Joe Parker for the Cosmic Ray γ Group Kyoto University

Size: px
Start display at page:

Download "Joe Parker for the Cosmic Ray γ Group Kyoto University"

Transcription

1 Joe Parker for the Cosmic Ray γ Group Kyoto University Cosmic Ray Group NID Project 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

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

3 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: 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

4 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

5 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: ~ (4) cm σ = (3) 0476(3) cm Fast neutrons, γs, and p t tracks which escape the detector. durat tion X projection (2) cm σ = (1) cm 2D width from strips + time 3D track Time to distance: duration drift velocity 10 ns/clock pulse Drift velocity: ~34 μm/ns.

6 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%.

7 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.

8 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)

9 ~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

10 Transmission for 59 Co 59 Co (TOF = 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 ± μs. Neutrons at resonance Neutrons at resonance energy for selective imaging.

11 ~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.

12 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 cm 2, cm 2, and cm 2. Second 10 cm system built for JAEA. Now setting up 20 cm neutron imaging detector for use at 京大.

NEWAGE. Kentaro Miuchi (Kyoto University) (New generation WIMP search with an advanced gaseous tracker experiment)

NEWAGE. Kentaro Miuchi (Kyoto University) (New generation WIMP search with an advanced gaseous tracker experiment) Kentaro Miuchi (Kyoto University) with K. Nakamura, H. Nishimura T. Tanimori, H. Kubo, J. Parker, A, Takada, S. Iwaki, T. Sawano, Y. Matsuoka, Y. Sato, S. Komura (Kyoto) A. Takeda, H. Sekiya (Kamioka)

More information

Motivation Electron-Tracking Compton Telescope 1 st Flight of SMILE Preparation for next step summary

Motivation Electron-Tracking Compton Telescope 1 st Flight of SMILE Preparation for next step summary A. Takada (ISAS/JAXA), T. Tanimori, H. Kubo, K. Miuchi, S. Kabuki, Y. Kishimoto, J. Parker, H. Nishimura, K. Hattori, K. Ueno, S. Kurosawa, S. Iwaki, C. Ida, M. Takahashi, T. Sawano, K. Taniue, K. Nakamura,

More information

Motivation Electron-Tracking Compton Telescope 1 st Flight of SMILE Preparation for next step summary

Motivation Electron-Tracking Compton Telescope 1 st Flight of SMILE Preparation for next step summary A. Takada (ISAS/JAXA), T. Tanimori, H. Kubo, K. Miuchi, S. Kabuki, H. Nishimura, K. Hattori, K. Ueno, S. Kurosawa, C. Ida, S. Iwaki, M. Takahashi (Kyoto Univ.) Motivation Electron-Tracking Compton Telescope

More information

The simulation of the Electron Tracking Compton Camera with a gaseous time projection chamber and a scintillator

The simulation of the Electron Tracking Compton Camera with a gaseous time projection chamber and a scintillator The simulation of the Electron Tracking Compton Camera with a gaseous time projection chamber and a scintillator A. Takada 1, T. Tanimori 1, H. Kubo 1, H. Nishimura 1, K. Ueno 1, K. Miuchi 1, K. Tsuchiya

More information

Development of a new MeV gamma-ray camera

Development of a new MeV gamma-ray camera Development of a new MeV gamma-ray camera ICEPP Symposium February 16, 2004 Hakuba, Nagano, Japan Kyoto University Atsushi Takeda H. Kubo, K. Miuchi, T. Nagayoshi, Y. Okada, R. Orito, A. Takada, T. Tanimori,

More information

Precise Low-Energy Electron Tracking Using a Gaseous Time Projection Chamber for the Balloon-Borne Gamma Ray Compton Telescope

Precise Low-Energy Electron Tracking Using a Gaseous Time Projection Chamber for the Balloon-Borne Gamma Ray Compton Telescope Precise Low-Energy Electron Tracking Using a Gaseous Time Projection Chamber for the Balloon-Borne Gamma Ray Compton Telescope T. Mizumoto, T. Tanimori, H. Kubo, A. Takada, J. D. Parker, S. Sonoda, Y.

More information

1. MeV gamma ray Imaging & ETCC 2. Results of SMILE-I 3. Preparations of SMILE-II

1. MeV gamma ray Imaging & ETCC 2. Results of SMILE-I 3. Preparations of SMILE-II A. Takada, T. Tanimori, H. Kubo, K. Miuchi, S. Kabuki, J. D. Parker, Y. Kishimoto, T. Mizumoto, K. Ueno, S. Kurosawa, S. Iwaki, T. Sawano, K. Taniue, K. Nakamura, N. Higashi, Y. Matsuoka, S. Komura, Y.

More information

TitleDevelopment of an MeV gamma-ray ima. works must be obtained from the IEE

TitleDevelopment of an MeV gamma-ray ima.   works must be obtained from the IEE TitleDevelopment of an MeV gamma-ray ima Takeda, A; Kubo, H; Miuchi, K; Naga Author(s) Orito, R; Takada, A; Tanimori, T; U Bouianov, M Citation IEEE TRANSACTIONS ON NUCLEAR SCIENC 51(5): 2140-2144 Issue

More information

Micro Pixel Chamber Operation with Gas Electron Multiplier

Micro Pixel Chamber Operation with Gas Electron Multiplier Contents ts Micro Pixel Chamber Operation with Gas Electron Multiplier Kyoto University dept. of physics Cosmic-ray ygroup K. Hattori 1. μ-pic (Micro Pixel Chamber), micro-tpc (Time Projection Chamber

