02.07.2010 Alexey Kuryakin, RFNC-VNIIEF, Sarov, Russia, 1 Abstract NEUTRON SPECTROMETER BASED ON PROPORTIONAL RECOIL PROTONS COUNTER.

Slides:



Advertisements
Similar presentations
Poster Design & Printing by Genigraphics ® In the PANDA experiment, the Straw Tube Tracker (Fig. 1) designed for momentum analysis of charged.
Advertisements

Measurements of Angular and Energy Distributions of Prompt Neutron Emission from Thermal Induced Fission Vorobyev A.S., Shcherbakov O.A., Gagarski A.M.,
Combined evaluation of PFNS for 235 U(n th,f), 239 Pu(n th,f), 233 U(n th,f) and 252 Cf(sf) (in progress) V.G. Pronyaev Institute of Physics.
Dante Nakazawa with Prof. Juan Collar
INSTITUT MAX VON LAUE - PAUL LANGEVIN Fast Real-time SANS Detectors Charge Division in Individual, 1-D Position- sensitive Gas Detectors Patrick Van Esch.
PIGE experience in IPPE Institute of Physics and Power Engineering, Obninsk, Russia A.F. Gurbich.
*Shuji Maeo 1,2, Takayuki Yanagida 1, Yuui Yokota 1 and Akira Yoshikawa 1,3 1 Division of Physical Process Design, Institute of Multidisciplinary Research.
Y. Karadzhov MICE Video Conference Thu April 9 Slide 1 Absolute Time Calibration Method General description of the TOF DAQ setup For the TOF Data Acquisition.
Beam Loss Analysis Tool for the CTF3 PETS Tank M. Velasco, T. Lefevre, R. Scheidegger, M. Wood, J. Hebden, G. Simpson Northwestern University, Evanston,
Design and test of a high-speed beam monitor for hardon therapy H. Pernegger on behalf of Erich Griesmayer Fachhochschule Wr. Neustadt/Fotec Austria (H.
October-November 2003China - ALICE meeting1 PHOS in ALICE A PHOton Spectrometer with unique capabilities for the detection/identification of photons and.
Principle of operation and limits of application
1 Microstrip PSD detectors C. Fermon, V. Wintenberger, G. Francinet, F. Ott, Laboratoire Léon Brillouin CEA/CNRS Saclay.
Institute of Isotopes Hungarian Academy of Sciences Nuclear electronics for NCC measurements and training J. Bagi, J. Huszti, K. Szirmai Department of.
Status of DRIFT II Ed Daw representing the DRIFT collaboration: Univ. of Sheffield, Univ. of Edinburgh, Occidental College, Univ. of New Mexico Overview.

