Measurements of (n,px), (n,dx), (n,tx) and (n,αx) reactions. between 25 and 70 MeV at Louvain-la-Neuve
|
|
- Doreen Owen
- 5 years ago
- Views:
Transcription
1 Measurements of (n,px), (n,dx), (n,tx) and (n,αx) reactions between 25 and 70 MeV at Louvain-la-Neuve J.-P. Meulders, S. Benck, V. Corcalciuc, I. Slypen Institut de physique nucléaire, Chemin du cyclotron, 2 B-1348 Louvain-la-Neuve BELGIUM Meulders Jean-Pierre, Slypen Isabelle 1
2 Outline A. LLN program in neutron induced reactions 1. Introduction 2. Measurements 3. Results 4. Conclusions 2.1 Experimental set-up 2.2 Data reduction 3.1 Double-differential cross sections 3.2 Energy-differential cross sections 3.3 Applications B. Concerted Action Physical Aspect of Lead as a neutron producing target for accelerator transmutation devices Meulders Jean-Pierre, Slypen Isabelle 2
3 A. LLN program in neutron induced reactions 1. Introduction Measurements of double-differential cross sections of the (n,px), (n,dx), (n,tx) and (n,αx) reactions on 12 C, 16 O, 27 Al, Si, Pb and 209 Bi at different incident neutron energies (25-75 MeV) Angular distributions from 20 to 160 in steps of 10 energy-differential cross sections angle-differential cross sections total production cross sections Meulders Jean-Pierre, Slypen Isabelle 3
4 Interests: basic nuclear physics information a reaction mechanisms a nuclear structure many interdisciplinary applications a kerma factors for neutron therapy and neutron dosimetry (H, C, O) a single upset events in computer memory chips (Al, Si, O) a accelerator driven systems (Pb, Bi) Meulders Jean-Pierre, Slypen Isabelle 4
5 2.1. Experimental set-up 2. Measurements Neutron source: nat Li(p,n)Be reaction (3 mm thick target) Incident proton energy: 65 MeV Neutron energy of the monoenergetic peak: 62.7 MeV Neutron energy spectrum and beam profile Meulders Jean-Pierre, Slypen Isabelle 5
6 Experimental set-up 6 E-E telescopes connected to a reaction chamber Figure not on scale Meulders Jean-Pierre, Slypen Isabelle 6
7 Detailed vue of a E-E telescope Event by event acquisition Particle identification: charge integration of the output signals biparametric slow vs. fast component of CsI light output pulse biparametric E vs. E Meulders Jean-Pierre, Slypen Isabelle 7
8 Particle selection Slow vs. fast representation after background elimination E vs. E representation after identification of protons for further selection Meulders Jean-Pierre, Slypen Isabelle 8
9 Meulders Jean-Pierre, Slypen Isabelle 9
10 2.2 Data reduction Targets 12 C, Al 2 O 3, 27 Al, Si, Pb, 209 Bi (50x50x1 mm 3, 60x60x0.3 mm 3 ) Relative normalization of the spectra: neutron beam flux (2 different beam monitors) solid angles (including beam-profile) number of target nuclei Absolute normalization to the measured H(n,p) cross sections: (C 3 H 6 ) n target Energy calibration: recoil p / d from (C 3 H 6 ) n / (C 3 D 6 ) n target + an α-source Corrections for the particle loss due to the thickness ( 1 or 0.3 mm) of the target Meulders Jean-Pierre, Slypen Isabelle 10
11 Time of flight measurement between a capacitive beam pick-off and the E detector reconstruction of the neutron spectrum corresponding to the selected particles Deuteron spectrum and corresponding reconstructed neutron spectrum (insert) Meulders Jean-Pierre, Slypen Isabelle 11
12 3. Results 3.1 Double-differential cross sections 27 Al(n,px) for E n = 62.7 MeV at different lab. angles ( ) Meulders Jean-Pierre, Slypen Isabelle 12
13 1er transparent de confportrait.ppt Meulders Jean-Pierre, Slypen Isabelle 13
14 3.2 Energy differential cross sections for each particle and each incident neutron energy - to complete angular distribution: a exp (b cosθ) Al target, E = 62.7 MeV n lab. angle = 10 deg. LLN extrapolation data from proton induced reactions on Al at 61.0 MeV (Bertrand and Peelle) Meulders Jean-Pierre, Slypen Isabelle 14