More information

Performance of the Gamma-ray Imaging Detector with Micro-TPC

Performance of the Gamma-ray Imaging Detector with Micro-TPC Performance of the Gamma-ray Imaging Detector with Micro-TPC Cosmic-Ray Group Dept. of Physics, Graduate School of Science, Kyoto University R.Orito Orito,H.Kubo,K.,H.Kubo,K.Miuchi,T.Nagayoshi, A.Takada,A.Takeda,T.Tanimori

More information

Balloon-borne experiment for observation of sub-mev/mev gamma-rays from Crab Nebula using an Electron Tracking Compton Camera

Balloon-borne experiment for observation of sub-mev/mev gamma-rays from Crab Nebula using an Electron Tracking Compton Camera Balloon-borne experiment for observation of sub-mev/mev gamma-rays from Crab Nebula using an Electron Tracking Compton Camera S. Komura, T. Tanimori, H. Kubo, A.Takada, S. Iwaki, S. Kurosawa, Y. Matsuoka,

More information

Direction-Sensitive Dark Matter Search --NEWAGE--

Direction-Sensitive Dark Matter Search --NEWAGE-- Direction-Sensitive Dark Matter Search --NEWAGE-- (New generation WIMP search with an advanced gaseous tracker experiment) Kentaro Miuchi (Kobe University) with K. Nakamura, A. Takada T. Tanimori, H. Kubo,

More information

Experiment of the 30 cm-cube ETCC under the Intense Radiations with Proton Beam

Experiment of the 30 cm-cube ETCC under the Intense Radiations with Proton Beam Experiment of the 30 cm-cube ETCC under the Intense Radiations with Proton Beam Contents Y. Matsuoka T. Tanimori, H. Kubo, A. Takada, J. D. Parker, T. Mizumoto, Y. Mizumura, S. Sonoda, D. Tomono, S. Iwaki,

More information

Performance of high pressure Xe/TMA in GEMs for neutron and X-ray detection

Performance of high pressure Xe/TMA in GEMs for neutron and X-ray detection Performance of high pressure Xe/TMA in GEMs for neutron and X-ray detection R. Kreuger, C. W. E. van Eijk, Member, IEEE, F. A. F. Fraga, M. M. Fraga, S. T. G. Fetal, R. W. Hollander, Member, IEEE, L. M.

More information

Observation of Gamma-Rays from Relativistic Electron Precipitation with Balloon Experiment around the Polar regions

Observation of Gamma-Rays from Relativistic Electron Precipitation with Balloon Experiment around the Polar regions Observation of Gamma-Rays from Relativistic Electron Precipitation with Balloon Experiment around the Polar regions Yoshitaka Mizumura (Kyoto Univ.) T. Tanimori, H. Kubo, A. Takada, J. D. Parker, T. Mizumoto,

More information

arxiv: v1 [physics.ins-det] 6 Aug 2015

arxiv: v1 [physics.ins-det] 6 Aug 2015 Preprint typeset in JINST style - HYPER VERSION arxiv:1508.0187v1 [physics.ins-det] 6 Aug 015 A performance study of an electron-tracking Compton camera with a compact system for environmental gamma-ray

More information

1. Motivation & Detector concept 2. Performance 3. Confirmation experiments 4. Summary

1. Motivation & Detector concept 2. Performance 3. Confirmation experiments 4. Summary A. Takada, T. Tanimori, H. Kubo, J. D. Parker, T. Mizumoto, Y. Mizumura, T. Sawano, K. Nakamura, Y. Matsuoka, S. Komura, S. Nakamura, M.Oda, K. Miuchi, S. Kurosawa 1. Motivation & Detector concept 2. Performance

More information

Direction-Sensitive Dark Matter Search --NEWAGE--

Direction-Sensitive Dark Matter Search --NEWAGE-- Direction-Sensitive Dark Matter Search --NEWAGE-- (New generation WIMP search with an advanced gaseous tracker experiment) Kentaro Miuchi (Kobe University) with K. Nakamura, A. Takada, T. Tanimori, H.

More information

1. Motivation & Detector concept 2. Performance 3. Applications 4. Summary

1. Motivation & Detector concept 2. Performance 3. Applications 4. Summary A. Takada, T. Tanimori, H. Kubo, K. Miuchi, J. D. Parker, T. Mizumoto, Y. Mizumura, T. Sawano, Y. Matsuoka, S. Komura, S. Nakamura, M. Oda, S. Iwaki, K. Nakamura, S. Sonoda, D. Tomono (Kyoto Univ.) 1.

More information

1. Motivation & Detector concept 2. Performance 3. Confirmation experiments 4. Summary

1. Motivation & Detector concept 2. Performance 3. Confirmation experiments 4. Summary A. Takada, T. Tanimori, H. Kubo, J. D. Parker, T. Mizumoto, Y. Mizumura, T. Sawano, K. Nakamura, Y. Matsuoka, S. Komura, S. Nakamura, T. Kishimoto, M. Oda, T. Takemura, S. Miyamoto, K. Miuchi, S. Kurosawa

More information

TPC-like analysis for thermal neutron detection using a GEMdetector

TPC-like analysis for thermal neutron detection using a GEMdetector Bernhard Flierl - LS Schaile TPC-like analysis for thermal neutron detection using a GEMdetector Triple GEM Detector B-Cathode 6 mm drift space 2 mm GEMs 2 mm 2 mm APV25 readout 2 µm B-converter cathode

