Development of an active scintillating target for fission studies. J. Aupiais, G. Bélier CEA, DAM, DIF, F Arpajon France
|
|
- Juniper Adams
- 5 years ago
- Views:
Transcription
1 Development of an active scintillating target for fission studies J. Aupiais, G. Bélier CEA, DAM, DIF, F Arpajon France 1
2 Motivations Fast neutron induced reactions are important for future nuclear plant generations, since most of the retained solutions are fast reactors. In this context fast neutron induced fission is of prime importance and one is faced to the lack of data together with incomplete understanding of the process. 2
3 Need for a new (n,2n) reaction on 239 Pu 0,8 0,7 J.fréhaut 1985 J.A.Becker 2002 ENDFBVII.0 Cross section (barns) 0,6 0,5 0,4 0,3 0,2 Passive target Fission to be subtracted High uncertainties Indirect measurement (n, xnγ) with GEANIE/WNR Model dependent 0, Neutron energy (MeV) 3
4 Count rates Need for a very efficient fission veto 4
5 The neutron long counter CARMEN BC521 : Gd loaded (0.5%) scintillator ~1 m 3 Beam Detection efficiency : 85% for 252 Cf SF neutrons target Prompt peak γ,n trigger Capture time (µs) Capture time probability distribution ΣE γ Counting gate 50 µs Stockastic captures P ν Log(E) 5
6 Advantages «Ease» of fabrication. High mass concentrations moderated volumes. Pulse shape discrimination. No specific electronic noise associated with high masses. Good time resolution. 6
7 Fission veto 7
8 α detection efficiency Isotope dissolved in active volume high efficiencies Losses due to wall effects. borosilicate 5 MeV α range ~ 50 µm Scintillator Simulations 0.34 % (energy loss 300 kev) Measurement 0.320±0.058% W.J.Dowell NAS-NS
9 The fission case Two cumulative effects : Shorter ranges 2 Fragments geometric effet Losses estimated to 10-6 Light fragment range ~ 30 µm Heavy fragment range ~ 20 µm 9
10 Principle Photo detector liquid scintillator + actinide Scintillator : Toluene C 7 H mol/l (solvent). Naphthalene C 10 H mol/l. Scintillator PBBO C 25 H 17 NO 10-2 mol/l. Extractant HDEHP C 16 H 35 O 4 P 0.2 mol/l. For physicists : C 0.47 H 0.52 O P N
11 Minimization of quenching Procedure: Solution of An (up to 10 mg) 0.1 M HNO 3 Add hydroxylamine chlorhydrate 10-2 M (for elimination of NO 2 ) Add 1.2 ml Alphaex Shaking 5 min Centrifugation 2000 rpm 5 min Sampling 1 ml Alphaex Counting 11
12 Commercially available : Ordela 8100AB NIM-3w PERALS PhotoElectron-Rejecting Alpha Liquid-Scintillation Pyrex tube 12
13 Pulse shapre discrimination principle (PSD) β signal α signal Pulse duration particule identification Response to fission unknown 13
14 First test with 252 Cf α from 252 Cf Number of counts spontaneous fission β Channel number 14
15 Bi-dimensional spectrum 15
16 Homemade system Culture tube PM : burle
17 Optimization of PSD threshold 3000 α from 252 Cf α Number of counts spontaneous fission β Number of counts β Channel number spontaneous fission Channel number 17
18 Bi-dimensional spectrum 18
19 Energy non linearity α peak 6,118 MeV TKE=188 MeV 78 MeV ~30 MeV expected!!!! β suppressed spectra 19
20 Light absorption against actinide mass 20
21 Natural uranium α spectra with the PERALS system Scintillator volume 1 cm 3 Energy Resolution ~200 kev 238 U 4198 kev 234 U 4774 kev 574 kev 21
22 Tests with natural uranium nat U1 mg/cm 3 nat U 10 mg/cm 3 Natural uranium 10 µg/cm 3 ; 1 mg/cm 3 ; 10 mg/cm Bq de 252 Cf 22
23 Tests with thorium : representative of every actinide 232 Th 10 µg/cm Th 10 mg/cm 3 Natural thorium (&& Pu) 10 µg/cm 3 ; 1 mg/cm 3 ; 10 mg/cm Bq de 252 Cf 23
24 Dedicated cell + avalanche photodiode Avalanche photodiode Scintillator cell Compacity Active target Better energy resolution -A. Reboli & J. Aupiais NIMA550(2005)593 24
25 Open questions on the maximum attainable mass 1. Radiolyse aging for high specific activities isotope dependent 2. Quenching from chemical specific to each isotope 3. Pile-up. 25
26 Perspectives Fission studies : calorimetry, γ spectra, cross sections, P ν 1. Spontaneous fission Bruyères le Châtel 2. Neutron induced fission -- NFS 2012 Ultra-asymmetric fission : cluster disintegration 12 C 34 Si (probability about ) (n,xn) reaction CARMEN -- NFS
