Detector Array for Low Intensity radiation. DALI and DALI2. S.Takeuchi, T.Motobayashi. Heavy Ion Nuclear Physics Laboratory, RIKEN

Similar documents
A NEW GENERATION OF GAMMA-RAY TELESCOPE

Light ion recoil detector

A Comparison between Channel Selections in Heavy Ion Reactions

arxiv: v2 [nucl-ex] 24 Jun 2014

High-spin studies and nuclear structure in three semi-magic regions of the nuclide chart High-seniority states in Sn isotopes

Timing and Energy Response of Six Prototype Scintillators

The SpecMAT project: An array of gamma-ray detectors around an active gas target

W. Udo Schröder Departments of Chemistry & of Physics and Astronomy

Investigation of Pygmy Dipole Resonance in neutron rich exotic nuclei

SURROGATE REACTIONS. An overview of papers by Jason Burke from LLNL

Development of a 3D-Imaging Calorimeter in LaBr 3 for Gamma-Ray Space Astronomy

Dedicated Arrays: MEDEA GDR studies (E γ = MeV) Highly excited CN E*~ MeV, 4 T 8 MeV

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

Status of the TRACE array

arxiv: v1 [physics.ins-det] 16 May 2017

Sunday Monday Thursday. Friday

APPLICATION OF THE NUCLEAR REACTION ANALYSIS FOR AGING INVESTIGATIONS

Experimental Study of Stellar Reactions at CNS

Experimental Approach to Explosive Hydrogen Burning with Low-Energy RI Beams

C NS. Direct reactions of Borromean nuclei FM50. S. Shimoura CNS, University of Tokyo

(10%) (c) What other peaks can appear in the pulse-height spectrum if the detector were not small? Give a sketch and explain briefly.

Application of positrons in materials research

Design, Construction, Operation, and Simulation of a Radioactivity Assay Chamber

Nuclear Lifetimes. = (Eq. 1) (Eq. 2)

Physic 492 Lecture 16

Bremsstrahlung and Ion Beam Current Measurements with SuSI ECR Ion Source

hν' Φ e - Gamma spectroscopy - Prelab questions 1. What characteristics distinguish x-rays from gamma rays? Is either more intrinsically dangerous?

Characterization and Monte Carlo simulations for a CLYC detector

Nuclear physics activities in Vietnam (highlight from NHEP2016 conference)

Charged particle detection in GE6 To stop high energy particles need large thickness of Germanium (GE6 has ~13 cm) Charged particle detection in Ge

Measurements of liquid xenon s response to low-energy particle interactions

Detection of γ-rays from nuclear decay: 0.1 < E γ < 20 MeV

Nuclear Physics using RadioIsotope Beams. T. Kobayashi (Tohoku Univ.)

José Antonio Briz Monago, M. Carmona-Gallardo and. M.J.G. Borge, A. Perea, O. Tengblad, M. Turrión

Applied Nuclear Physics (Fall 2006) Lecture 21 (11/29/06) Detection of Nuclear Radiation: Pulse Height Spectra

Investigation of radiative proton-capture reactions using high-resolution g-ray spectroscopy

Study of multi-nucleon transfer reactions with light nuclei

Progress in measuring GMR in unstable nuclei: Decay detector calibration and inverse reaction experiment. J. Button, Y.-W. Lui, and D.H.

KEK isotope separation system for β-decay spectroscopy of r-process nuclei

Role of Hexadecupole Deformation in the Shape Evolution of Neutron-rich Nd Isotopes

Accreting Neutron Stars

Doppler Shift Attenuation Method: The experimental setup at the MLL and the lifetime measurement of the 1 st excited state in 31 S

Preparatory experiments for cold-neutron induced fission studies at IKI

Digital Gamma-ray Spectroscopy & Imaging with Semiconductor detectors Frontiers of gamma-ray spectroscopy

COMPARATIVE STUDY OF PIGE, PIXE AND NAA ANALYTICAL TECHNIQUES FOR THE DETERMINATION OF MINOR ELEMENTS IN STEELS

Study of Neutron-Proton Correlation & 3N-Force in 12 C

Low-spin structure of 210 Bi

Addendum to the ISOLDE and Neutron Time-of-Flight Committee

Large volume LaBr 3 :Ce detectors and HECTOR +

A Measurement of Monoenergetic Neutrons from 9 Be(p,n) 9 B

Radiation (Particle) Detection and Measurement

Measurement of the 14 Be(p,n) 14 B(1 + ) Reaction in Inverse Kinematics

Physics with Exotic Nuclei

Exotic Nuclei II. Neutron-rich nuclides. Michael Thoennessen FRIB/NSCL Michigan State University

Arjan Plompen. Measurements of sodium inelastic scattering and deuterium elastic scattering

