Joe Parker for the Cosmic Ray γ Group Kyoto University

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Transcription:

Joe Parker for the Cosmic Ray γ Group Kyoto University Cosmic Ray Group NID Project Team @ 京大 K. Hattori, C. Ida, S. Iwaki, S. Kabuki, H. Kubo, S. Kurosawa, K. Miuchi, H. Nishimura, J. D. Parker, T. Sawano, M. Takahashi, T. Tanimori, K. Ueno

μpic (10 10 cm 2 ) 400 μm Ele ectric field 10 cm Anode pitch: 400 μm. 256 256 strip read out (10 10 cm 2 size). Maximum gain: ~15000. Energy resolution: 22% @ 5.9 kev. Gain uniformity: ~4% (σ). > 1 month stable operation at gain of ~6000. Amplifier Shaper Discriminators Position Encoder

Aluminum vessel Aluminum drift plane (thickness = 0.5 mm) Drift cage μpic Drift cage μpic TPC measures 3D track of proton triton triton pair. Active volume: 10 10 5 cm 3. Gas mixture: Ar C 2 H 6 3 He (up to 2 atm total pressure). Position resolution: < 0.4 mm. Time resolution: ~1 μs (for neutron event). Detection efficiency: up to ~30% (for thermal neutrons). 0 cm 5 Amplifier Shaper Discriminators Entrance window

Amplifier Shaper Discriminators μpic FPGA encoder 33 bit LVDS ( 2) VME memory Proton and triton ID from pulse width distribution. > 2 improvement in position resolution. Digital out (256 ch 2) 32 bits: direction, time, position, edge External gate PC VME bus Data structure μpic 1 bit orientation Threshold 20 bits time 10 bits strip no. 1bit edge 0 1 ASD Time above threshold ( energy dep.) proton neutron position o triton

Data taken at Kyoto U. Tandem van de Graaff. Neutrons from 7 Li(p,n) 7 Be reaction (T p = 3 MeV). Gas mixture: Ar(82.8%) C 2H 6(9.2%) 3 He(8%) at 1 atm. Gas gain: ~1000. 1.3344(4) cm σ = 0.0476(3) 0476(3) cm Fast neutrons, γs, and p t tracks which escape the detector. durat tion X projection 1.31945(2) cm σ = 0.02834(1) cm 2D width from strips + time 3D track Time to distance: duration drift velocity 10 ns/clock pulse Drift velocity: ~34 μm/ns.

NOBORU beam line Experiment objectives Rate dependence of DAQ. Position resolution. Selection of neutron energy by time of flight. Demonstrate t SANS and radiography. Sample holder Beam heig ght (60 cm) NID (14.45m from moderator) Gas mixture: Ar(63%) C 2 H 6 (7%) 3 He(30%) at 2 atm. Detection efficiency: ~30%.

Single pulses Sum of pulses 40 ms DAQ bottlenecks FPGA encoder 100 MHz Output buffer LVD S VME to PC Data rates observed at J PARC 30 MHz 100 khz ~ 1.5 MHz. VME memory VME bus 2.6 PC MHz ~70 MHz peak rate. Output t buffer overflow 1.49 MHz 0.97 MHz ~16000 pulses Encoder output buffer (limits DAQ rate). VME to PC data transfer (limits DAQ live time). Max. rate ~1.4 MHz. DAQ live time ~20% at 1.49 MHz.

2 mm slits Position from midpoint of p t track. No proton ID Resolution: 960 ± 105 μm (σ) plus 5.0 cm proton ID 0.25 mm Cd test chart DAQ rate: ~1.2 MHz Exposure time: 8.9 min (with live DAQ) Proton ID from pulsewidth distribution. Corrected neutron interaction point. Resolution from edge: 349 ± 36 μm (σ)

~10 cm Neutron time of flight flight (TOF) N0 sample Steel 1 cm welded steel plate DAQ rate: 972 khz Exposure time: 10.5 min Bragg edges are clearly visible. Weld Steel plate Bragg edges i

Transmission for 59 Co 59 Co (TOF = 90.99 μs) Ta Mo Mn/Cu Co Na Cu 23 Na (TOF = 19.6 μs) Assorted metals DAQ rate: 1.48 MHz Exposure time: 5.5 min Known resonance at 132 ev (TOF = 90.9 μs). Observed at 90.86 ± 023 0.23 μs. Neutrons at resonance Neutrons at resonance energy for selective imaging.

~1 cm Distance from beam center Spherical SiO2 nanoparticles Diameter: ~200 nm. Sample distance: 1666 mm. Beam size: 4 4 mm 2. DAQ rate: 520 khz. Exposure time: 35.0 min. 7 Å 8 Å q projection (6 <λ< 10 Å) Position of diffraction peak depends on wavelength. Peak is constant in q.

TPC based on micro pattern gaseous detector and FPGA DAQ system. Position resolution of < 0.4 mm; timing resolution of ~1 μs. High data rates. Strong rejection of background gammas and fast neutrons. Detector performance studied at J PARC: Confirmed good position resolution with DAQ X ray mode 8. Selection of neutron energy by time of flight. Demonstrated application to SANS and radiography. μpic system is available in 10 10 cm 2, 20 20 cm 2, and 30 30 cm 2. Second 10 cm system built for JAEA. Now setting up 20 cm neutron imaging detector for use at 京大.