Energetic particle environment as seen by SphinX P. Podgorski 1, O. V. Dudnik 2, S. Gburek 1, M. Kowalinski 1, J. Sylwester 1, M. Siarkowski 1, S. Plocieniak.
NEW COMMENTS TO ILC BEAM ENERGY MEASUREMENTS BASED ON SYNCHROTRON RADIATION FROM MAGNETIC SPECTROMETER E.Syresin, B. Zalikhanov-DLNP, JINR R. Makarov-MSU.
14/02/2007 Paolo Walter Cattaneo 1 1.Trigger analysis 2.Muon rate 3.Q distribution 4.Baseline 5.Pulse shape 6.Z measurement 7.Att measurement OUTLINE.
Experimental set-up Abstract Modeling of processes in the MCP PMT Timing and Cross-Talk Properties of BURLE Multi-Channel MCP PMTs S.Korpar a,b, R.Dolenec.
ArgonneBeamTest_ ppt1 Argonne Beam Test preparation Tsunefumi Mizuno Tuneyoshi Kamae
Possibilities of TOF measurements on NPI neutron generators Mitja Majerle Department of Nuclear Reactions Nuclear Physics Institute ASCR.
FLC Group Test-beam Studies of the Laser-Wire Detector 13 September 2006 Maximilian Micheler Supervisor: Freddy Poirier.
Energy Distribution of Cosmic Ray Muons Paul Hinrichs With David Lee Advised by Phil Dudero.
Applications of Micro-TPC to Dark Matter Search 1. WIMP signatures 2. Performance of the Micro-TPC 3. WIMP-wind measurement 4. Future works 5. Conclusions.
Neutron scattering systems for calibration of dark matter search and low-energy neutrino detectors A.Bondar, A.Buzulutskov, A.Burdakov, E.Grishnjaev, A.Dolgov,
NanoPHYS’12 – December 17-19, 2012 K. Nakano, S. Miyasaka, K. Nagai and S. Obata (Department of Physics, Tokyo Institute of Technology) Drift Chambers.
Digital analysis of scintillator pulses generated by high-energy neutrons. Jan Novák, Mitja Majerle, Pavel Bém, Z. Matěj 1, František Cvachovec 2, 1 Faculty.
M. Manolopoulou 1, M. Fragopoulou 1, S. Stoulos 1, E. Vagena 1, W. Westmeier 2, M. Zamani 1 1 School of Physics, Aristotle University of Thessaloniki,
Performance limits of a 55  m pixel CdTe detector G.Pellegrini, M. Lozano, R. Martinez, M. Ullan Centro Nacional de Microelectronica, Barcelona, 08193,
Experimental set-up for on the bench tests Abstract Modeling of processes in the MCP PMT Timing and Cross-Talk Properties of BURLE/Photonis Multi-Channel.
2. RUTHERFORD BACKSCATTERING SPECTROMETRY Basic Principles.
Development of X-ray Spectrometry for Nuclear Decay Data Applications at IFIN-HH Aurelian Luca Horia Hulubei National Institute of Physics and Nuclear.
Dec.11, 2008 ECL parallel session, Super B1 Results of the run with the new electronics A.Kuzmin, Yu.Usov, V.Shebalin, B.Shwartz 1.New electronics configuration.
BigCal Reconstruction and Elastic Event Selection for GEp-III Andrew Puckett, MIT on behalf of the GEp-III Collaboration.
Development of the Readout ASIC for Muon Chambers E. Atkin, I. Bulbalkov, A. Voronin, V. Ivanov, P. Ivanov, E. Malankin, D. Normanov, V. Samsonov, V. Shumikhin,
Valerio Re, Massimo Manghisoni Università di Bergamo and INFN, Pavia, Italy Jim Hoff, Abderrezak Mekkaoui, Raymond Yarema Fermi National Accelerator Laboratory.
STATUS OF PREPARATION OF dp-ELASTIC SCATTERING STUDY AT THE EXTRACTED BEAM OF NUCLOTRON. Yu.V.Gurchin LHE JINR September 2009.
FIT (Fast Interaction Trigger) detector development for ALICE experiment at LHC (CREN) Institute for Nuclear Research (INR RAS) National Research Nuclear.
Study of high energy cosmic rays by different components of back scattered radiation generated in the lunar regolith N. N. Kalmykov 1, A. A. Konstantinov.
A. Zelenski a, G. Atoian a *, A. Bogdanov b, D.Raparia a, M.Runtso b, D. Steski a, V. Zajic a a Brookhaven National Laboratory, Upton, NY, 11973, USA b.
NASA 2001 Mars Odyssey page 1 Workshop HEND Russian Aviation and Space Agency Institute for Space Research Present knowledge of HEND efficiency.
Electron tracking Compton camera NASA/WMAP Science Team  -PIC We report on an improvement on data acquisition for a Time Projection Chamber (TPC) based.
2001 Mars Odyssey page 1 W o r k s h o p H E N D Institute for Space Research, June , 2003 HEND physical calibrations: status report A. Kozyrev,
Proportional chambers with cathode readout in high particle flux environment Michał Dziewiecki.
Click to edit Master subtitle style Presented By Mythreyi Nethi HINP16C.
1. What is an NMR Spectrum ? 2. What are the Spectral Features? 3. What are the Spectral Parameters? 4. How much should be known about the NMR Phenomena.
1 Chapter No. 17 Radiation Detection and Measurements, Glenn T. Knoll, Third edition (2000), John Willey. Measurement of Timing Properties.
Second Workshop on large TPC for low energy rare event detection, Paris, December 21 st, 2004.
Radioanalytical practical at the Department of Neutron Activation Analysis FLNP JINR, Dubna Supervisors S.S. Pavlov and M.V. Frontasyeva Summer School.
Multi-Purpose Fast Neutron Spectrum Analyzer with Real-Time Signal Processing Yu.S. Sulyaev 1, E.A. Puryga 1,2, A.D. Khilchenko 1,2, A.N. Kvashnin 1, S.V.
 A) Pulse Height Spectroscopy  Identify the equipment such as detector, electronics modules and NIM.
Recent development of gaseous position-sensitive thermal neutron detectors for the IBR-2 spectrometers A.V.Belushkin, A.A.Bogdzel, A.N.Chernikov, A.V.Churakov,
V.Aulchenko 1,2, L.Shekhtman 1,2, B.Tolochko 3,2, V.Zhulanov 1,2 Budker Institute of Nuclear Physics, , Novosibirsk, Russia Novosibirsk State University,
1 Alushta 2016 CROSS SECTION OF THE 66 Zn(n,α) 63 Ni REACTION at CROSS SECTION OF THE 66 Zn(n, α) 63 Ni REACTION at E n = 4.0, 5.0 and 6.0 MeV I. Chuprakov,
3/06/06 CALOR 06Alexandre Zabi - Imperial College1 CMS ECAL Performance: Test Beam Results Alexandre Zabi on behalf of the CMS ECAL Group CMS ECAL.
NEM433 Radiation Detection and Measurement Laboratory Fall 2013 Osman Şahin ÇELİKTEN.
GEM gas detectors for Soft X-ray imaging in Fusion devices with neutron-gamma background and polycapillary lenses F. Murtas 2, S. Dabagov 2,4, L. Gabellieri.
 13 Readout Electronics A First Look 28-Jan-2004.
Akhmatov Z.A1, Khokonov A.Kh1,2, Masaev M.B1, Romanenko V.S1.
Gamma Ray Spectrometry System Design for ITER Plasma Diagnostics
MoNA detector physics How to detect neutrons. Thomas Baumann NSCL.
A First Look J. Pilcher 12-Mar-2004
Status of n-XYTER read-out chain at GSI
1. Introduction Secondary Heavy charged particle (fragment) production
High Rate Photon Irradiation Test with an 8-Plane TRT Sector Prototype
Neutron Beam Test for Measuring Quenching Factor of CsI(Tl) Crystal
Segmented high resolution fast neutron spectrometer:
HE instrument and in-orbit performance
Gain measurements of Chromium GEM foils
Presentation transcript:

Alexey Kuryakin, RFNC-VNIIEF, Sarov, Russia, 1 Abstract NEUTRON SPECTROMETER BASED ON PROPORTIONAL RECOIL PROTONS COUNTER WITH POSSIBILITY OF γ-BACKGROUND DISCRIMINATION Y. I. Vinogradov, A.M. Shvetsov, O. P. Vikhlyantsev, A.V. Kuryakin Russian Federal Nuclear Center, All-Russian Research Institute of Experimental Physics, Sarov, Russia, The neutron spectrometer with proportional recoil protons counter was developed in VNIIEF and used for a number of years [1, 2]. The bottom range of measurements of the spectrometer in mixed n-γ fields has been limited by energy 0.5 MeV The carried out researches [3] have shown possibility of discrimination of impulses of the counter from neutrons and γ -quanta by their shape and expansions of a range of measurement of neutron spectra in the field of low energies to tens keV. Then it has been developed hardware and the spectrometer software, allowing to register amplitude of an impulse of the proportional counter and a maximum growth rate of an impulse on forward front and to write down them in ListMode (a mode of consecutive record of parametres of impulses). The program part includes a number of the service possibilities allowing to adjust registration equipment during measurements (in on-line mode), to estimate visually the quality of discrimination of impulses from neutrons and γ ‑ quanta and to receive hardware spectra. The complex of the programs is used for off-line mode analysis of the received data, which provides processing of the list of the received data with discrimination of impulses, caused by neutrons and γ ‑ quanta, construction of corresponding hardware spectra, calculation of response matrix of the proportional gas counter and reconstruction of spectra. Research of possibilities of the spectrometer with n-g discrimination, spent on 252 Cf source, has shown that the bottom range of measurements of neutron spectra decreases till keV. Reference list: 1.Kuvshinov M. I., Shvetsov A. M., Egorov V. P. et al. Measurement of neutron spectra for spherical critical assemblies of 235 U(90 %), 235 U(36 %), and 239 Pu(98 %) // Proceedings International Conference on the Physics of Reactors PHYSOR96, Mito, Ibaraki, Japan, September 16–20, 1996 / Japan Atomic Energy Research Institute Inc., Japan Vol. 2. P.338 ‑ Shvetsov A. M., Egorov V. P., Fomushkin E. F. et al. Measurements of leakage neutrons spectra for spherical assemblies of 235 U(90 %), 235 U(36 %), and 239 Pu(98 %) // Proceedings International Conference on Nuclear Data for Science and Technology, Trieste, Italy, May 18–23, 1997 / Italian Phis. Soc. Inc., Bologna, Italy Part 2. P.1359– A. M. Shvetsov, Yu. I. Vinogradov, O. P. Vikhlyantsev, A. V. Kuryakin. Investigation of the possibility of γ-background discrimination in a neutron spectrometer with a proportional counter of recoil protons. // Bulletin of the Russian Academy of Sciences: Physics, 2007, т.71, № 12, с

Alexey Kuryakin, RFNC-VNIIEF, Sarov, Russia, 2 Neutron detector Designed and used in VNIIEF for number of years Proportional gas counter, ~14% efficiency, ΔE/E~3.7% Range: 0.5÷8 MeV without, or 0.05÷8 MeV with n-γ discrimination ~ 3 kV voltage, 3 bar methane (CH 4 + some 3 He uses for calibration) CAMAC based data acquisition, n spectra reconstruction software Construction of proportional counter: 1 – glass isolation; 2 - cathode, Ø 75 mm × 1 m; 3 – anode, Ø40 µm; 4 – guard pipes; 5 – spring for anode; 6 - flanges, 7 – fluoroplastic gaskets; 8 – details from kovar (Fe+Co+Ni alloy)