15 Cross sections on Al at E = 62.7 MeV n LLN data data from proton induced reactions on Al at 61 MeV GNASH calculation FKK prediction Meulders Jean-Pierre, Slypen Isabelle 15
16 3.3 Applications Kerma (Kinetic Energy Released per Mass unit) k d = N ( σ ) de i i E i E Elemental composition by weight of ICRU muscle, fat, bone, muscle-equivalent plastic A-150 and tissueequivalent gas (TE). i Element ICRU muscle (%) (ICRU 1977) Fat (adipose) (%) (ICRU 1989) Bone (cortical) (%) (ICRU 1989) A-150 plastic (%) TE gas (%) H ± C ± O ± N ± Ca ±0.1 - F ±0.1 - others Meulders Jean-Pierre, Slypen Isabelle 16
17 Total kerma on Oxygen without LLN data Kerma factor (fgym 2 ) Brady (1979) Romero (1985) Schrewe (1995) Schrewe (1997) Hartmann (1992) De Luca (1988) Chadwick (1998) Brenner (1983) White (1992) Dimbylow (1982) Neutron energy (MeV) Meulders Jean-Pierre, Slypen Isabelle 17
18 Total kerma on Oxygen with LLN data Kerma factor (fgym 2 ) present work p re se nt wo rk e xtra p o la tion Brady (1979) Romero (1985) Schrewe (1995) Schrewe (1997) Hartmann (1992) De Luca (1988) Chadwick (1998) Brenner (1983) White (1992) Dimbylow (1982) Neutron energy (MeV) Meulders Jean-Pierre, Slypen Isabelle 18
19 microelectronic Comparison Si(n,px) - Al(n,px) for E = 62.7 MeV n Al 3 20 o 3 70 o Si d/ded σω (mb/mev sr) o 60 o o 140 o Proton Energy (MeV) Meulders Jean-Pierre, Slypen Isabelle 19
20 Accelerator driven systems Measurements of double differential cross sections of (n,px), (n,dx), (n,tx) and (n,αx) reactions on Lead and Bismuth at 9 angles and for several incident neutron energies between 30 and 65 MeV (July 1998) Collaboration for Lead measurements Subatech Nantes LPC Caen Analysis in progress for Lead data M. Kerveno, Ph. D. student, Subatech Nantes Meulders Jean-Pierre, Slypen Isabelle 20
21 2e transparent de confportrait.ppt Meulders Jean-Pierre, Slypen Isabelle 21
22 B. Concerted Action : Physical aspects of lead as a neutron producing target for accelerator transmutation devices N Name Organisation Laboratory City Abbreviated Name 1 J.-P. Meulders UCL Louvain-la-Neuve 2 N. Olsson UU University of Uppsala 3 R. Michel ZSR Hannover 4 H. Schuhmacher PTB Braunschweig 5 S. Leray CEA Saclay Saclay 6 P. Eudes CNRS Nantes Subatech Nantes 7 S. Brandenburg KVI Groningen 8 A. Koning ECN Petten 9 P. Armbuster GSI Darmstadt 10 D. Filges FZJ Jülich 11 A. Willis CNRS Orsay IPN Orsay 12 J.-F. Lecolley LPC Caen LPC Caen 13 J. Cugnon U. Lg. Liège Meulders Jean-Pierre, Slypen Isabelle 22
23 Experiments on lead targets involved in the Concerted Action (1/8/98-31/7/2000) Responsible Institution Energy Reaction Site of experiment CNRS Nantes MeV (p,xn) + (p,xp), (p,xd), (p,xt), (p,xα) UCL Louvain-la- Neuve UCL Louvain-la- Neuve MeV (n,xp), (n,xd), (n,xt), (n,xα) UCL Louvain-la- Neuve ZSR Hannover < 70 MeV (p,x) Paul Scherrer Institute Villigen (CH) Participating partners CNRS Caen, UCL CNRS Nantes, LPC Caen FZJ PTB MeV (n,x) UCL Louvain-la- ZSR, UCL Braunschweig Neuve ZSR Hannover 100 MeV (n,x) UU Uppsala UU, PTB UU Uppsala MeV (n,n) UU Uppsala UU, LPC Caen, CNRS Nantes KVI Groningen 190 MeV (p,f), (p,x) KVI Groningen ECN Petten, CNRS Orsay CEA Saclay MeV (p,xn), (d,xn) CEA Saturne Saclay GSI Darmstadt MeV H(Pb,x) GSI Darmstadt CEA Saclay, CNRS Orsay FZJ Jülich < 2500 MeV (p,xn) multiplicity FZJ Jülich U. Lg, UU, LPC Caen, CNRS Orsay Meulders Jean-Pierre, Slypen Isabelle 23
LIGHT CHARGED PARTICLE PRODUCTION INDUCED BY FAST NEUTRONS (E N = MEV) ON 59 Co AND nat Fe. Abstract
LIGHT CHARGED PARTICLE PRODUCTION INDUCED BY FAST NEUTRONS (E N = 25-65 MEV) ON 59 Co AND nat Fe E. Raeymackers, N. Nica, 1 * I. Slypen, S. Benck, J-P. Meulders, V. Corcalciuc* Institut de Physique Nucléaire,
More informationExperiments with gold, lead and uranium ion beams and their technical and theoretical interest.