7 th AGATA week

HiRA: Science and Design Considerations

The statistical properties of 92 Mo and implications for the p-process

TIGRESS Auxiliary Detectors

Development of a new MeV gamma-ray camera

Physics with Exotic Nuclei. Hans-Jürgen Wollersheim

SCI-O11. Design of a Compton Spectrometer Experiment for Studying Electron Response of a Scintillator

Disordered Materials: Glass physics

Nuclear spectroscopy using direct reactions of RI beams

Background Neutron Studies for Coherent Elastic Neutrino-Nucleus Scattering Measurements at the SNS

Positron Annihilation Spectroscopy

Desorption and Sputtering on Solid Surfaces by Low-energy Multicharged Ions

Status & Future for In-Beam Spectrometers for Tagging at JYFL

Figure 1. Decay Scheme for 60Co

JRC Place on dd Month YYYY Event Name 1

Isospin symmetry breaking in mirror nuclei. Experimental and theoretical methods

Radiation Detection for the Beta- Delayed Alpha and Gamma Decay of 20 Na. Ellen Simmons

Future gamma-ray spectroscopic experiment (J-PARC E63) on 4 ΛH

* On leave from FLNR / JINR, Dubna

Gamma-ray spectroscopy with the scintillator/photomultiplierand with the high purity Ge detector: Compton scattering, photoeffect, and pair production

Gamma-Ray coincidence and 60 Co angular correlation

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

PHYS 3650L - Modern Physics Laboratory

Fission fragment mass distributions via prompt γ -ray spectroscopy

arxiv: v1 [nucl-ex] 4 Sep 2008

Studies of Hadron Calorimeter

The Versatile Array of Neutron Detectors at Low Energy

Production and Separation of Radioactive Beams. Mg and 20 Na with MARS

Doppler Correction after Inelastic Heavy Ion Scattering 238 U Ta system at the Coulomb barrier

The Compton Effect. Martha Buckley MIT Department of Physics, Cambridge, MA (Dated: November 26, 2002)

E1 strength of the subthreshold 3/2 + state in 15 O studied by Coulomb excitation

NUCLEON TRANSFER REACTION STUDIES AT GANIL USING RADIOACTIVE NUCLEAR BEAMS

Design of a Lanthanum Bromide Detector for TOF PET

The Advanced Gamma Tracking Array detector characterisation

5 Atomic Physics. 1 of the isotope remains. 1 minute, 4. Atomic Physics. 1. Radioactivity 2. The nuclear atom

Monte Carlo Simulations for Modern gammatracking

Detekce a spektrometrie neutronů. neutron detection and spectroscopy

arxiv:physics/ v1 3 Aug 2006

Basics and Means of Positron Annihilation

Overview about the Work with Liquid Scintillators

CALIBRATION OF SCINTILLATION DETECTORS USING A DT GENERATOR Jarrod D. Edwards, Sara A. Pozzi, and John T. Mihalczo

Quasi-Free Knockout Reaction Studies at RIBF

Experimental Techniques and Methods

Particle emission at the proton drip-line

University of Groningen. Study of compression modes in 56Ni using an active target Bagchi, Soumya

Transcription:

Detector Array for Low Intensity radiation DALI and DALI2 S.Takeuchi, T.Motobayashi Heavy Ion Nuclear Physics Laboratory, RIKEN H.Murakami, K.Demichi, H.Hasegawa, Y.Togano Department of Physics, Rikkyo University

γ-ray SPECTROSCOPY WITH UNSTABLE NUCELI RIPS radioactive beam Target Liq.H 2 / Liq. 4 He / Pb / F1 D2 F2 γ-ray detection array D1 Inelastic scattering in inverse kinematics Excitation energy Transition probability Angular distribution for particle-γ

Unstable nuclei Low Beam intensity High detection efficiency Fast secondary beams RARF (β ~ 0.3) and RIBF (β ~ 0.6) Doppler Shift Depending on the emission angle High angular resolution for High energy resolution Detector θ lab Beam particle θ lab Target Scattered particle

DALI 32 Mg(p,p ) β~0.3 Previous system (typical spec.) up to 68 NaI(Tl) detectors angular resolution : ~15 degree efficiency : about 15% for 1MeV H.Hasegawa, Master s thesis, Rikkyo Univ., 2003

DEVELOPMENT of A NEW ARRAY MOTIVATION: For More neutron-rich nuclei : Low Intensity For using at RIBF : Fast beam REQUIREMENTS: Higher Efficiency Higher Angular Resolution High Energy Resolution Angular Distribution measurements 160 NaI(Tl) Detectors Large Volume and Many Segments

DOPPLER SHIFT and BROADENING E proj γ lab ( 1 cosθ ) E lab = γ β γ E E proj γ proj γ 2 lab β sinθ = 1- βcosθ lab 2 2 lab lab 2 βγ ( ) ( β cosθ ) θ + 1 β cosθ lab 2 2 β β E + E lab γ lab γ 2 Detector arrangement Beam velocity or Target thickness Intrinsic resolution Detector θ lab Beam particle θ lab Target Scattered particle