Week 10: Chap. 14 Slow Neutron Detection
Week 10: Chap. 14 Slow Neutron Detection (Gamma ray) Backgrounds Slow Neutron Detection -- nuclear reactions --- spectra properties -- Proportional Counters --- fill gas --- lined detectors Fast neutron
More informationPreparatory experiments for cold-neutron induced fission studies at IKI
Preparatory experiments for cold-neutron induced fission studies at IKI A. Oberstedt 1, S. Oberstedt 2, R. Billnert 1, J. Karlsson 1, X. Ledoux 3, J.-G. Marmouget 3 and F.-J. Hambsch 2 1 School of Science
More informationSURROGATE REACTIONS. An overview of papers by Jason Burke from LLNL
SURROGATE REACTIONS An overview of papers by Jason Burke from LLNL Compound Nuclear Reaction cross sections Cross sections for compound-nuclear reactions are required input for astrophysical models and
More informationMeasurement of prompt fission γ-ray spectra in fast neutroninduced
Available online at www.sciencedirect.com Physics Procedia 31 (2012 ) 13 20 GAMMA-1 Emission of Prompt Gamma-Rays in Fission and Related Topics Measurement of prompt fission γ-ray spectra in fast neutroninduced
More informationThe Nucifer Experiment: Non-Proliferation with Reactor Antineutrinos
The Nucifer Experiment: Non-Proliferation with Reactor Antineutrinos Andi S. Cucoanes1 for the Nucifer Collaboration* * V.M.Bui2, M.Cribier1, A.S.Cucoanes1, M.Fallot2, M.Fechner1, J.Gaffiot1, L.Giot2,
More informationarxiv: v1 [physics.ins-det] 29 Jun 2011
Investigation of Large LGB Detectors for Antineutrino Detection P. Nelson a,, N. S. Bowden b, a Department of Physics, Naval Postgraduate School, Monterey, CA 99, USA b Lawrence Livermore National Laboratory,
More informationA Trial of Neutrino Detection from Joyo Fast Research Reactor
A Trial of Neutrino Detection from Joyo Fast Research Reactor F.Suekane Tohoku University For KASKA group, made up of; Tohoku Univ., Tokyo Inst. of Tech., Niigata Univ., Tokyo Metropolitan Univ., Tohoku
More informationFAST NEUTRON MULTIPLICITY COUNTER
FAST NEUTRON MULTIPLICITY COUNTER Di Fulvio A. 1, Shin T. 1, Sosa C. 1, Tyler J. 1, Supic L. 1, Clarke S. 1, Pozzi S. 1, Chichester D. 2 1 Department of Nuclear Engineering and Radiological Science of
More informationVorobyevA.S., ShcherbakovO.A., GagarskiA.M., Val ski G.V., Petrov G.A.
Investigation of the Prompt Neutron Emission Mechanism in Low Energy Fission of 233, 235 U(n th, f) and 252 Cf(sf) VorobyevA.S., ShcherbakovO.A., GagarskiA.M., Val ski G.V., Petrov G.A. Petersburg Nuclear
More informationScintillation 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 informationCapture and Fission with DANCE and NEUANCE
Capture and Fission with DANCE and NEUANCE Marian Jandel Nuclear and Radiochemistry Group P(ND)^2-2, Oct 14-17, 2014, Bruyeres-le-Chatel, France UNCLASSIFIED Nuclear data measurements at DANCE Neutron
More informationAngular and energy distributions of the prompt fission neutrons from thermal neutron-induced fission of 239 Pu
Angular and energy distributions of the prompt fission neutrons from thermal neutron-induced fission of 239 Pu Vorobyev AS, Shcherbakov OA, Gagarski AM, Val ski GV, Petrov GA National Research Center Kurchatov
More informationCharged particles detectors Arrays (1)
Charged particles detectors Arrays (1) Basic concepts of particle detection: scintillators & semiconductors Light charged particles (p, α, e) Arrays: DIAMANT, ISIS, EUCLIDES, MiniOrange Large Arrays: CHIMERA,
More informationCf-252 spontaneous fission prompt neutron and photon correlations
Cf-252 spontaneous fission prompt neutron and photon correlations M. J. Marcath 1,*, P. Schuster 1, P. Talou 2, I. Stetcu 2, T. Kawano 2, M. Devlin 2, R. C. Haight 2, R. Vogt 3,4, J. Randrup 5, S. D. Clarke
More informationHe-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 informationDETERMINATION OF THE NEUTRON FISSION CROSS-SECTION FOR 233 Pa FROM 0.5 TO 10 MeV USING THE TRANSFER REACTION 232 Th( 3 He,pf) 234 Pa.