More information

Precision neutron flux measurement with a neutron beam monitor

Precision neutron flux measurement with a neutron beam monitor Journal of Physics: Conference Series OPEN ACCESS Precision neutron flux measurement with a neutron beam monitor To cite this article: T Ino et al 2014 J. Phys.: Conf. Ser. 528 012039 View the article

More information

HARPO: Measurement of polarised gamma rays (1.7 to 72MeV) with the HARPO TPC

HARPO: Measurement of polarised gamma rays (1.7 to 72MeV) with the HARPO TPC HARPO: Measurement of polarised gamma rays (1.7 to 72MeV) with the HARPO TPC Philippe Gros for the HARPO collaboration 1/39 Gamma Astronomy HARPO project Setup at the NewSUBARU photon beam Gas monitoring

More information

Waste Characterization

Waste Characterization Radiation Monitoring Systems & Waste Characterization Lecture 4 - Neutron Detectors M.Taiuti MASTER UNIVERSITARIO DI II LIVELLO IN SCIENZE E TECNOLOGIE DEGLI IMPIANTI NUCLEARI Neutron Detectors What does

More information

R&D on Astroparticles Detectors. (Activity on CSN )

R&D on Astroparticles Detectors. (Activity on CSN ) R&D on Astroparticles Detectors (Activity on CSN5 2000-2003) Introduction Results obtained with the R&D activity (2000-2003) with some drift chambers prototypes are reported. With different photocathode

More information

Study of the HARPO TPC for a high angular resolution g-ray polarimeter in the MeV-GeV energy range. David Attié (CEA/Irfu)

Study of the HARPO TPC for a high angular resolution g-ray polarimeter in the MeV-GeV energy range. David Attié (CEA/Irfu) Study of the HARPO TPC for a high angular resolution g-ray polarimeter in the MeV-GeV energy range David Attié (CEA/Irfu) Outline Motivation of an MeV-GeV polarimeter Scientific case and expected performance

More information

Kiseki Nakamura (Kyoto university)

Kiseki Nakamura (Kyoto university) CYGNUS2013@Toyama 2013/06/10 Kiseki Nakamura (Kyoto university) T.Tanimori (1), K.Miuchi (2), K.Kubo (1), T.Mizumoto (1), J.Parker (1), A.Takada (3), H.Nishimura (1), T.Sawano (1), Y.Matsuoka (1), S.Komura

More information

Construction of the energy-resolved neutron imaging system RADEN in J-PARC MLF

Construction of the energy-resolved neutron imaging system RADEN in J-PARC MLF 3.5.5 Construction of the energy-resolved neutron imaging system RADEN in J-PARC MLF T. Shinohara 1, T. Kai 1, K. Oikawa 1, M. Segawa 1, M. Harada 1, T. Nakatani 1, M. Ooi 1, M. Arai 1, H. Sato 2, T. Kamiyama

More information

SIGN: A Pressurized Noble Gas Approach to WIMP Detection

SIGN: A Pressurized Noble Gas Approach to WIMP Detection SIGN: A Pressurized Noble Gas Approach to WIMP Detection J.T. White Texas A&M University Dark Side of the Universe U. Minnesota, 6/7/2007 Why Gaseous Nobles? Original Motivation: Neon Electron mobility

More information

Research at FSU, using RESOLUT facility Development of and research with two new detector-systems

Research at FSU, using RESOLUT facility Development of and research with two new detector-systems Nuclear Astrophysics and Structure Research with Radioactive Beams Research at FSU, using RESOLUT facility Development of and research with two new detector-systems ResoNeut: Low-energy neutron detector-array

More information

Measurement of the n_tof beam profile in the second experimental area (EAR2) using a silicon detector

Measurement of the n_tof beam profile in the second experimental area (EAR2) using a silicon detector Measurement of the n_tof beam profile in the second experimental area (EAR) using a silicon detector Fidan Suljik Supervisors: Dr. Massimo Barbagallo & Dr. Federica Mingrone September 8, 7 Abstract A new

More information

MONTE-CARLO SIMULATIONS OF TIME- RESOLVED, OPTICAL READOUT DETECTOR for PULSED, FAST-NEUTRON TRANSMISSION SPECTROSCOPY (PFNTS)

MONTE-CARLO SIMULATIONS OF TIME- RESOLVED, OPTICAL READOUT DETECTOR for PULSED, FAST-NEUTRON TRANSMISSION SPECTROSCOPY (PFNTS) MONTE-CARLO SIMULATIONS OF TIME- RESOLVED, OPTICAL READOUT DETECTOR for PULSED, FAST-NEUTRON TRANSMISSION SCTROSCOPY (PFNTS) a*, David Vartsky a, I. Mardor a, M. B. Goldberg a, D. Bar a, G. Feldman a,

More information

Scintillation efficiency measurement of Na recoils in NaI(Tl) below the DAMA/LIBRA energy threshold

Scintillation efficiency measurement of Na recoils in NaI(Tl) below the DAMA/LIBRA energy threshold Scintillation efficiency measurement of Na recoils in NaI(Tl) below the DAMA/LIBRA energy threshold Jingke Xu, Princeton (now @LLNL) Sept 24, 2015 2015 LowECal Workshop, Chicago, IL Outline 1. Overview

More information

Los Alamos National Laboratory Facility Review

Los Alamos National Laboratory Facility Review Los Alamos National Laboratory Facility Review Ron Nelson P-27 & LANSCE Neutron Data Needs & Capabilities for Applications LBNL 27 May 2015 Los Alamos Neutron Science Center User Facilities Los Alamos

More information

NEWAGE experiment. Kentaro Miuchi. (Kyoto Uni.) new generation WIMP-search with an advanced gaseous tracker experiment

