1 / 24

Setup for hypernuclear gamma-ray spectroscopy at the J-PARC K1.8 beam line

Setup for hypernuclear gamma-ray spectroscopy at the J-PARC K1.8 beam line. Department of Physics, Tohoku Univ. K. Shirotori for the Hyperball-J collaboration. Contents. Introduction Magnetic spectrometer : SksMinus g -ray detector array : Hyperball-J Summary. Introduction.

elinor
Télécharger la présentation

Setup for hypernuclear gamma-ray spectroscopy at the J-PARC K1.8 beam line

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Setup for hypernuclear gamma-ray spectroscopy at the J-PARC K1.8 beam line Department of Physics, Tohoku Univ. K. Shirotori for the Hyperball-J collaboration

  2. Contents • Introduction • Magnetic spectrometer : SksMinus • g-ray detector array : Hyperball-J • Summary K. Shirotori NP07 6/2

  3. Introduction

  4. E13 Day-1 experiment at J-PARC Several light hypernuclear g-ray spectroscopy experiments are planned. (4LHe,7LLi, 10LB, 11LB, 19LF) (K-, p- ) reaction @ pK = 1.5 GeV/c Hyperball-J Particle-g coincidence g-ray measurement Missing mass analysis Optimized magnetic spectrometer + Hyperball-J K. Shirotori NP07 6/2

  5. Magnetic spectrometer -SksMinus-

  6. Previous SKS setup • Incident beam direction • Size and placement of detectors at the exit of the SKS magnet 2.2T qscat~20° 1.05 GeV/c (p+, K+) reaction (K+ 0.72 GeV/c) K. Shirotori NP07 6/2

  7. Previous SKS setup • Incident beam direction • Size and placement of detectors at the exit of the SKS magnet 2.7T qscat~20° 1.05 GeV/c (p+, K+) reaction (K+ 0.72 GeV/c) K. Shirotori NP07 6/2

  8. SksMinus setup For the beam condition • Determination of incident beam angle (20 degree) • Larger drift chamber 2.7T qscat~20° 1.05 GeV/c (p+, K+) reaction (K+ 0.72 GeV/c) K. Shirotori NP07 6/2

  9. SksMinus setup (K-, p- ) reaction @ pK = 1.5 GeV/c ⇒Analyze 1.4 GeV/c p- Requirements • Acceptance >100 msr, ~20o scattering angles • Momentum resolution < 4 MeV/c (FWHM) SDC1~4 : Drift chambers STOF : TOF counter SAC : Aerogel Cherenkov counter Beam decay background veto _ • SMF : m- from K- → m- + n • SP0 : p- from K- → p- + p0 Target ~20 g/cm2 1 m K. Shirotori NP07 6/2

  10. Drift chamber and TOF counter To keep the large acceptance BD and BT from BNL are used as SDC3&4 and STOF, respectively. BD BD1 BD2 BT 48D48 Magnet 270 cm 170 cm Ajimura-san BNL-AGS D6 line K. Shirotori NP07 6/2

  11. Simulation results of acceptance and momentum resolution • Acceptance at 1.4 GeV/c, ~130 msr • Enough angular acceptance, ~20 degree • Momentum resolution at 1.4 GeV/c ~2.1 MeV/c (FWHM) K. Shirotori NP07 6/2

  12. Target 20cm BAC SAC m Beam K Decay Background events : Beam decay • Trigger rate • Missing mass _ K- → m-n (63.4%) ⇒Muon Filter K- → p- p0 (21.1%) ⇒PiZero Veto Overlap _ K. Shirotori NP07 6/2

  13. Beam decay veto counters Muon Filter γ p- (absorbed in the iron) m- (passing through) 86%of m-n events detected Others rejected (stopped in the iron) by offline analysis Totally > 99.9 % • Over kill for true π ~2.5% 80% of p-p0 events detected 10 sets of 3 mm lead plate and 8 mm scintillation counter layer at 1.5 GeV/c beam. Sufficient performance to reduce the trigger rate and background K. Shirotori NP07 6/2

  14. Hyperball-J

  15. Hyperball-J Severe radiation damage High counting rate at J-PARC • Mechanical cooler • PWO background suppressor • Waveform readout Simulated efficiency by Geant4 Hyperball-J (half) ~6% photo peak efficiency @ 1 MeV K. Shirotori NP07 6/2

  16. R&D in KEK and Tohoku Univ. Cooling power Ge crystal temperature less than 85K when biased Low mechanical vibration for 2 keV energy resolution Minimization of microphonics noise New Ge detector with Mechanical cooling 13 cm Cooler Ge 10 cm Mechanical cooler ⇒Suppression of the radiation damage effect with Ge crystal below 85 K (Liquid nitrogen cooling ~90 K) Ge Achieved K. Shirotori NP07 6/2 Compressor

  17. Background suppressor : PbWO4 The PWO crystal has very first decay constant ~6 ns. (~300 ns for BGO) But small light yield (PWO/BGO=1/10) • Doped PWO crystal • Cooling of PWO below 0℃ Ge energy spectrum 1 MeV g ray (simulation) -type U-type W-type L-type PWO suppression for g ray spectroscopy is possible. K. Shirotori NP07 6/2

  18. 10 V Waveform readout Pulse height ADC ⇒ Sampling ADC (waveform digitization) (after shaping) To improve energy resolution and recover rejected events at high counting rates • Baseline shift restoration • Pile-up signal decomposition Baseline Preamp output After shaping K. Shirotori NP07 6/2

  19. Waveform readout Pulse height ADC ⇒ Sampling ADC (waveform digitization) (after shaping) To improve energy resolution and recover rejected events at high counting rates • Baseline shift restoration • Pile-up signal decomposition No baseline restoration In the LNS test experiment, the positron beam is irradiated to Ge detector to make frequent baseline shits by reset signal. ⇒The restoration of the baseline shits 3.7 keV⇒ 3.1 keV (FWHM) (2.6 keV w/o beam) Baseline restoration 60Co 1.3 MeV g-ray spectrum K. Shirotori NP07 6/2

  20. Summary

  21. Summary • J-PARC E13 experiment by the (K-, p-) reaction @ pK =1.5 GeV/c • Optimal magnetic spectrometer • New Hyperball system for the high counting rate • Magnetic spectrometer, SksMinus and newly constructed array, Hyperball-J SksMinus performance • More than 100 msr acceptance and 20 degree coverage • ~2 MeV/c momentum resolution Hyperball-J • ~6 % efficiency • Mechanical cooling system • PWO counter • Waveform readout The experiment will be performed in 2009. K. Shirotori NP07 6/2

  22. Backup

  23. Particle identification Reaction ID by BAC and SAC (n=1.03) @ trigger Rejection of K- beam through background SAC ~98% + Beam veto (SFV) STOF : Time resolution ~150 ps (rms) SAC BAC Beam veto (SFV) K. Shirotori NP07 6/2

  24. (K-, p-) reaction Large production rate (/beam) Large elementary cross section, n(K-, p-)L : order of mb > n(p+, K+)L : ~102mb, p(e, e’K+)L : ~1 mb Large sticking probability Angular selectivity Small momentum transfer q~5°~ 100 MeV/c : DL = 0 q~10°~ 200 MeV/c : DL = 1 or 2 @ 1.5 GeV/c beam Spin-flip cross section exists at large angles (q >10°). More advantages in hypernuclear g-ray spectroscopy experiment K. Shirotori NP07 6/2

More Related