/files/detectorWS...HypTPC for high-rate beams 佐甲博之(原子力機構) 新学術領域「中性子星核物質」](https://reader036.vdocuments.pub/reader036/viewer/2022062607/603f5fe5d9554514e75fce8b/html5/thumbnails/11.jpg)
544
54
4
130
Target
position
11
GEM (Gas Electron Multiplier)
・4 GEM (250mmx250mm) sheets
・3-GEM layers
50mm + 50mm +100mm thick
Gain ~ 104
Segmented electrodes
・to reduce spark rate / electrode
・to minimize acceptance loss
when an electrode is broken due
to discharge
Simulated Hit distribution
![Page 12: HypTPC for high-rate beamslambda.phys.tohoku.ac.jp/nstar/content/files/detectorWS...HypTPC for high-rate beams 佐甲博之(原子力機構) 新学術領域「中性子星核物質」](https://reader036.vdocuments.pub/reader036/viewer/2022062607/603f5fe5d9554514e75fce8b/html5/thumbnails/12.jpg)
Mask GEM for >106 Hz beam Reduce GEM HV in the beam trajectory region to make
beam trajectories invisible
“Mask region” is adjustable (5mm pitch).
Mask GEM
Mask region (5mm pitch)
Each electrode can be applied HV independently.
![Page 13: HypTPC for high-rate beamslambda.phys.tohoku.ac.jp/nstar/content/files/detectorWS...HypTPC for high-rate beams 佐甲博之(原子力機構) 新学術領域「中性子星核物質」](https://reader036.vdocuments.pub/reader036/viewer/2022062607/603f5fe5d9554514e75fce8b/html5/thumbnails/13.jpg)
HypTPC
13
Field cage
GEMs
Readout pads
![Page 14: HypTPC for high-rate beamslambda.phys.tohoku.ac.jp/nstar/content/files/detectorWS...HypTPC for high-rate beams 佐甲博之(原子力機構) 新学術領域「中性子星核物質」](https://reader036.vdocuments.pub/reader036/viewer/2022062607/603f5fe5d9554514e75fce8b/html5/thumbnails/14.jpg)
Ion backflow
Backflow ratio
BR= Iion/Ielectron
Cathode
90Sr
Gating grid
pad A
A ions produced
in GEMs
e- GEMs
Iion
Ielectron
Ie/Ii~4%
e- e- e-
i+ i+ i+ i+
Ie/Ii<0.04% with
the gate closed
14
EI
![Page 15: HypTPC for high-rate beamslambda.phys.tohoku.ac.jp/nstar/content/files/detectorWS...HypTPC for high-rate beams 佐甲博之(原子力機構) 新学術領域「中性子星核物質」](https://reader036.vdocuments.pub/reader036/viewer/2022062607/603f5fe5d9554514e75fce8b/html5/thumbnails/15.jpg)
15
TPC prototype test NIMA763(2014)65-81
• Beam test at RCNP – Proton beam at 400 MeV
– Beam rate up to 106 Hz /cm2
Hit position distortion<0.1mm with GG
Efficiency vs beam rate
3m
TPC
SSD
Proton
beam
Position resolution (B=0) sx=0.40mm (4mm pad)
Gate open at gate operation
![Page 16: HypTPC for high-rate beamslambda.phys.tohoku.ac.jp/nstar/content/files/detectorWS...HypTPC for high-rate beams 佐甲博之(原子力機構) 新学術領域「中性子星核物質」](https://reader036.vdocuments.pub/reader036/viewer/2022062607/603f5fe5d9554514e75fce8b/html5/thumbnails/16.jpg)
TPC hit distortions
TPC
Beam
High density positive ion sheet
GEM
Electron drift path
Primary
electrons
16
xTPC (mm)
xT
PC
-xS
SD
(mm
)
GATE open Beam rate = 9x103/cm2
![Page 17: HypTPC for high-rate beamslambda.phys.tohoku.ac.jp/nstar/content/files/detectorWS...HypTPC for high-rate beams 佐甲博之(原子力機構) 新学術領域「中性子星核物質」](https://reader036.vdocuments.pub/reader036/viewer/2022062607/603f5fe5d9554514e75fce8b/html5/thumbnails/17.jpg)
Particle identification with TPC
17
p-
p+
p
K+
p/K : p<=0.5 GeV/c
p/p : p<=1.1 GeV/c
E45
Courtesy of S.H. Hwang
![Page 18: HypTPC for high-rate beamslambda.phys.tohoku.ac.jp/nstar/content/files/detectorWS...HypTPC for high-rate beams 佐甲博之(原子力機構) 新学術領域「中性子星核物質」](https://reader036.vdocuments.pub/reader036/viewer/2022062607/603f5fe5d9554514e75fce8b/html5/thumbnails/18.jpg)
Modification of the strip pattern
(field cage and target holder)
The place
where positive
Ions can be
attached
1.5
1
0.5
2
Remove
Insulator
(ALICE-TPC
Like solution)