NEWAGE experiment. Kentaro Miuchi. (Kyoto Uni.) new generation WIMP-search with an advanced gaseous tracker experiment NEWAGE experiment new generation WIMP-search with an advanced gaseous tracker experiment Kentaro Miuchi (Kyoto Uni.) 1. Goal and current status Goal: WIMP detection and direction measurement WIMP-anemometry

More information

Development of Scintillator Detectors at J-PARC/MLF

Development of Scintillator Detectors at J-PARC/MLF Development of Scintillator Detectors at J-PARC/MLF J-PARC, JAEA Kazuhiko Soyama Basic Energy Sciences Neutron & Photon Detector Workshop August 1-3, 2012 Holiday Inn Gaithersburg, USA Contents 1. J-PARC,

More information

Neutron Imaging at Spallation Neutron Sources

Neutron Imaging at Spallation Neutron Sources Neutron Imaging at Spallation Neutron Sources E.H. LEHMANN, A. KAESTNER Paul Scherrer Institut, Deptm. Spallation Neutron Source, Switzerland OUTLINE 1. Introduction: Motivation for Neutron Imaging 2.

More information

PHOTOELECTRON COLLECTION EFFICIENCY AT HIGH PRESSURE FOR A GAMMA DETECTOR ENVISAGING MEDICAL IMAGING

PHOTOELECTRON COLLECTION EFFICIENCY AT HIGH PRESSURE FOR A GAMMA DETECTOR ENVISAGING MEDICAL IMAGING 822 PHOTOELECTRON COLLECTION EFFICIENCY AT HIGH PRESSURE FOR A GAMMA DETECTOR ENVISAGING MEDICAL IMAGING C.D.R. Azevedo 1, C.A.B. Oliveira 1, J.M.F. dos Santos 2, J.F.C.A. Veloso 1 1.University of Aveiro,

More information

Timing and cross-talk properties of BURLE multi-channel MCP-PMTs

Timing and cross-talk properties of BURLE multi-channel MCP-PMTs Timing and cross-talk properties of BURLE multi-channel MCP-PMTs, Peter Križan, Rok Pestotnik University of Maribor, University of Ljubljana and Jožef Stefan Institute Outline of the talk: Motivation:

More information

Performance test of triple GEM detector at CERN n_tof facility

Performance test of triple GEM detector at CERN n_tof facility Performance test of triple GEM detector at CERN n_tof facility S.Puddu 2,4, G.Claps 1, G. Croci 3, F. Murtas 1,2, A.Pietropaolo 3, C. Severino 2,4, M. Silari 2 1) LNF-INFN 2) CERN 3)IFP-CNR 4)LHEP-Bern

More information

Spatial resolution measurement of Triple-GEM detector and diffraction imaging test at synchrotron radiation

Spatial resolution measurement of Triple-GEM detector and diffraction imaging test at synchrotron radiation Spatial resolution measurement of Triple-GEM detector and diffraction imaging test at synchrotron radiation Y.L. Zhang, a,b,c H.R. Qi, b,c Z.W. Wen, a,b,c H.Y. Wang, b,c,d Q. Ouyang, b,c Y.B. Chen, b,c

More information

High pressure xenon gas detector with segmented electroluminescence readout for 0nbb search

High pressure xenon gas detector with segmented electroluminescence readout for 0nbb search High pressure xenon gas detector with segmented electroluminescence readout for 0nbb search Kiseki Nakamura Kobe university for the AXEL collaboration PMT AXEL experiment High pressure xenon gas TPC for

More information

Data Acquisition. What choices need to be made?

Data Acquisition. What choices need to be made? 1 Specimen type and preparation Radiation source Wavelength Instrument geometry Detector type Instrument setup Scan parameters 2 Specimen type and preparation Slide mount Front loading cavity Back loading

More information

He-3 Neutron Detectors

He-3 Neutron Detectors Application He-3 Neutron Detectors General Considerations, Applications: He-3 filled proportional counters are standard neutron detectors and are most suitable for the detection of thermal neutrons. Larger

More information

Towards Proton Computed Tomography

Towards Proton Computed Tomography SCIPP Towards Proton Computed Tomography L. R. Johnson, B. Keeney, G. Ross, H. F.-W. Sadrozinski, A. Seiden, D.C. Williams, L. Zhang Santa Cruz Institute for Particle Physics, UC Santa Cruz, CA 95064 V.

More information

Measurements of Neutron Total and Capture Cross Sections at the TOF spectrometers of the Moscow Meson Factory

Measurements of Neutron Total and Capture Cross Sections at the TOF spectrometers of the Moscow Meson Factory Measurements of Neutron Total and Capture Cross Sections at the TOF spectrometers of the Moscow Meson Factory Yu.V. Grigoriev 1,2, D.V. Khlustin 1, Zh.V. Mezentseva 2, Yu.V. Ryabov 1 1 Institute for Nuclear

More information

Nuclear cross-section measurements at the Manuel Lujan Jr. Neutron Scattering Center. Michal Mocko

Nuclear cross-section measurements at the Manuel Lujan Jr. Neutron Scattering Center. Michal Mocko Nuclear cross-section measurements at the Manuel Lujan Jr. Neutron Scattering Center Michal Mocko G. Muhrer, F. Tovesson, J. Ullmann International Topical Meeting on Nuclear Research Applications and Utilization

More information

GEM at CERN. Leszek Ropelewski CERN PH-DT2 DT2-ST & TOTEM

GEM at CERN. Leszek Ropelewski CERN PH-DT2 DT2-ST & TOTEM GEM at CERN Leszek Ropelewski CERN PH-DT2 DT2-ST & TOTEM MicroStrip Gas Chamber Semiconductor industry technology: Photolithography Etching Coating Doping A. Oed Nucl. Instr. and Meth. A263 (1988) 351.