DETERMINATION OF THE NEUTRON FISSION CROSS-SECTION FOR 233 Pa FROM 0.5 TO 10 MeV USING THE TRANSFER REACTION 232 Th( 3 He,pf) 234 Pa M. Petit 1), M. Aiche 1), S. Andriamonje 1), G. Barreau 1), S. Boyer
More informationDetermination of 210 Pb and 210 Po in Water Samples
1 Determination of 210 Pb and 210 Po in Water Samples Marin Ayranov 1, Zornitza Tosheva 2, Antoine Kies 2 1 Institute for Nuclear Research and Nuclear Energy, 72 Tzarigradsko chaussee, BG-1784 Sofia, Bulgaria
More informationCross-section Measurements of Relativistic Deuteron Reactions on Copper by Activation Method
Nuclear Physics Institute, Academy of Sciences of the Czech Republic Department of Nuclear Reactors, Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague Cross-section
More informationNeutrinos. Why measure them? Why are they difficult to observe?
Outline What is a neutrino? Why do we want to study them? Building a detector to detect the undetectable What does a neutrino detector see? How do you seperate a neutrino signal from the background? Neutrinos
More informationSOFIA Fission studies at GSI
SOFIA Fission studies at GSI Julie-Fiona Martin for the SOFIA collaboration CEA, DAM, DIF Perspective on Nuclear Data for the Next Decade - Oct. 2014 1 Intro 2 Experimental setup Secondary beam Fission
More informationObservation of Reactor Antineutrinos at RENO. Soo-Bong Kim for the RENO Collaboration KNRC, Seoul National University March 29, 2012
Observation of Reactor Antineutrinos at RENO Soo-Bong Kim for the RENO Collaboration KNRC, Seoul National University March 29, 2012 Outline Introduction Experimental setup & detector Data-taking & data
More informationInvestigation of fast neutron spectroscopy capability of 7 Li and 6. Li enriched CLYC scintillator for nuclear physics experiments
ANSRI Application of Novel Scintillators for Research and Industry 16 May, 1 th _ 6 th 16 Dublin, Ireland Investigation of fast neutron spectroscopy capability of 7 Li and 6 Li enriched CLYC scintillator
More informationLouis Baum University of Michigan, REU Student Summer UM Nuclear Sciences Group
Louis Baum University of Michigan, REU Student Summer 2011 UM Nuclear Sciences Group Overview Background Why Detectors Time of Flight Road Blocks Conclusion Main Side Project Californium 252 Fission Source
More informationAn 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 informationCharacterization of 3D thermal neutron semiconductor detectors
Characterization of 3D thermal neutron semiconductor detectors J.Uher 1, C.Fröjdh 2, J.Jakůbek 1, C.Kenney 3, Z.Kohout 4, V.Linhart 1, S.Parker 5, S.Petersson 2, S.Pospíšil 1, G.Thungström 2 (1),, Czech
More informationChapter 3: Neutron Activation and Isotope Analysis
Chapter 3: Neutron Activation and Isotope Analysis 3.1. Neutron Activation Techniques 3.2. Neutron Activation of Paintings 3.3. From Qumran to Napoleon 3.4. Neutron Activation with Accelerators 3.5. Isotope
More informationNeutron capture cross section on Lu isotopes at DANCE
Neutron capture cross section on Lu isotopes at DANCE Los Alamos National Laboratory Los Alamos, New-Mexico 8755, USA and CEA, DAM, DIF F-9197 Arpajon, France E-mail: olivier.roig@cea.fr A. Couture 1 Los
More informationSCINTILLATION DETECTORS AND PM TUBES
SCINTILLATION DETECTORS AND PM TUBES General Characteristics Introduction Luminescence Light emission without heat generation Scintillation Luminescence by radiation Scintillation detector Radiation detector
More informationDetectors for the measurement of ionizing radiation
For the measurement of radiation, the following reactions during the irradiation of matter are predominantly utilized: Ionization in gases (Ionization chamber, proportional flow counter, release counter)
More informationPhotonuclear Activation File. Status and Perspectives
Photonuclear Activation File ((( P A F ))) Status and Perspectives M-L. Giacri, A. Vanlauwe, J-C. David, D. Doré, D. Ridikas, I. Raskinyte, E. Dupont, V. Macary CEA Saclay, DSM/Dapnia/SPhN http://www-dapnia.cea.fr/sphn/mnm/
More informationJRC Place on dd Month YYYY Event Name 1
JRC Place on dd Month YYYY Event Name 1 A new measurement of the prompt fission neutron emission spectrum of 235 U(n,f) Correlation of prompt neutron emission with fission fragment properties F.-J. Hambsch
More informationHrant Gulkanyan and Amur Margaryan
ALPHA-SPECTROSCOPY OF 252 Cf DECAYS: A NEW APPROACH TO SEARCHING FOR THE OCTONEUTRON YerPhI Preprint -1628 (2014) Hrant Gulkanyan and Amur Margaryan A.I. Alikhanyan National Science Laboratory (Yerevan
More informationRapid Extraction of Plutonium from Urine by Pyrosulfate Fusion and
Rapid Extraction of Plutonium from Urine by Pyrosulfate Fusion and PERALS Spectroscopy R.L. Metzger, P.H. Pouquette, and G.W. Klingler Radiation Safety Engineering, Inc. Chandler, AZ Abstract To effectively
More information(a) (i) State the proton number and the nucleon number of X.