Alexey Kuryakin, RFNC-VNIIEF, Sarov, Russia, 3 Principle of energy calibration Gas counter contains some 3 He for calibration Use 3 He(n,p)T reaction with peak E=0.764 MeV Thermal peak Channel, k N,Counts k0k0ΔkΔk

Alexey Kuryakin, RFNC-VNIIEF, Sarov, Russia, 4 Why need n-γ discrimination γ influent to low range spectra (E < 0.5 MeV) γ influence is difficult to calculate theoretically Low energy range limited to 0.5 MeV due to n+γ Some kind of n-γ discrimination required for E < 0.5 MeV n+γ n (clean) neutron counter spectra E,MeV N,counts

Alexey Kuryakin, RFNC-VNIIEF, Sarov, Russia, 5 Principle of n-γ discrimination Neutrons produce recoil protons γ–quanta produce electrons Hardware p, e pulses have different shapes (front timing) t front, (dE/dt) max /E max criteria can be used for n-γ separation E max (dE/dt) max time Hardware pulse from counter channel Typical hardware signal from gas detector t front Typical shape of pulse front registered with TDS-3000, 50 MHz

Alexey Kuryakin, RFNC-VNIIEF, Sarov, Russia, 6 n-γ discrimination criteria Preliminary study show that: t front criteria is not good for n-γ (dE/dt) max /E max criteria is good γ-quantum neutrons N,counts

Alexey Kuryakin, RFNC-VNIIEF, Sarov, Russia, 7 n-γ discrimination efficiency and range Fit [E,E+ Δ E] slice spectra with 2 log-normal distributions Find S γ, S n and cross (mutual overlap) ΔS areas Criteria for n-γ low range is Δ S/S n ·100% < 5% This range depends on N γ /N n [70÷80] keV slice spectra Low energy n-γ range (by 5% level) depends on N γ /N n ratio. N γ /N n = 2.5 N γ /N n = 0.7 N γ /N n = 0.3 N γ /N n = 0.2

Alexey Kuryakin, RFNC-VNIIEF, Sarov, Russia, 8 Low energy n-γ range vs N γ /N n E n-γ(0.05),MeV Low energy n-γ range (by 5% level) depends on N γ /N n ratio.

Alexey Kuryakin, RFNC-VNIIEF, Sarov, Russia, 9 n-γ discrimination tests n-γ discrimination tested with mixed n-γ and clear γ sources Low energy range without n-γ discrimination ~ 0.5 MeV Low energy range with n-γ discrimination ~ 60÷80 keV (depend on N γ /N n ) γ-quantum neutrons γ-quantum (dE/dt) max /E max, µs -1 E,MeV n+γ – source ( 252 Cf)γ – source ( СОСГИ-М )

Alexey Kuryakin, RFNC-VNIIEF, Sarov, Russia, 10 n-γ discrimination hardware CAMAC based data acquisition system designed HV – high voltage unit (Canberra 3106D), PA – charge sensitive 10 ns preamplifier (POLON 1105A), SA – spectrometry 2 µs amplifier (Canberra 2025), DU – discriminator unit (Canberra 2035A), SD – logic shaper and delay (Canberra 2055), FA – fast amplifier (Canberra 2111), ST – stretcher (ORTEC 242), ADC – 13 bit analog to digital converter (ORTEC AD 413A), C1,C2 – counter (POLON 420A), OR – output register (POLON OR350), CC – CAMAC controller (PKK4, VNIIEF designed), PC – personal computer for data acquisition with CRW-DAQ control software by VNIIEF.

Alexey Kuryakin, RFNC-VNIIEF, Sarov, Russia, 11 Online software (data acquisition) CRW-DAQ package designed in VNIIEF, Sarov Registered in Russian Federation registry  Data acquisition in List mode, 2-parameter events CAMAC based data acquisition, up to 60 kHz rate γ n (dE/dX) max E max

Alexey Kuryakin, RFNC-VNIIEF, Sarov, Russia, 12 Offline software Preliminary spectrum processing –Energy calibration by 3 He(n,p)T reaction –n-γ discrimination, background subtraction Response matrix calculation (SUPREMAC) –Uses NDX, ENDF/B-VI nuclear constants database –Uses Monte-Carlo for response matrix calculation –Optimized for performance Neutron spectrum reconstruction (UFONIM) –Ill-posed problem ( Fredholm equations of 1 st kind ) –Uses iteration method by Tarasko –Randomization method to calculate stat. errors Designed in VNIIEF G - response matrix, U – n-spectrum to find, S – hardware spectrum.