ALICE-TPC field strips
Original
Modified
![Page 19: HypTPC for high-rate beamslambda.phys.tohoku.ac.jp/nstar/content/files/detectorWS...HypTPC for high-rate beams 佐甲博之(原子力機構) 新学術領域「中性子星核物質」](https://reader036.vdocuments.pub/reader036/viewer/2022062607/603f5fe5d9554514e75fce8b/html5/thumbnails/19.jpg)
Ion drift outside the field cage • Most serious problem
• All the positive ions hit the field cage wall
Equipotential lines Drift lines of positive ions
along a beam particle
Gas vessel wall
(actual a metal plate) Field strip wall
(printed circuit on polyimide)
Gas vessel wall Field strip wall
![Page 20: HypTPC for high-rate beamslambda.phys.tohoku.ac.jp/nstar/content/files/detectorWS...HypTPC for high-rate beams 佐甲博之(原子力機構) 新学術領域「中性子星核物質」](https://reader036.vdocuments.pub/reader036/viewer/2022062607/603f5fe5d9554514e75fce8b/html5/thumbnails/20.jpg)
20
![Page 21: HypTPC for high-rate beamslambda.phys.tohoku.ac.jp/nstar/content/files/detectorWS...HypTPC for high-rate beams 佐甲博之(原子力機構) 新学術領域「中性子星核物質」](https://reader036.vdocuments.pub/reader036/viewer/2022062607/603f5fe5d9554514e75fce8b/html5/thumbnails/21.jpg)
![Page 22: HypTPC for high-rate beamslambda.phys.tohoku.ac.jp/nstar/content/files/detectorWS...HypTPC for high-rate beams 佐甲博之(原子力機構) 新学術領域「中性子星核物質」](https://reader036.vdocuments.pub/reader036/viewer/2022062607/603f5fe5d9554514e75fce8b/html5/thumbnails/22.jpg)
22
![Page 23: HypTPC for high-rate beamslambda.phys.tohoku.ac.jp/nstar/content/files/detectorWS...HypTPC for high-rate beams 佐甲博之(原子力機構) 新学術領域「中性子星核物質」](https://reader036.vdocuments.pub/reader036/viewer/2022062607/603f5fe5d9554514e75fce8b/html5/thumbnails/23.jpg)
Physics possibilities with HypTPC • L(1405) : p-pK0L(1405)
L(1405)Lg (KN compositeness, T. Sekihara, PRC89 (2014) 025202)
• L*, S* studies in K-p reactions with PWA
– K-pK0n,pS,pL,hL,ppL,pKn,…
• K-pp : p+dK+K-pp
K-ppLp,S0p,Lp0p,S0p0p
• X excited states: K-p K+X-*, X-* LK-, S0K-, S-K0, X-p0, X0p-, X-g
K-p K0X0*, X0* LK0, S0K0, S+K-, X-p+
• X-C atom (E42) :K-CK+X-X, X- capture in C
X-ray detection in TPC? (Ar gas) 23
![Page 24: HypTPC for high-rate beamslambda.phys.tohoku.ac.jp/nstar/content/files/detectorWS...HypTPC for high-rate beams 佐甲博之(原子力機構) 新学術領域「中性子星核物質」](https://reader036.vdocuments.pub/reader036/viewer/2022062607/603f5fe5d9554514e75fce8b/html5/thumbnails/24.jpg)
Application of TPCs • High multiplicity events in HI collisions
– RHIC-STAR, LHC-ALICE(50kHz,continuous readout)
• TPCs with various gas
– X-ray detection (X-ray polarization) (DME, C2H6O)
• e from photoelectron effect
– g detection (Ar)
• Compton camera (e from Compton scattering)
– neutron detection (3He)
• Liquid Argon TPC
– Neutrino, dark matter search (good dE/dx resolution)
• Liquid Xe TPC
– High resolution gamma detection
24
![Page 25: HypTPC for high-rate beamslambda.phys.tohoku.ac.jp/nstar/content/files/detectorWS...HypTPC for high-rate beams 佐甲博之(原子力機構) 新学術領域「中性子星核物質」](https://reader036.vdocuments.pub/reader036/viewer/2022062607/603f5fe5d9554514e75fce8b/html5/thumbnails/25.jpg)
25
Summary • TPC is an excellent detector for 3-d imaging
• However,TPC has a disadvantage for high particle rate
• A large acceptance TPC for E42 (H-dibaryon search) and E45 (baryon resonance study) experiments at J-PARC for high rate beams has been developed – Target inside drift volume with a target holder
– GEMs and gating grid to suppress field distortion
• Applications of HypTPC to other hadron physics possible with various targets (and gas?)