PhysicsAndMathsTutor.com 1 1. Nuclei of 218 84Po decay by the emission of an particle to form a stable isotope of an element X. You may assume that no emission accompanies the decay. (a) (i) State the
More informationActivation Analysis. Characteristic decay mechanisms, α, β, γ Activity A reveals the abundance N:
2.5. Isotope analysis and neutron activation techniques The previously discussed techniques of material analysis are mainly based on the characteristic atomic structure of the elements and the associated
More informationNeutron Induced Nuclear Counter Effect in Hamamatsu Silicon APDs and PIN Diodes
Neutron Induced Nuclear Counter Effect in Hamamatsu Silicon APDs and PIN Diodes Rihua Mao, Liyuan Zhang, Ren-yuan Zhu California Institute of Technology Introduction Because of its immunity to magnetic
More informationReactor On/Off Monitoring with a Prototype of Plastic Anti-neutrino Detector Array (PANDA)
Reactor On/Off Monitoring with a Prototype of Plastic Anti-neutrino Detector Array (PANDA) Yasuhiro Kuroda A, Yo Kato A, Nozomu Tomita A, Ryoko Nakata, Shugo Oguri, Chikara Ito B, Yoshizumi Inoue C, Makoto
More informationMeasurement of (n, xn γ) reaction cross sections in W isotopes
Measurement of (n, xn γ) reaction cross sections in isotopes Greg Henning IPHC/CNRS 1 Context: Nuclear data evaluations for applications 4 th generation nuclear reactors and new fuel cycles, currently
More informationIntroduction to Radiological Sciences Neutron Detectors. Theory of operation. Types of detectors Source calibration Survey for Dose
Introduction to Radiological Sciences Neutron Detectors Neutron counting Theory of operation Slow neutrons Fast neutrons Types of detectors Source calibration Survey for Dose 2 Neutrons, what are they?
More informationPhase stability and lithium loading capacity in a liquid scintillation cocktail
Phase stability and lithium loading capacity in a liquid scintillation cocktail Denis E. Bergeron, H. Pieter Mumm, Mark Tyra Physical Measurement Laboratory, National Institute of Standards and Technology,
More informationin Cross-Section Data
Sensitivity of Photoneutron Production to Perturbations in Cross-Section Data S. D. Clarke Purdue University, West Lafayette, Indiana S. A. Pozzi University of Michigan, Ann Arbor, Michigan E. Padovani
More informationThe neutron multiplicity study at spontaneous fission of short-lived isotopes (z > 100) using VASSILISSA recoil separator
The neutron multiplicity study at spontaneous fission of short-lived isotopes (z > 100) using VASSILISSA recoil separator Svirikhin A.I. Joint Institute for Nuclear Research, Dubna, Russia Manipal University,
More informationA 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 informationNeutron emission asymmetries from linearly polarized γ rays on nat Cd, nat Sn, and 181 Ta
Neutron emission asymmetries from linearly polarized γ rays on nat Cd, nat Sn, and 8 Ta Clarke Smith, Gerald Feldman, and the HIγS Collaboration George Triangle C. Smith, G. Feldman (GWU) Washington University
More information1 Introduction. KOPIO charged-particle vetos. K - RARE Meeting (Frascati) May Purpose of CPV: veto Kl
Introduction - Purpose of CPV: veto Kl decay modes with a real or apparent π and a pair of charged particles - Examples of background modes: (i) K l π π + π (ii) K l π π ± eν there are always (iii) K l
More informationPresent and Future of Fission at n_tof
16th ASRC International Workshop " Nuclear Fission and Structure of Exotic Nuclei " Present and Future of Fission at n_tof Christina Weiss, CERN, Geneva/Switzerland 20.03.2014 Present and Future of Fission
More informationAddendum to the ISOLDE and Neutron Time-of-Flight Committee
` EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH Addendum to the ISOLDE and Neutron Time-of-Flight Committee IS530: Properties of low-lying intruder states in 34 Al and 34 Si sequentially populated in beta-decay
More informationDedicated Arrays: MEDEA GDR studies (E γ = MeV) Highly excited CN E*~ MeV, 4 T 8 MeV
Dedicated Arrays: MEDEA GDR studies (E γ = 10-25 MeV) Highly excited CN E*~ 250-350 MeV, 4 T 8 MeV γ-ray spectrum intermediate energy region 10 MeV/A E beam 100 MeV/A - large variety of emitted particles
More informationMeasurements of liquid xenon s response to low-energy particle interactions
Measurements of liquid xenon s response to low-energy particle interactions Payam Pakarha Supervised by: Prof. L. Baudis May 5, 2013 1 / 37 Outline introduction Direct Dark Matter searches XENON experiment
More informationQuality Assurance. Purity control. Polycrystalline Ingots
Quality Assurance Purity control Polycrystalline Ingots 1 Gamma Spectrometry Nuclide Identification Detection of Impurity Traces 1.1 Nuclides Notation: Atomic Mass Atomic Number Element Neutron Atomic
More informationDepartment of Chemistry, University of Rochester, Rochester, N.Y POC:
A Mobile Accelerator-Based Neutron Diagnostics Instrument W. Udo Schröder and Jan Tōke Department of Chemistry, University of Rochester, Rochester, N.Y. 14627 POC: schroeder@chem.rochester.edu Project
More informationMeasurement 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 informationCHARACTERIZING THE DETECTOR RESPONSE AND TESTING THE PERFORMANCE OF A NEW WELL COUNTER FOR NEUTRON COINCIDENCE MEASUREMENTS OF PLUTONIUM IN RESIDUES
LA-UR-01-3848 CHARACTERIZING THE DETECTOR RESPONSE AND TESTING THE PERFORMANCE OF A NEW WELL COUNTER FOR NEUTRON COINCIDENCE MEASUREMENTS OF PLUTONIUM IN RESIDUES A. P. Belian, M. C. Browne, N. Ensslin,
More informationLiquid Scintillator Timing Property
Liquid Scintillator Timing Property Minfang Yeh Neutrino and Nuclear Chemistry, BNL MIT workshop, Dec 15, 2015 Main Neutrino Interactions in Scintillator + p ; KamLAND v e + 12 C e 12 B 12 C e v e v +
More informationApplication of prompt gamma activation analysis with neutron beams for the detection and analysis of nuclear materials in containers
Application of prompt gamma activation analysis with neutron beams for the detection and analysis of nuclear materials in containers Zsolt Révay Institute of Isotopes, Budapest, Hungary Dept. of Nuclear
More informationCharacterization of a Portable Neutron Coincidence Counter Angela Thornton and W. Charlton Texas A&M University College Station, TX
Characterization of a Portable Neutron Coincidence Counter Angela Thornton and W. Charlton Texas A&M University College Station, TX 77843 Abstract Neutron coincidence counting is a technique widely used
More informationResearch in NDA Techniques for Waste Characterization at the JRC
1 Research in NDA Techniques for Waste Characterization at the JRC Bent Pedersen Nuclear Security Unit Institute for Transuranium Elements Joint Research Centre presented at Annual meeting of LABONET Network
More informationThis paper should be understood as an extended version of a talk given at the
This paper should be understood as an extended version of a talk given at the Abstract: 1 st JINA workshop at Gull Lake, 2002. Recent experimental developments at LANL (Los Alamos, NM, USA) and CERN (Geneva,
More informationMonte Carlo Simulations for Future Geoneutrino Detectors
Monte Carlo Simulations for Future Geoneutrino Detectors Morgan Askins Abstract The main contribution of heat in the earth s mantle is thought to be the radioactive decays of 238 U, 232 T h, and 40 K.