More information

RTPC Simulation Studies for Tagged Deep Inelastic Experiment. Rachel Montgomery SBS Collaboration Meeting, Jefferson Lab, 22/07/16

RTPC Simulation Studies for Tagged Deep Inelastic Experiment. Rachel Montgomery SBS Collaboration Meeting, Jefferson Lab, 22/07/16 RTPC Simulation Studies for Tagged Deep Inelastic Experiment Rachel Montgomery SBS Collaboration Meeting, Jefferson Lab, 22/07/16 1 Tagged DIS Measurement with RTPC and SBS Measure DIS cross section, detecting

More information

Neutron Instruments I & II. Ken Andersen ESS Instruments Division

Neutron Instruments I & II. Ken Andersen ESS Instruments Division Neutron Instruments I & II ESS Instruments Division Neutron Instruments I & II Overview of source characteristics Bragg s Law Elastic scattering: diffractometers Continuous sources Pulsed sources Inelastic

More information

MTV - S1183 Beam Time Summary. Performance test of MTV new detector : CDC. Yumi Totsuka. Department of Physics, Rikkyo University, Tokyo, Japan

MTV - S1183 Beam Time Summary. Performance test of MTV new detector : CDC. Yumi Totsuka. Department of Physics, Rikkyo University, Tokyo, Japan MTV - S1183 Beam Time Summary Performance test of MTV new detector : CDC Yumi Totsuka Department of Physics, Rikkyo University, Tokyo, Japan TRIUMF-ISAC Science Forum (30. Nov. 2011) Schedule: Beam Time

More information

5 th ASRC International Workshop, 14 th -16 th March 2012

5 th ASRC International Workshop, 14 th -16 th March 2012 Fission Fragment Fragment Spectroscopy with Large Arrays and STEFF A.G. Smith, J. Dare, A. Pollitt, E. Murray The University of Manchester W. Urban, T. Soldner ILL Grenoble I. Tsekhanovich, J. Marrantz

More information

1. MeV gamma ray Imaging & ETCC 2. Results of SMILE-I 3. Preparations of SMILE-II. A. Takada (Kyoto Univ.)

1. MeV gamma ray Imaging & ETCC 2. Results of SMILE-I 3. Preparations of SMILE-II. A. Takada (Kyoto Univ.) 1. MeV gamma ray Imaging & ETCC 2. Results of SMILE-I 3. Preparations of SMILE-II A. Takada (Kyoto Univ.) Observation of MeV gamma-ray will provide us Nucleosynthesis SNR : Radio-isotopes Galactic plane

More information

Neutron Structure Functions and a Radial Time Projection Chamber

Neutron Structure Functions and a Radial Time Projection Chamber Neutron Structure Functions and a Radial Time Projection Chamber Stephen Bültmann Old Dominion University for the BoNuS Collaboration The Structure of the Neutron The BoNuS Experiment at CLAS A New Proton

More information

Technology Comparison: brief update

Technology Comparison: brief update Technology Comparison: brief update People contributing: Ciaran, Cosmin, Kentaro, S.V. Running a bit late (Spent most of my time writing code, instead of text for paper.) Simulation framework mostly completed

More information

Prompt gamma measurements for the verification of dose deposition in proton therapy. Contents. Two Proton Beam Facilities for Therapy and Research

Prompt gamma measurements for the verification of dose deposition in proton therapy. Contents. Two Proton Beam Facilities for Therapy and Research Prompt gamma measurements for the verification of dose deposition in proton therapy Two Proton Beam Facilities for Therapy and Research Ion Beam Facilities in Korea 1. Proton therapy facility at National

More information

Initial Studies in Proton Computed Tomography

Initial Studies in Proton Computed Tomography SCIPP Initial Studies in Proton Computed Tomography L. R. Johnson, B. Keeney, G. Ross, H. F.-W. Sadrozinski, A. Seiden, D.C. Williams, L. Zhang Santa Cruz Institute for Particle Physics, UC Santa Cruz,

More information

Measurement of 39 Ar in Underground Argon for Dark Matter Experiments

Measurement of 39 Ar in Underground Argon for Dark Matter Experiments Measurement of 39 Ar in Underground Argon for Dark Matter Experiments Jingke Xu Princeton University June 7 th, 2013 1 Evidences for Dark Matter Rotation Curve Gravitational Lensing CMB Power Spectrum

More information

II. 5. Study for NaI(Tl) and Scintillation Fiber with 80 MeV Proton Beam Toward ESPRI Experiment at NIRS-HIMAC, RIKEN-RIBF

II. 5. Study for NaI(Tl) and Scintillation Fiber with 80 MeV Proton Beam Toward ESPRI Experiment at NIRS-HIMAC, RIKEN-RIBF CYRIC Annual Report 2005 II. 5. Study for NaI(Tl) and Scintillation Fiber with 80 MeV Proton Beam Toward ESPRI Experiment at NIRS-HIMAC, RIKEN-RIBF Zenihiro J. 1, Matsuda Y. 2, Sakaguchi H. 3, Takeda H.