Experiments with gold, lead and uranium ion beams and their technical and theoretical interest. (Karl-Heinz Schmidt, GSI Darmstadt) 1. The Problem of Nuclear Waste 1.1 Nuclear Reactor 1.2 Transmutation
More informationFISSION: RECENT RESEARCH AND NEW APPLICATIONS
FISSION: RECENT RESEARCH AND NEW APPLICATIONS New applications of nuclear fission Accelerator-driven systems (ADS) - Incineration of nuclear waste, - Energy production, - Research program HINDAS. Next-generation
More informationMEASUREMENTS OF PARTICULE EMISSION SPECTRA IN PROTON INDUCED REACTIONS OF INTEREST FOR THE DEVELOPMENT OF ACCELERATOR DRIVEN SYSTEMS
MEASUREMENTS OF PARTICULE EMISSION SPECTRA IN PROTON INDUCED REACTIONS OF INTEREST FOR THE DEVELOPMENT OF ACCELERATOR DRIVEN SYSTEMS N. Marie, C. Le Brun, F.R. Lecolley, J.F. Lecolley, F. Lefèbres, M.
More informationM.B. Chadwick.
LA-UR-97-1797 Title: of Nuclear Data for Fast Neutron and Proton Radiotherapy: A New ICRU Report Author(s): M.B. Chadwick Submitted to: http://lib-www.lanl.gov/la-pubs/00412577.pdf Los Alamos NATIONAL
More informationProton induced reactions on natural U at 62.9 MeV
Proton induced reactions on natural U at 62.9 MeV Arnaud Guertin, Stéphane Auduc, G. Rivière, Philippe Eudes, Ferid Haddad, Claude Lebrun, Thomas Kirchner, C. Le Brun, F.R. Lecolley, J.F. Lecolley, et
More informationNeutron multiplicity. Total radioactivity (Ci) Time after beam cut. Target A s 1min 1h 1d 1m 1y 10y 100y
0 proton 000 MeV proton 500 MeV pronto 200 MeV 0-0 25 50 75 00 25 50 75 200 225 250 Target A ' data and Mote Carlo simulations on spallation New relevant for the design of ADS reactions J.Benlliure University
More informationLight-ion production in the interaction of 96 MeV neutrons with oxygen
Light-ion production in the interaction of 96 MeV neutrons with oxygen arxiv:nucl-ex/05004v 8 Jan 2005 U. Tippawan,2, S. Pomp, A. Ataç,3, Bergenwall,4, J. Blomgren, S. Dangtip,5, A. Hildebrand, C. Johansson,
More informationBasic Studies for Transmutation (BASTRA): MUSE HINDAS
Basic Nuclear Data Activities in FP5 F Mellier (CEA, Cadarache) JP Meulders (UCL, Leuven-la la-neuve) A Mengoni (CERN, Geneva) Basic Studies for Transmutation (BASTRA): MUSE HINDAS n_tof-nd-ads ADS (Accelerator
More informationFINAL TECHNICAL REPORT
FINAL TECHNICAL REPORT CONTRACT N :FIKW-CT-2000-00031 PROJECT N : FIS5-00150 ACRONYM : HINDAS TITLE : High and Intermediate energy Nuclear Data for Accelerator-driven Systems PROJECT CO-ORDINATOR : Université
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 informationResults from the IAEA Benchmark of Spallation Models
Journal of the Korean Physical Society, Vol. 59, No. 2, August 2011, pp. 791 796 Results from the IAEA Benchmark of Spallation Models S. Leray and J. C. David CEA-Saclay, Irfu-SPhN, Gif-sur-Yvette, 91191,
More informationNeutrons For Science (NFS) at SPIRAL-2
Neutrons For Science (NFS) at SPIRAL-2 X. Ledoux 1), M. Aïche 2), G. Ban 3), G. Barreau 2), P. Baumann 4), P. Bem 5), V. Blideanu 6), J. Blomgren 7), S. Czajkowski 2), P. Dessagne 4), E. Dupont 6), T.