More informationFactors Affecting Detector Performance Goals and Alternative Photo-detectors
XENON Experiment - SAGENAP Factors Affecting Detector Performance Goals and Alternative Photo-detectors Department of Physics Brown University Source at http://gaitskell.brown.edu Gaitskell Review WIMP
More informationThe investigations in the field of advanced nuclear power systems for energy production and transmutation of RAW in NAS of Belarus
The investigations in the field of advanced nuclear power systems for energy production and transmutation of RAW in NAS of Belarus on behalf of YALINA team Dr. Kiyavitskaya H. ISTC meeting «Feature technology:
More informationNeutron transmission and capture measurements for 241 Am at GELINA
Neutron transmission and capture measurements for 241 Am at GELINA C. Lampoudis, S. Kopecky, A. Plompen, C. Sage P. Schillebeeckx, R. Wynants, O. Bouland, G. Noguere and F. Gunsing 3 rd International Workshop
More informationNeutrons For Science
Neutrons For Science NFS is one of the two facilities of the LINAG Experimental Area se of the LINAG s beams to produce neutrons between 1 and 40 MeV The NFS is composed of : - A neutron beam in a Time-Of-Flight
More informationRADIATION DETECTION AND MEASUREMENT
RADIATION DETECTION AND MEASUREMENT SECOND EDITION GLENN F. KNOLL Professor of Nuclear Engineering The University of Michigan Ann Arbor, Michigan WILEY JOHN WILEY & SONS New York Chichester Brisbane Toronto
More informationRivelazione di neutrini solari - Borexino Lino Miramonti 6 Giugno 2006 Gran Sasso
Rivelazione di neutrini solari - Borexino Lino Miramonti 6 Giugno 2006 Gran Sasso 1 RADIOCHEMICAL Integrated in energy and time CHERENKOV Less than 0.01% of the solar neutrino flux is been measured in
More informationCHARACTERISTICS OF LIGHT CHARGED PARTICLE EMISSION IN THE TERNARY FISSION OF 250 CF AND 252 CF AT DIFFERENT EXCITATION ENERGIES
CHARACTERISTICS OF LIGHT CHARGED PARTICLE EMISSION IN THE TERNARY FISSION OF 25 CF AND 252 CF AT DIFFERENT EXCITATION ENERGIES S. VERMOTE AND C. WAGEMANS Department of Physics and Astronomy, University
More informationMCNP6 simulation validation of fast neutron coincidence detection system for nuclear security and safeguards applications
MCNP6 simulation validation of fast neutron coincidence detection system for nuclear security and safeguards applications Débora M. Trombetta 1, Bo Cederwall 1, Kåre Axell1 2 1 Department of Physics, KTH
More informationHigh Precision Nondestructive Assay to Complement DA. H.O. Menlove, M.T. Swinhoe, and J.B. Marlow Los Alamos National Laboratory
High Precision Nondestructive Assay to Complement DA H.O. Menlove, M.T. Swinhoe, and J.B. Marlow Los Alamos National Laboratory LA-UR-07-6857 Abstract Large scale spent fuel reprocessing plants and fuel
More informationPulsed Neutron Interrogation Test Assembly - PUNITA
Pulsed Neutron Interrogation Test Assembly - PUNITA Bent Pedersen Nuclear Security Unit Institute for Transuranium Elements - ITU Joint Research Centre presented at IPNDV WG3 meeting, 12-13 May 2016 JRC,
More informationNuclear Reactions A Z. Radioactivity, Spontaneous Decay: Nuclear Reaction, Induced Process: x + X Y + y + Q Q > 0. Exothermic Endothermic
Radioactivity, Spontaneous Decay: Nuclear Reactions A Z 4 P D+ He + Q A 4 Z 2 Q > 0 Nuclear Reaction, Induced Process: x + X Y + y + Q Q = ( m + m m m ) c 2 x X Y y Q > 0 Q < 0 Exothermic Endothermic 2
More informationThe NFS project. Part of the SPIRAL-2 project built on the GANIL site, Caen, France. NFS is one of the two facilities of the LINAG Experimental Area
The NFS project Part of the SPIRAL-2 project built on the GANIL site, Caen, France NFS is one of the two facilities of the LINAG Experimental Area Neutron beam between 100 kev and 40 MeV Irradiation station
More informationNeutron- and muoninduced. underground physics experiments. L. Pandola, V. Tomasello and V. Kudryavtsev. for the JRA1 and N3 simulation groups
Neutron- and muoninduced background in underground physics experiments L. Pandola, V. Tomasello and V. Kudryavtsev for the JRA1 and N3 simulation groups ILIAS 4 th Annual Meeting, Chambery, 2007 ILIAS
