ストレンジ・ダイバリオン探索実験に用いる 高時間分解能TOF検出器の開発

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ストレンジ・ダイバリオン探索実験に用いる 高時間分解能TOF検出器の開発 Development of a high-resolution TOF counter using MPPC array for strange-dibaryon searches 科研費 若手研究(B) 26800158 理化学研究所 仁科加速器センター 佐久間 史典 RIKEN F.Sakuma 日本物理学会第71回年次大会 @ 東北学院大学 2016, 3/21

d*: s-channel resonance Di-baryon (S=0) Discovery of d* di-baryon WASA@COSY, PRL106(2011)242302 p n  d p0 p0 (Tp=1.0/1.2/1.4GeV) d*: s-channel resonance m = 2.37 GeV, G = 68 MeV t-channel DD contribution

Y. Sada, et al., arXiv:1601.06876 (PTEP accepted) Di-baryon (S=-1) KbarNN bound state? Still controversial… E15? Y. Sada, et al., arXiv:1601.06876 (PTEP accepted) J-PARC E15: K- 3He  L p n (山我 21pAC-2)

experimental search via Di-baryon (S=-2) Belle PRL110,222022(2013). H di-baryon? (resonance?) Lattice-QCDs predict the existence, but… No experimental evidence so far KbarKbarNN bound state? Theo. calcs. predict the existence No experimental search has been performed p K experimental search via pbar 3He  K+ K0 L L S.Maeda, Y.Akaishi, T.Yamazaki Proc. Jpn. Acad., B 89 (2013) 418.

pbar+3He annihilation at rest with 3NA processes: 𝒑 + 𝟑 𝑯𝒆 →𝚲+𝚲+𝑿 LL Measurement pbar+3He annihilation at rest with 3NA processes: 𝒑 + 𝟑 𝑯𝒆 →𝚲+𝚲+𝑿 aiming to search for KbarKbarNN with deep bound energy: 𝑝 + 3 𝐻𝑒 → 𝐾 + + 𝐾 0 + 𝑲 − 𝑲 − 𝒑𝒑+𝐵.𝐸.−109𝑀𝑒𝑉 H-dibaryon (resonance): 𝑝 + 3 𝐻𝑒 → 𝐾 + + 𝐾 0 +𝑯 Gola of LL study LL prod. rate Study of IM(LL) LL interaction 3He(stopped-pbar, LL) measurement would provide hints of S=-2 di-baryon

J-PARC K1.8BR  E31  E62/E57  E15  LoI Experiments to explore KbarN interaction At the KbarN threshold: Kbar-atom Below the KbarN threshold: L(1405) KbarNN KbarKbarNN  E31 川﨑 21aAW-6  E62/E57  E15 山我 21pAC-2 Sensitive in different energy region & isospin  LoI S.Ohnish et al., PRC93, 025207 KbarN

Cylindrical Detector System (CDS) CDH ~80ps AC T0 DC DEF ~1ns ~50ps Improvement of PID in the CDS TOF with T0-CDH  change to DEF-CDH for p/Kstop exp. present DEF consists of WLS-fiber+MPPC (st~1ns)  change to a high resolution detector (st<100ps) -

TOF Detector with MPPCs Plastic scint. with MPPC Multi-MPPCs Series connection Direct connection btw scint. and MPPCs Fast pre-amplifire Operation in magnetic field Small & Compact Cheep & Robust High-Resolution (st<100ps) Solution Pioneer works: MEG2 upgrade MPPC holder (3 MPPCs in series) Connect MPPC folder and scint. with thin wires Rapping: ESR (3M) S13360-3050CS (3*3mm2) Drill f0.5mm holes in a plastic scint.(EJ-230)

Fast Pre-Amplifier Fuji Diamond International Inc. 1504-S2 1 ch/module HP MSA-0385 (Cascadable Silicon Bipolar MMIC Amplifier) x 2 Pole Zero Cancellation Bandwidth (3dB): 100kHz ~ 2GHz Dynamic Range (output): -2V ~ +2V Gain: 10~16 (depend on PZC) Noise: <10mV rms HP MSA-0385 HV out in HV in out +12V (140mA) 8cm 4.5cm