More informationFission Fragment characterization with FALSTAFF at NFS
EPJ Web of Conferences 42, 01001 (2013) DOI: 10.1051/ epjconf/ 20134201001 C Owned by the authors, published by EDP Sciences, 2013 Fission characterization with FALSTAFF at NFS D. Doré 1, F. Farget 2,
More informationEUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH. Letter of Intent to the ISOLDE and Neutron Time-of-Flight Committee
EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH Letter of Intent to the ISOLDE and Neutron Time-of-Flight Committee Measurement of the 235 U(n, f) cross section relative to the H(n, n)h reaction up to 1 GeV:
More informationLight-ion production in the interaction of 96 MeV neutrons with silicon
Light-ion production in the interaction of 96 MeV neutrons with silicon arxiv:nucl-ex/4117v2 1 Apr 24 U. Tippawan 1,2, S. Pomp 1, A. Ataç 1, B. Bergenwall 1, J. Blomgren 1, S. Dangtip 1,2, A. Hildebrand
More informationTracking at the LAND/R B setup on 17
3 Tracking at the LAND/R B setup on 17 the example of Ne(γ,2p)15O R. Plag*, J. Marganiec 21. Januar 2011 Dedicated to the students of LAND/R3B Outline rp process and motivation coulomb dissociation as
More informationSimulation of quasi-monoenergetic Li(p,n) neutron source up to 50 MeV proton energy
Forschungszentrum Karlsruhe in der Helmholtz-Gemeinschaft Nuclear Physics Institute Řež Simulation of quasi-monoenergetic Li(p,n) neutron source up to 50 MeV proton energy S.P. Simakov 1, P. Bém 2, V.
More informationUnfolding of neutron spectra with an experimentally determined diamond detector response function
Unfolding of neutron spectra with an experimentally determined diamond detector response function Physikalisch-Technische Bundesanstalt, D-38116 Braunschweig, Germany E-mails: Andreas.Zimbal@ptb.de, Marcel.Reginatto@ptb.de,
More informationBenchmark of Spallation Models
Progress in NUCLEAR SCIENCE and TECHNOLOGY, Vol. 2, pp.942-947 (2011) ARTICLE Benchmark of Spallation Models Jean-Christophe DAVID 1,*, Detlef FILGES 2, Franz GALLMEIER 3, Mayeen KHANDAKER 4, Alexander
More informationTHE USE OF GE DETECTORS FOR (N,XN) CROSS-SECTION MEASUREMENTS AT INTENSE AND LOW FREQUENCY PULSED NEUTRON BEAMS. Abstract
THE USE OF GE DETECTORS FOR (N,XN) CROSS-SECTION MEASUREMENTS AT INTENSE AND LOW FREQUENCY PULSED NEUTRON BEAMS Strahinja Lukic, 1 Paule Baumann, 1 Catalin Borcea, 2 Erwin Jericha, 3 Stevan Jokic, 4 Aleksandra
More informationN/Z influence on the level density parameter
EPJ Web of Conferences 88, 00030 ( 2015) DOI: 10.1051/ epjconf/ 20158800030 C Owned by the authors, published by EDP Sciences - SIF, 2015 N/Z influence on the level density parameter G. Ademard 1,L.Augey
More informationReactivity monitoring using the Area method for the subcritical VENUS-F core within the framework of the FREYA project
Reactivity monitoring using the Area method for the subcritical VENUS-F core within the framework of the FREYA project N. Marie 1, G. Lehaut 1, J.-L. Lecouey 1, A. Billebaud 2, S. Chabod 2, X. Doligez
More information(PHENS) for Active Diagnostics of Radiation Environment in Spacecraft
15th Workshop on Radiation Monitoring for the International Space Station 7-9 September 2010, University of Rome Tor Vergata Portable High-Energy Neutron Spectrometer (PHENS) for Active Diagnostics of
More informationThe heavy ion irradiation facility at KVI-CART
The heavy ion irradiation facility at KVI-CART Brian N. Jones 1, Marc-Jan van Goethem 1,2, Rob Kremers 1, Harry Kiewiet 1, Emiel van der Graaf 1, Sytze Brandenburg 1 1 University of Groningen, KVI-Center
More informationtwo-proton radioactivity discovery of two-proton radioactivity experimental results with TPC s future studies