More informationNeutron capture and fission reactions on. sections, -ratios and prompt -ray emission from fission. 1 Introduction and Motivation
EPJ Web of Conferences 42, 01002 (2013) DOI: 10.1051/ epjconf/ 20134201002 C Owned by the authors, published by EDP Sciences, 2013 Neutron capture and fission reactions on 235 U : cross sections, -ratios
More informationNeutron 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 informationLSC for Quality Control of 99m TC Eluate from 99 Mo- 99m Tc Generator
LSC2017 Conference 1-5th May, 2017, Copenhagen LSC for Quality Control of 99m TC Eluate from 99 Mo- 99m Tc Generator Xiaolin Hou Technical University of Denmark, Center for Nuclear Technologies Roskilde,
More informationResults on geoneutrinos at Borexino experiment. Heavy Quarks and Leptons Yamagata Davide Basilico
Results on geoneutrinos at Borexino experiment Heavy Quarks and Leptons 2018 - Yamagata Davide Basilico Outline 1. Geoneutrinos 2. Borexino 3. Analysis and results 2 What are geoneutrinos? Distribution
More informationVerification measurements of alpha active waste
Verification measurements of alpha active waste Bent Pedersen Nuclear Security Unit Directorate Nuclear Safety and Security JRC 9th Edition of the International Summer School on Nuclear Decommissioning
More informationRDCH 702 Lecture 8: Accelerators and Isotope Production
RDCH 702 Lecture 8: Accelerators and Isotope Production Particle generation Accelerator Direct Voltage Linear Cyclotrons Synchrotrons Photons * XAFS * Photonuclear Heavy Ions Neutrons sources Fission products
More informationVerification measurements of alpha active waste
Verification measurements of alpha active waste Bent Pedersen Nuclear Security Unit Institute for Transuranium Elements (ITU), JRC Operational Issues in Radioactive Waste Management and Nuclear Decommissioning
More informationFuture research program on prompt γ-ray emission in nuclear fission
Future research program on prompt γ-ray emission in nuclear fission Robert Billnert, Aleksandar Dragic, Angélique Gatera, Alf Göök, Pierre Halipré, Mattieu Lebois, Andreas Oberstedt, Stephan Oberstedt,
More informationAvailable online at ScienceDirect. Physics Procedia 64 (2015 )
Available online at www.sciencedirect.com ScienceDirect Physics Procedia 64 (2015 ) 101 106 Scientific Workshop on Nuclear Fission dynamics and the Emission of Prompt Neutrons and Gamma Rays, THEORY-3
More informationStudy of prompt neutron emission spectra in fast neutron induced fission of 238 U and 232 Th and 30 kev neutron induced fission on 235 U
Study of prompt neutron emission spectra in fast neutron induced fission of 238 U and 232 Th and 30 kev neutron induced fission on 235 U S. Appannababu 1, J. Praena 2, P.F. Mastinu 1, T. Marchi 1, V.V.
More informationThe Search for θ13 : First Results from Double Chooz. Jaime Dawson, APC
The Search for θ13 : First Results from Double Chooz Jaime Dawson, APC Contents Brief reminder θ13 current knowledge Reactor experiments Double Chooz Far detector Calibration Neutrinos & Backgrounds Oscillation
More informationCorrelation in Spontaneous Fission of Cf252
Correlation in Spontaneous Fission of Cf252 Stefano Marin 1, Matthew J. Marcath 1, Patricia F. Schuster 1, Shaun D. Clarke 1, and Sara A. Pozzi 1 1. Department of Nuclear Engineering and Radiological Sciences,
More informationDetermination of H-3 and C-14 in the frame of decommissioning projects at the Paul Scherrer Institute
Determination of H-3 and C-14 in the frame of decommissioning projects at the Paul Scherrer Institute Jost Eikenberg, Maya Jäggi, Max Rüthi Paul Scherrer Institute, CH-5232 Villigen, Switzerland Content
More informationRadiation Detection and Measurement
Radiation Detection and Measurement Third Edition Glenn F. Knoll Professor of Nuclear Engineering and Radiological Sciences University of Michigan Ann Arbor, Michigan John Wiley & Sons, Inc. New York/Chichester/Weinheim/Brisbane/Toronto/Singapore
More informationPoS(ICHEP2016)474. SoLid: Search for Oscillations with a Lithium-6 Detector at the SCK CEN BR2 reactor