OVERVIEW - DALI2-160 NaI(Tl) detectors Each detector Array 4.5 x 8 x 16 (cm 3 ) E/E ~ 9% @ 662keV 16 layers 6~14 detectors in each layer

SPECIFICATION SAINT-GOBAIN x 80 detectors 45 x 80 x 160 (mm) About 8%@662keV ( 137 Cs) SCIONIX x 80 detectors 40 x 80 x 160 (mm) About 9%@662keV( 137 Cs)

Half of DALI2

EXPERIMENT ROOM (E6 RIPS beam-line)

DALI and DALI2 DALI DALI2 Arrangement Brick wall like Hedgehog like Size 6 x 6 x 12 (cm 3 ) 4.5 x 8 x 16 (cm 3 ) # of Detectors 68 160 Volume ~ 30 liter ~ 90 liter # of Layers 6 8 16 Angular resolution ~ 15 degree ~ 8 degree Energy resolution (β~0.3) 12% @ 1MeV 8% @ 1MeV Efficiency (β~0.3) 15% @1MeV 21% @1MeV

CIRCUIT NaI(Tl) PMT HV supply Splitter Delay & Attenuator TFA other TFA channels other CFD channels OR CFD Att. : 6-10dB or NONE FAN In/Out TFA : rise time ~ 50ns QDC : GATE Width 500ns BUSY Gate & Delay Logic Delay Dynamic range ~100kev ~5MeV signal Gate & Delay stop QDC gate start TDC

IMPROVEMENT of ENERGY RESOLUTION 12 Be(α,α ) 12 Be * DALI Eγ = 2100 kev, β ~ 0.3 DALI2 9.8% 6.6% (a) : DALI ( θ~15 ) E/E = 9.8% (FWHM) (b) : DALI2 ( θ~8 ) E/E = 6.6% (FWHM)

IMPROVEMENT of ANGULAR DISTRIBUTION 36 DALI Si(Be,Be ) 36 Si * DALI2 16 C(p,p ) 16 C * E(2+) = 1399 kev E(2+) = 1766 kev θ θ

PAST EXPERIMENTS with DALI2 12 Be(α,α ) 12 Be *, 12 Be(α,t) 13 B * (CNS, Rikkyo, RIKEN) 54 Ni, 50 Fe, 46 Cr Coulex (Rikkyo, RIKEN) 27 F(p,p ) 27 F *, 16 C(p,p ) 16 C * (ATOMKI, Tokyo, RIKEN) 4 He( 22 O, 23 F * ) (CNS, RIKEN) 26 Ne(Pb,Pb) 26 Ne * (Orsay, TIT, RIKEN) 78-82 Ge Coulex (Tokyo, RIKEN) 19 C(p,p ) 19 C * (ATOMKI, RIKEN) 22 O(d,p) 23 O (ATOMKI, RIKEN) などなど

EXAMPLES - 66 Fe(p,p ) 66 Fe * - 66 Fe * E x (2 + ) = 573 kev Beam Energy 53.07 AMeV Intensity 57 cps Time 14 hours Liq. H 2 Target 67-86mg/cm 2 E/E@573 kev 10% Yield 250 counts たぶん きっと 64 Fe

Efficiency and Resolution GEANT3 simulation with target chamber and holder β = 0.3(RARF), 0.6(RIBF) Eγ = 0.5, 1.0, 2.0 MeV 0.5 MeV 1.0 MeV 2.0 MeV Eff. (β=0.3) 34% 21% 12% Res. (β=0.3) 11.6% 8.0% 6.5% Eff. (β=0.6) 31% 18% 8% Res. (β=0.6) 14.8% 12.3% 9.8%

SUMMARY We have developed DALI2 for in-beam γ-ray spectroscopy with fast unstable nuclei (@RIBF). The performance is improved compared with DALI. Energy Resolution E/E ~ 8%@1MeV Detection Efficiency ε ~ 21%@1MeV Several experiments have already done with DALI2 and we are planning experiments with low intensity beam and/or measuring γ-γ coincidence.

COMING EXPERIMENTS with DALI2 Inelastic scattering of 64 Cr (running) γ-γ coincidence of 32 Mg and 34 Si Inelastic scattering of 42 Si With Liquid hydrogen and/or helium targets FUTURE EXPERIMENTS in RIBF Efficiency and Energy resolution : 18% and 12% for 1MeV (β~0.6) Target : More neutron-rich nuclei ( ex. 78 Ni >0.1 cps ) Possible array for higher efficiency and energy resolution is the combination of DALI and DALI2. 1+2=3 DALI3?