More information

µ-pic gaseous area detector for small-angle X-ray scattering experiments

µ-pic gaseous area detector for small-angle X-ray scattering experiments Doctoral Thesis µ-pic gaseous area detector for small-angle X-ray scattering experiments Kaori Hattori Department of Physics, Graduate School of Science, Kyoto University January, 9 Abstract A detector

More information

LAB 4: Gamma-ray coincidence spectrometry (2018)

LAB 4: Gamma-ray coincidence spectrometry (2018) LAB 4: Gamma-ray coincidence spectrometry (2018) As you have seen, in several of the radioactive sources we encountered so far, they typically emit more than one gamma photon per decay or even more than

More information

GEMs and Solid State Converters

GEMs and Solid State Converters Neutron Detection with CASCADE The synthesis of GEMs and Solid State Converters Contents Conduct Construct The Helium-3 crisis 2 9/11 Costs: 2000-3000 /L If you can get it Size of the Helium-3 Stockpile,

More information

V. 3. Development of an Accelerator Beam Loss Monitor Using an Optical Fiber

V. 3. Development of an Accelerator Beam Loss Monitor Using an Optical Fiber CYRIC Annual Report 2001 V. 3. Development of an Accelerator Beam Loss Monitor Using an Optical Fiber Kawata N. Baba M. Kato M.*, Miura T.**, and Yamadera A.***, Cyclotron and Radioisotope Center, Tohoku

More information

First Results and Realization Status of a Proton Computed Radiography Device

First Results and Realization Status of a Proton Computed Radiography Device First Results and Realization Status of a Proton Computed Radiography Device V. Sipala for the PRIMA collaboration V.Sipalaa,b, D.LoPrestia,b, N.Randazzob, M.Bruzzid,e, D.Menichellie,d, C.Civininid, M.Bucciolinic,d,

More information

A new detector for neutron beam monitoring

A new detector for neutron beam monitoring A new detector for neutron beam monitoring European Organization for Nuclear Research (CERN), Geneva, Switzerland in collaboration with Commissariat à l Energie Atomique (CEA), Saclay, France, Instituto

More information

Simulation for radiography of neutron and X-ray as well as the shielding of radioactive rays

Simulation for radiography of neutron and X-ray as well as the shielding of radioactive rays Project Title: RICC Usage Report for Fiscal Year 2010 Simulation for radiography of neutron and X-ray as well as the shielding of radioactive rays Name : 王盛 (Wang Sheng) Affiliation: VCAD Modeling Team

More information

BEAM BEAM. cathode anode cathode

BEAM BEAM. cathode anode cathode High-rate axial-field ioniza2on chamber for par2cle iden2fica2on of radioac2ve beams, J. Vadas, Varinderjit Singh, G. Visser, A. Alexander, J. Huston, B.B. Wiggins, A. Chbihi, M. Famiano, M. Bischak To

More information

The accelerators at LNS - INFN and diagnostics aspects of the radioactive beams

The accelerators at LNS - INFN and diagnostics aspects of the radioactive beams The accelerators at LNS - INFN and diagnostics aspects of the radioactive beams L. Cosentino, P. Finocchiaro, A. Pappalardo LNS INFN Catania J. Harasimowicz Univ. of Liverpool Cockroft Institute LNS INFN

More information

Recent Progress on D 3 - The Directional Dark Matter Detector

Recent Progress on D 3 - The Directional Dark Matter Detector Recent Progress on D 3 - The Directional Dark Matter Detector Cosmic ray track (~7mm) detected with µd 3 prototype Motivation Detection Principle Performance of prototypes Plans for future Related activities

More information

CRaTER Pre-Ship Review (PSR) Instrument Calibration Science Requirements Compliance

CRaTER Pre-Ship Review (PSR) Instrument Calibration Science Requirements Compliance CRaTER Pre-Ship Review (PSR) Instrument Calibration Science Requirements Compliance Justin C Kasper Smithsonian Astrophysical Observatory January 3, 2008 Outline Calibration Relate the ADU of the Pulse

More information

& SUN ZhiJia 1;2. Abstract

& SUN ZhiJia 1;2. Abstract Study on the imaging ability of the 2D neutron detector based on MWPC TIAN LiChao 1;2;3*, CHEN YuanBo 1;2, TANG Bin 1;2,ZHOU JianRong 1;2,QI HuiRong 1;2, LIU RongGuang 1;2, ZHANG Jian 1;2, YANG GuiAn 1;2,

More information

High-Resolution Gamma-Ray and Neutron Detectors For Nuclear Spectroscopy

High-Resolution Gamma-Ray and Neutron Detectors For Nuclear Spectroscopy High-Resolution Gamma-Ray and Neutron Detectors For Nuclear Spectroscopy Thomas Niedermayr, I. D. Hau, S. Terracol, T. Miyazaki, S. E. Labov and S. Friedrich Former colleagues: M. F. Cunningham, J. N.

More information

Exploring the spatial resolution of positionsensitive microchannel plate detectors

Exploring the spatial resolution of positionsensitive microchannel plate detectors Exploring the spatial resolution of positionsensitive microchannel plate detectors Blake Wiggins, Davinder Siwal, Romualdo T. desouza Cold neutrons A. S. Tremsin et al, Nucl. Instr. Meth. A 652, 400 (2011).