SoLid: Search for Oscillations with a Lithium-6 Detector at the SCK CEN BR2 reactor University of Bristol E-mail: dan.saunders@bristol.ac.uk The disappearance of reactor antineutrinos into a new neutral
More informationarxiv: v1 [physics.ins-det] 3 Feb 2011
Nuclear Instruments and Methods in Physics Research A 00 (2018) 1 5 Alogo.pdf Nuclear Instruments and Methods in Physics Research A Scintillation decay time and pulse shape discrimination in oxygenated
More informationWaveform Analysis for DM-Ice17. Zachary Pierpoint University of Wisconsin - Madison October 21, 2013 Yale Weak Interactions Discussions Group
Waveform Analysis for DM-Ice17 Zachary Pierpoint University of Wisconsin - Madison October 21, 213 Yale Weak Interactions Discussions Group DM-Ice17 Energy Spectrum counts / day / kev / kg 1 28 Tl+ 214
More informationAm cross section measurements at GELINA. S. Kopecky EC JRC IRMM Standards for Nuclear Safety, Security and Safeguards (SN3S)
241 Am cross section measurements at GELINA S. Kopecky EC JRC IRMM Standards for Nuclear Safety, Security and Safeguards (SN3S) TOF - Facility GELINA Pulsed white neutron source (10 mev < E n < 20 MeV)
More information1220 QUANTULUS The Ultra Low Level Liquid Scintillation Spectrometer
1220 QUANTULUS The Ultra Low Level Liquid Scintillation Spectrometer PerkinElmer LAS (UK) Ltd, Chalfont Rd, Seer Green, Beaconsfield, Bucks HP9 2FX tel: 0800 896046 www.perkinelmer.com John Davies January
More informationKamLAND. Introduction Data Analysis First Results Implications Future
KamLAND Introduction Data Analysis First Results Implications Future Bruce Berger 1 Tohoku University, Sendai, Japan University of Alabama University of California at Berkeley/LBNL California Institute
More informationHigh efficiency 3 He neutron detector TETRA for DESIR.
DESIR workshop, May 2010 High efficiency 3 He neutron detector TETRA for DESIR. Yuri Penionzhkevich Joint Institute for Nuclear Research, Dubna Beta Decay of Exotic Nuclei: Goal to study Neutron emission
More informationCOMPARATIVE STUDY OF PIGE, PIXE AND NAA ANALYTICAL TECHNIQUES FOR THE DETERMINATION OF MINOR ELEMENTS IN STEELS
COMPARATIVE STUDY OF PIGE, PIXE AND NAA ANALYTICAL TECHNIQUES FOR THE DETERMINATION OF MINOR ELEMENTS IN STEELS ANTOANETA ENE 1, I. V. POPESCU 2, T. BÃDICÃ 3, C. BEªLIU 4 1 Department of Physics, Faculty
More informationThe TDCR method in LSC. P. Cassette Laboratoire National Henri Becquerel CEA/LNE, France
The TDCR method in LSC P. Cassette Laboratoire National Henri Becquerel CEA/LNE, France LIQUID SCINTILLATION USERS FORUM 2009 Summary I. Some information on LSC II. LSC in metrology: the free parameter
More informationA Monte Carlo Simulation of Prompt Gamma Emission from Fission Fragments
A Monte Carlo Simulation of Prompt Gamma Emission from Fission Fragments D. Regnier, O. Litaize, O. Serot CEA Cadarache, DEN/DER/SPRC/LEPH WONDER, 27/09/2012 D. Regnier, O. Litaize, O. Serot - CEA Cadarache,
More informationRadiation Detection and Measurement
Radiation Detection and Measurement Fourth Edition Glenn F. Knoll Professor Emeritus of Nuclear Engineering and Radiological Sciences University of Michigan Ann Arbor, Michigan WILEY John Wiley & Sons,
More informationChapter 11: Neutrons detectors
Chapter 11: Neutrons detectors 1 Contents Principles of neutrons detection Slow neutron detection methods Fast neutron detection methods 2 Introduction Neutrons are uncharged particles cannot be directly
More informationTIME-RESOLVED LIQUID SCINTILLATION COUNTING
[RADOCARBON, VOL 32, No. 3, 1990, P 381-386] TME-RESOLVED LQUD SCNTLLATON COUNTNG MCHAEL KESSLER Packard nstrument Company, One State Street, Meriden, Connecticut 06450 ABSTRACT. Historically, scientists
More informationAdvanced Heavy Water Reactor. Amit Thakur Reactor Physics Design Division Bhabha Atomic Research Centre, INDIA
Advanced Heavy Water Reactor Amit Thakur Reactor Physics Design Division Bhabha Atomic Research Centre, INDIA Design objectives of AHWR The Advanced Heavy Water Reactor (AHWR) is a unique reactor designed
More information