The 2-Body Photodisintegration Reaction 4He(g,n)3He below 30 MeV

Slides:



Advertisements
Similar presentations
Compton integrating method Beam test summary PREX/Happex Collaboration Meeting Alexandre Camsonne.
Advertisements

Recent Results from the Collaboration E. J. Downie DNP Meeting October 2009.
Dante Nakazawa with Prof. Juan Collar
TOF spectrometers for measurement of n d /n t ratios K.Okada, T.Nishitani 2, K. Ochiai 2, K.Kondo 2, M.Sasao, M. Okamoto, K.Shinto, S.Kitajima Tohoku Univ.
Expected counting rates. FRS experimental setup Total load is limited by SC1 and MUSIC1.
EAR2 simulation update Collaboration board meeting Christina Weiss & Vasilis Vlachoudis.
Gamma-Ray Spectra _ + The photomultiplier records the (UV) light emitted during electronic recombination in the scintillator. Therefore, the spectrum collected.
HIGS Frozen Spin Target System (HIFROST) Pil-Neyo Seo University of Virginia Triangle Universities Nuclear Laboratory (TUNL) PSTP International Workshop,
SLEGS Proto type on SINAP LINAC Jin-Gen Chen & SLEGS Collaboration.
Beam Based Alignment of High Intensity Gamma Source (HIGS) Targets at Duke University Free Electron Laser Laboratory (DFELL) M. Emamian, Changchun Sun,
Bruce Faddegon, UCSF Inder Daftari, UCSF Joseph Perl, SLAC
Neutron Generation and Detection Lee Robertson Instrument & Source Division Oak Ridge National Laboratory 17 th National School on Neutron and X-ray Scattering.
Institute for Safety Research Dávid Légrády IP-EUROTRANS ITC2 Development of a Neutron Time-of-Flight Source at the ELBE Accelerator ELBE Neutron source.
A scintillation detector for neutrons below 1 MeV with gamma-ray rejection Scintillators are 3 mm BC408, 10 layers total Adjacent layers are optically.
Analysis of PSI beam test R.Sawada 09/Feb/2004 MEG collaboration R.Sawada 09/Feb/2004 MEG collaboration
Calibrated Parameters for Online Analysis using the Spectrodaq/SpecTCL data acquisition system at TUNL J.H. Kelley 1, B. Fallin 2, A. Hutcheson 2, A.P.
Measurement of Gas Bremsstrahlung at the Pohang Light Source Hyosang Lee Seoul National University, Q2C Pusan National University, HANUL HNP2011.
Compton/Linac based Polarized Positrons Source V. Yakimenko BNL IWLC2010, Geneva, October 18-22, 2010.
5th July 00PSI SEU Studies1 Preliminary PSI SEU Studies Study SEU effects by measuring the BER of the link in  /p beams at PSI. Measure the SEU rate as.
NNSA Synergistic Activities at TUNL The Triangle Universities Nuclear Lab is developing excellent facilities for studying (n, xn  ) reactions. Resources.
Possible calibration methods for the final LXe calorimeter A. Papa 01/20/2004.
J.T. White Texas A&M University SIGN (Scintillation and Ionization in Gaseous Neon) A High-Pressure, Room- Temperature, Gaseous-Neon-Based Underground.
Lead Fluoride Calorimeter for Deeply Virtual Compton Scattering in Hall A Alexandre Camsonne Hall A Jefferson Laboratory October 31 st 2008.
Production & Measurement of Thermal Neutron at RCNP Chhom Sakborey Nguyen Thi Duyen An Tran Hoai Nam Li Chunjuan Wang Mian.
MEG Run 2008 液体キセノンガンマ線検出器 東京大学 素粒子物理国際研究セン ター 西村 康宏、 他 MEG コラボレー ション 2008 年秋季物理学会@山形大学小白川キャンパス.
Experimental Nuclear Physics Some Recent Activities 1.Development of a detector for low-energy neutrons a. Hardware -- A Novel Design Idea b. Measure the.
DEAR SDD --> SIDDHARTA
1 NaI calibrationneutron observation NaI calibration and neutron observation during the charge exchange experiment 1.Improving the NaI energy resolution.
Possible calibration methods for the final LXe calorimeter A. Papa 02/11/
FIT (Fast Interaction Trigger) detector development for ALICE experiment at LHC (CREN) Institute for Nuclear Research (INR RAS) National Research Nuclear.
Compton Scattering from Deuterium above the Pion Production Threshold Collaboration  Duke University Luke Myers  Luke Myers  Seth Henshaw.
Background Subtraction in Next Generation 0  Experiments Double-Beta Decay Challenges in 0  Decay Detection Benjamin Spaun Whitworth College Advisors:
ObservedChannel181Hf180Hf(n,γ)181Hf180mHf180Hf(n,n')180mHf179m2Hf180Hf(n,2n)179m2Hf179Hf(n,n')179m2Hf175Hf176Hf(n,2n)175Hf173Hf174Hf(n,2n)173Hf The Astrophysical.
48 Ti(n, xnyp  ) reaction cross sections using spallation neutrons for E n = 1 to 20 MeV Excitation functions have been measured for the interaction of.
CNS CVD Diamond S. Michimasa. Properties of diamond Extreme mechanical hardness and extreme high thermal conductivity Broad optical transparency in region.
Prototypes photon veto detectors for NA62 experiment CERN M. Raggi - INFN/Frascati for the NA62 Photon Veto Working Group LNF, RM1, NA, PI, SOFIA First.
g beam test of the Liquid Xe calorimeter for the MEG experiment
Prospect of SiPM application to TOF in PANDA
Monte Carlo simulation of active neutron interrogation system developed for detection of illicit materials А.Sh. Georgadze Kiev Institute for Nuclear Research.
On behalf of TEXONO collaboration
Positron production rate vs incident electron beam energy for a tungsten target
“Performance test of a lead glass
Chapter 5 Interactions of Ionizing Radiation
In collaboration with Winthrop Brown, T.Y. Fan, Franz Kaertner,
MoNA detector physics How to detect neutrons. Thomas Baumann NSCL.
Dr. Mikhail Runtso, Mr. Pavel Naumov,
The Electromagnetic calorimeter of the MEG Experiment
Liquid Xenon Detector for the MEG Experiment
DSSSD for b decay investigations of heavy neutron-rich isotopes
Triangle Universities Nuclear Laboratory
Conceptual design of TOF and beam test results
Compton effect and ThomX What possible future?
Polarized Internal Gas Target in a Strong Toroidal Magnetic Field
Basic Physics Processes in a Sodium Iodide (NaI) Calorimeter
Presented at 2016 IEEE Nuclear Science Symposium - N28-32
AGATA week Uppsala, July 2008
Measurement of the 187Re(n,2n)186mRe Destruction Cross Section
A Precision Measurement of GEp/GMp with BLAST
(g,z) Breakup Experiments Charged Particles in the Final State
Measurement of the 187Re(n,2n)186mRe Destruction Cross Section
The Astrophysical 187Re/187Os Ratio: First Direct Measurement of the 187Re(n, 2nγ)186mRe Cross Section J. H. Kelley, NC State U. and Triangle Universities.
MEG実験の液体Xe検出器について 東大 ICEPP  森研究室 M1 金子大輔.
Diagnosis of a High Harmonic Beam Using
Rare Isotope Spectroscopic INvestigation at GSI
Pakistan Institute of Engineering and Applied Sciences (PIEAS)
Triangle Universities Nuclear Laboratory
Chapter 5 - Interactions of Ionizing Radiation
Neutron Ball Background Testing
Rare Isotope Spectroscopic INvestigation at GSI
Rare Isotope Spectroscopic INvestigation at GSI
Presentation transcript:

The 2-Body Photodisintegration Reaction 4He(g,n)3He below 30 MeV John Kelley, R. Raut, G. Rusev, S.C. Stave, A.P. Tonchev,  W. Tornow Triangle Universities Nuclear Laboratory North Carolina State University Duke University

“Equality” vs Inequality of 4He(g,n/p)3He/3H s What are the Implications? Charge Symmetry Isospin Mixing

Present State

4He(g,3He)n below 30 MeV at the High Intensity g-ray Source (HIGS) Compton backscatter FEL photons from electrons in a storage ring FEL.

Photon Flux from Plastic Scintillator Paddle Efficiency measured by comparison with NaI Pb 10” x 12” NaI detector Well understood efficiency g-ray beam Plastic scintillator paddle / PMT Pb 10 mm Collimator

Experimental Setup PMT 3He-Xe gas Pb scintillator Plastic g-ray beam Plastic Scintillator paddle/PMT Pb 10 mm Collimator

Active 4He/Xe 5 cm diameter scintillation cell Eg (MeV) Pressure PSI. Xe/He E3He 3He range mm 27 (710 4He/40 Xe) 0.056 1.6 0.8 27.5 750 1.73 0.9 28 1.85 1.0 max 50 mm diameter

4He/Xe scintillation cell vs Xe scintillation cell “target out”

Photon-induced reaction thresholds (in MeV) Isotope Nat. Abundance (%) (g,p) (g,a) (g,n) (g,2n) (g,na) xenon isotopes 128 1.92 8.17 1.77 9.61 16.84 11.19 131 21.18 8.82 2.55 6.61 15.87 8.85 136 8.87 9.93 3.66 7.99 14.44 11.73 magnesium isotopes 24 78.99 11.69 9.31 16.53 26 11.01 14.15 10.61 11.09 oxygen isotopes 16 99.762 12.13 7.16 15.67 18 0.200 15.94 6.23 8.05 He isotopes 4 99.762 19.81 - 20.58 Atomic effects “charged” kinetic energy Edge effects ignored Lt 1 MeV 1-3 MeV (1.6) 5-10 MeV 10-20 MeV Eg=27 MeV 4He+g -> 3He(1.6 MeV) & n (4.8 MeV)

High Rate/ High Threshold Anti-Pileup Circuit High Threshold – minimize multi-pulse pileup in the CFD Linear Gate Dt~100 ns – (with inhibit Dt~10 us) minimize pileup in Spectroscopic Amplifier Scaler PULSER FIFO AMP AMP FIFO FIFO Linear Gate AMP inhibit 3He Cell CFD Scaler GDG Busy Inhibit Paddle AMP Logic Scaler Computer Busy

Results Proof of principle Beamtime expected in the next quarter