More information

Micro Pixel Chamber with resistive electrodes for spark reduction

Micro Pixel Chamber with resistive electrodes for spark reduction Micro Pixel Chamber with resistive electrodes for spark reduction arxiv:1310.5550v1 [physics.ins-det] 21 Oct 2013 Atsuhiko Ochi a, Yuki Edo a, Yasuhiro Homma a, Hidetoshi Komai a and Takahiro Yamaguchi

More information

FARCOS Femtoscope Array for Correlations & Spectroscopy

FARCOS Femtoscope Array for Correlations & Spectroscopy FARCOS Femtoscope Array for Correlations & Spectroscopy Overview of project and physics inputs Present status (mechanics, electronics) and perspectives for the use with GET electronics G. Cardella, INFN-Catania

More information

Particle Energy Loss in Matter

Particle Energy Loss in Matter Particle Energy Loss in Matter Charged particles loose energy when passing through material via atomic excitation and ionization These are protons, pions, muons, The energy loss can be described for moderately

More information

IPRD 2016 IPRD Light Dark Matter searches at LSM, Modane and SNOLab. Ioannis KATSIOULAS CEA, Saclay / IRFU / SEDI.

IPRD 2016 IPRD Light Dark Matter searches at LSM, Modane and SNOLab. Ioannis KATSIOULAS CEA, Saclay / IRFU / SEDI. IPRD 2016 IPRD 2016 Light Dark Matter searches at LSM, Modane and SNOLab Ioannis KATSIOULAS CEA, Saclay / IRFU / SEDI ioannis.katsioulas@cea.fr New Experiments With Spheres AIM: Search for WIMPs in the

More information

Alpha-Gamma discrimination by Pulse Shape in LaBr 3 :Ce and LaCl 3 :Ce

Alpha-Gamma discrimination by Pulse Shape in LaBr 3 :Ce and LaCl 3 :Ce Alpha-Gamma discrimination by Pulse Shape in LaBr 3 :Ce and LaCl 3 :Ce F.C.L. Crespi 1,2, F.Camera 1,2, N. Blasi 2, A.Bracco 1,2, S. Brambilla 2, B. Million 2, R. Nicolini 1,2, L.Pellegri 1, S. Riboldi

More information

Neutron cross section measurement of MA

Neutron cross section measurement of MA Neutron cross section measurement of MA Hideo Harada Nuclear Science and Engineering Directorate, Japan Atomic Energy Agency 2007 Symposium on Nuclear Data Nov. 30, 2007, RICOTTI Convention Center 2007

More information

THE AMS RICH COUNTER

THE AMS RICH COUNTER THE AMS RICH COUNTER G. BOUDOUL ISN Grenoble ISN-GRENOBLE 1 The AMS RICH collaboration: Bologna, Grenoble, Lisbon, Madrid, Maryland, Mexico 2 The AMS collaboration UNAM S.C.C. TING (MIT), PI 3 AMS Scientific

More information

GEANT4 simulation of the 10 B-based Jalousie detector for neutron diffractometers

GEANT4 simulation of the 10 B-based Jalousie detector for neutron diffractometers GEANT4 simulation of the 10 B-based Jalousie detector for neutron diffractometers Irina Stefanescu 1, R. Hall-Wilton 1, G. Kemmerling 2, M. Klein 3, C.J. Schmidt 3,4, W. Schweika 1,2 1 European Spallation

More information

1.4 The Tools of the Trade!

1.4 The Tools of the Trade! 1.4 The Tools of the Trade! Two things are required for material analysis: excitation mechanism for originating characteristic signature (radiation) radiation detection and identification system (spectroscopy)

More information

Measurements of W-value, Mobility and Gas Gain in Electronegative

Measurements of W-value, Mobility and Gas Gain in Electronegative 1 2 3 4 5 6 7 8 9 Measurements of W-value, Mobility and Gas Gain in Electronegative Gaseous CS 2 and CS 2 Gas Mixtures Kirill Pushkin and Daniel Snowden-Ifft Department of Physics, Occidental College,

More information

Progress of the interaction between e - and molecule in Fudan University

Progress of the interaction between e - and molecule in Fudan University Progress of the interaction between e - and molecule in Fudan University B. Wei, Z. Chen, X. Wang, R. Hutton, Y. Zou Fudan University, Shanghai The 2nd Research Coordination Meeting (RCM) of the CRP, 23-25

More information

Particle Energy Loss in Matter

Particle Energy Loss in Matter Particle Energy Loss in Matter Charged particles, except electrons, loose energy when passing through material via atomic excitation and ionization These are protons, pions, muons, The energy loss can

More information

Xenon Compton Telescopes at Columbia: the post LXeGRIT phase. E.Aprile. Columbia University

Xenon Compton Telescopes at Columbia: the post LXeGRIT phase. E.Aprile. Columbia University Xenon Compton Telescopes at Columbia: the post LXeGRIT phase E.Aprile Columbia University Seeon 2003 Sensitivity Goals for An Advanced Compton Telescope ~10-7 ph cm -2 s -1 ( 3σ) for narrow lines and ~

More information

High Spatial Resolution in thermal Neutron Detection: from CASCADE to BASTARD. Markus Köhli. DPG Frühjahrstagung Münster

High Spatial Resolution in thermal Neutron Detection: from CASCADE to BASTARD. Markus Köhli. DPG Frühjahrstagung Münster High Spatial Resolution in thermal Neutron Detection: from CASCADE to BASTARD DPG Frühjahrstagung Münster 27.03.2017 Physikalisches Institut (LCTPC) Rheinische Friedrich-Wilhelms-Universität Bonn Markus

More information

Title Neutron Beam at J-PARC/MLF/BL09. Kino, Koichi; Yonemura, Masao; Kiya. Citation Physics Procedia (2015), 69:

Title Neutron Beam at J-PARC/MLF/BL09. Kino, Koichi; Yonemura, Masao; Kiya. Citation Physics Procedia (2015), 69: Title First Imaging Experiment of Neutron Beam at J-PARC/MLF/BL09 a Lithi Kino, Koichi; Yonemura, Masao; Kiya Author(s) Ishikawa, Yoshihisa; Parker, Joseph Kamiyama, Takashi Citation Physics Procedia (2015),

More information

An introduction to Neutron Resonance Densitometry (Short Summary)

An introduction to Neutron Resonance Densitometry (Short Summary) An introduction to Neutron Resonance Densitometry (Short Summary) H. Harada 1, M. Koizumi 1, H. Tsuchiya 1, F. Kitatani 1, M. Seya 1 B. Becker 2, J. Heyse 2, S. Kopecky 2, C. Paradela 2, P. Schillebeeckx

More information

Technical Specifications and Requirements on Direct detection for Dark Matter Searches

Technical Specifications and Requirements on Direct detection for Dark Matter Searches Technical Specifications and Requirements on Direct detection for Dark Matter Searches Jin Li THU/IHEP Symposium of the Sino-German GDT Cooperation 04/08/2013 Tübingen Outline Introduction Direct detection

More information

MS482 Materials Characterization ( 재료분석 ) Lecture Note 4: XRF

MS482 Materials Characterization ( 재료분석 ) Lecture Note 4: XRF 2016 Fall Semester MS482 Materials Characterization ( 재료분석 ) Lecture Note 4: XRF Byungha Shin Dept. of MSE, KAIST 1 Course Information Syllabus 1. Overview of various characterization techniques (1 lecture)

More information

Development of High-Z Semiconductor Detectors and Their Applications to X-ray/gamma-ray Astronomy

Development of High-Z Semiconductor Detectors and Their Applications to X-ray/gamma-ray Astronomy Development of High-Z Semiconductor Detectors and Their Applications to X-ray/gamma-ray Astronomy Taka Tanaka (SLAC/KIPAC) 9/19/2007 SLAC Advanced Instrumentation Seminar Outline Introduction CdTe Diode

More information

discovery of two-proton radioactivity future studies Bertram Blank, CEN Bordeaux-Gradignan Hirschegg, january 2008

discovery of two-proton radioactivity future studies Bertram Blank, CEN Bordeaux-Gradignan Hirschegg, january 2008 two-proton radioactivity discovery of two-proton radioactivity Experimental results with TPC future studies Bertram Blank, CEN Bordeaux-Gradignan Hirschegg, 14-18 january 2008 alpha emission of 4 He 2

More information

Status report of CPHS and neutron activities at Tsinghua University

Status report of CPHS and neutron activities at Tsinghua University IL NUOVO CIMENTO 38 C (2015) 185 DOI 10.1393/ncc/i2015-15185-y Colloquia: UCANS-V Status report of CPHS and neutron activities at Tsinghua University X. Wang( 1 )( 2 )( ),Q.Xing( 1 )( 2 ),S.Zheng( 1 )(

More information

Neutron Capture Experiments with DANCE

Neutron Capture Experiments with DANCE Neutron Capture Experiments with DANCE G. E. Mitchell North Carolina State University Raleigh, NC USA This work was supported in part by the U. S. DoE Grants No. DE-FG52-06NA26194 and DE-FG02-97-ER41042.

More information

mean free path stopping power absorption coefficient detected recoil rate detected 0νββ events

mean free path stopping power absorption coefficient detected recoil rate detected 0νββ events mean free path stopping power absorption coefficient detected recoil rate detected 0νββ events The T-REX Project: in Rare-Event searches, top0logy can be the key: merge MPGDs (Micromegas) with low-background

More information

DARWIN. Marc Schumann Physik Institut, Universität Zürich. Aspera Technology Forum 2010, October 21-22, 2010

DARWIN. Marc Schumann Physik Institut, Universität Zürich. Aspera Technology Forum 2010, October 21-22, 2010 21-22 DARWIN Marc Schumann Physik Institut, Universität Zürich Aspera Technology Forum 2010, October 21-22, 2010 www.physik.uzh.ch/groups/groupbaudis/xenon/ Dark Matter: Evidence & Detection NASA/WMAP

More information

MEASUREMENT OF TEMPORAL RESOLUTION AND DETECTION EFFICIENCY OF X-RAY STREAK CAMERA BY SINGLE PHOTON IMAGES

MEASUREMENT OF TEMPORAL RESOLUTION AND DETECTION EFFICIENCY OF X-RAY STREAK CAMERA BY SINGLE PHOTON IMAGES Proceedings of IBIC212, Tsukuba, Japan MEASUREMENT OF TEMPORAL RESOLUTION AND DETECTION EFFICIENCY OF X-RAY STREAK CAMERA BY SINGLE PHOTON IMAGES A. Mochihashi, M. Masaki, S. Takano, K. Tamura, H. Ohkuma,

More information

Electromagnetic calorimeters of the CMD-3 detector

Electromagnetic calorimeters of the CMD-3 detector Electromagnetic calorimeters of the CMD-3 detector Budker Institute of Nuclear Physics D. Epifanov Outline: VEPP-2000 and CMD-3 Barrel calorimeter ( LXe + CsI) Endcap calorimeter ( BGO ) First results

More information

arxiv: v1 [astro-ph.im] 6 Dec 2010

arxiv: v1 [astro-ph.im] 6 Dec 2010 arxiv:12.1166v1 [astro-ph.im] 6 Dec 20 MIMAC: A micro-tpc matrix for directional detection of dark matter, J. Billard, G. Bosson, O. Bourrion, C. Grignon, O. Guillaudin, F. Mayet, J.P. Richer LPSC, Universite

More information