Pre-Test with Cosmic-Ray 2 types of MPPCs 2nd gen. MPPC (S12572-050C) 3rd gen. MPPC (S13360-3050CS) CAMAC(ADC/TDC)+Kinoko 95mm 5mm 20mm MPPC*3 (3mm2) Cover Ratio: 27% Vmax 3rd gen. MPPC (S13360-3050C) has better performance

Beam-Test @ K1.8BR Beam-test with 1 GeV/c p- @ K1.8BR beam-dump in Nov.-Dec., 2015 length and thickness dependence CAMAC(ADC/TDC)+Kinoko ~1000 trig./spill(5.5s) [2*2mm2]

Beam-Test @ K1.8BR Beam-test with 1 GeV/c p- @ K1.8BR beam-dump in Nov.-Dec., 2015 length and thickness dependence CAMAC(ADC/TDC)+Kinoko ~1000 trig./spill(5.5s) [2*2mm2] ADC slewing correction

Results st<80ps was achieved with the new DEF Counter L mm 5or3mm 20mm MPPC*3 (3mm2) Cover Ratio: (t=5mm) 27% (t=3mm) 45% st<80ps was achieved with the new DEF Counter sum of # of Npe > 100 no position dependence of st st~80 ps was achieved with “l~200mm (t=5mm)” st~100ps is expected with “l=300mm (t=5mm)”

New DEF Design of the new DEF was completed all modules have been in hand will be installed in this year? depend on beam-time schedule @ K1.8BR 14mm f168mm Effective area: 96*100mm2

Summary A high-resolution TOF counter using MPPC array was developed for strange-dibaryon searches KbarNN (E15): K- 3He  L p n KbarKbarNN (LoI): pbar 3He  K+ K0 L L A new Beam-Definition-Counter (DEF) was fabricated and we confirmed st to be <80ps A plastic scintillator (3*20*115mm3) with 3 MPPCs in series connection Also we achieved st~80ps with a l=200mm (t=5mmm) counter Outlook: Pre-amplifire: integration in 1-module (~8 channels) Counter: test of a large size detector for a neutron counter, etc. c.f. NueLAND@FAIR: 270*5*5cm3, 6mm2-MPPC*4, st<150ps

Past Experiments of Double-Strangeness Production in Stopped-pbar Annihilation Channel # of events yield (x10-4) DIANA@ITEP [pbar+Xe] PLB464, 323 (1999). K+K+X 4 0.31+/-0.16 K+K0X 3 2.1+/-1.2 OBELIX @CERN/LEAR [pbar+4He] NPA797, 109 (2007). K+K+S-S-ps 34+/-8 0.17+/-0.04 K+K+S-S+np- 36+/-6 2.71+/-0.47 K+K+S-Ln 16+/-4 1.21+/-0.29 K+K+K-Lnn 4+/-2 0.28+/-0.14 Double strangeness production-yield: O(10-4) No result of LL measurement so far

Trigger rate = ~1k/spill Simple multiplicity trigger in the CDS Estimated trigger rate at 50 kW with Geant4.10 QGSP BERT physics list. SC: start counter Trigger rate = ~1k/spill NO problem!

Expected Yield & Sensitivity Expected yield @ 50kW: 10-4 [LL/pbar] * 800 [pbar/spill] * 655 [spill/h] * 21 [h] ~ 1100 [LL/day] * 0.01 [acceptance*Lpp-] * 0.7 [DAQ*ana] * 14 [days] ~ 110 [LL/2-weeks] R(H/K-K-pp) = 10-5/pbar  N(H/K-K-pp) ~ 10/2-weeks Sensitivity of LL *S/N of LL is assumed to be 2.5 LL I.M. LL~10-4/pbar sensitivities of ~10-5 (3s)