two-proton radioactivity discovery of two-proton radioactivity experimental results with TPC s future studies Bertram Blank CEN Bordeaux-Gradignan EPS European Nuclear Physics Conference 2009 Spring meeting
More informationEXPERIMENTAL STUDY OF NEUTRON FIELDS PRODUCED IN PROTON REACTIONS WITH HEAVY TARGETS. Nuclear Physics Institute AS CR, Rez Czech Republic
EXPERIMENTAL STUDY OF NEUTRON FIELDS PRODUCED IN PROTON REACTIONS WITH HEAVY TARGETS A. Kugler, V. Wagner Nuclear Physics Institute AS CR, 25068 Rez Czech Republic I. Introduction One of important aspects
More informationICTP-IAEA Joint Workshop on Nuclear Data for Science and Technology: Medical Applications. 30 September - 4 October, 2013
2484-11 ICTP-IAEA Joint Workshop on Nuclear Data for Science and Technology: Medical Applications 30 September - 4 October, 2013 Experimental techniques (Nuclear reaction data, estimation of uncertainties)
More informationX. Ledoux and the NFS collaboration. Outline - Description of the facility - Neutron transport simulations - Letter Of Intents
X. Ledoux and the NFS collaboration Outline - Description of the facility - Neutron transport simulations - Letter Of Intents Neutrons For Science NFS is one of the two facilities of the LINAG Experimental
More informationNuclear data for advanced nuclear systems
XXII INTERNATIONAL BALDIN SEMINAR ON HIGH ENERGY PHYSICS PROBLEMS Nuclear data for advanced nuclear systems (XXII Baldin seminar) Vladimír Wagner Nuclear physics institute of CAS, 250 68 Řež, Czech Republic,
More informationSTUDY ON THE ENERGY RESPONSE OF PLASTIC SCINTILLATION DETECTOR TO MEV NEUTRONS ABSTRACT
STUDY ON THE ENERGY RESPONSE OF PLASTIC SCINTILLATION DETECTOR TO 0.75-14.75 MEV NEUTRONS Jianfu Zhang 1, 2, Xiaoping Ouyang 1, 2, Suizheng Qiu 1, Xichao Ruan 3, Jinlu Ruan 2 1 School of Nuclear Science
More informationThe Neutrons For Science facility
The Neutrons For Science facility X. Ledoux and the NFS collaboration OUTLINE Presentation Status of construction First experiments and commissioning The NFS project Part of the SPIRAL-2 project built
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 informationNeutron Detector Systems for Neutron Nuclear Data Measurements
Neutron Detector Systems for Neutron Nuclear Data Measurements Robert C. Haight * Los Alamos Neutron Science Center Los Alamos, NM 87545, USA E-mail: haight@lanl.gov Nuclear data are essential in a wide
More informationReview of ISOL-type Radioactive Beam Facilities
Review of ISOL-type Radioactive Beam Facilities, CERN Map of the nuclear landscape Outline The ISOL technique History and Geography Isotope Separation On-Line Existing facilities First generation facilities
More informationActivation Products in Proton Therapy
Activation Products in Proton Therapy Syed M. Qaim Institut für Nuklearchemie Forschungszentrum Jülich GmbH D-52425 Jülich, Germany Lecture delivered during the Workshop on Nuclear Data for Medical Applications,
More informationICTP-IAEA Joint Workshop on Nuclear Data for Science and Technology: Medical Applications. 30 September - 4 October, 2013
2484-4 ICTP-IAEA Joint Workshop on Nuclear Data for Science and Technology: Medical Applications 30 September - 4 October, 2013 Formation of Activation Products in Radiation Therapy Syed M. Qaim Forschungszentrum
More informationMEASUREMENTS OF NUCLEON-INDUCED FISSION CROSS-SECTIONS OF SEPARATED TUNGSTEN ISOTOPES AND NATURAL TUNGSTEN IN THE MEV ENERGY REGION
MEASUREMENTS OF NUCLEON-INDUCED FISSION CROSS-SECTIONS OF SEPARATED TUNGSTEN ISOTOPES AND NATURAL TUNGSTEN IN THE 50-200 MEV ENERGY REGION Eismont V.P. 1, Filatov N.P. 1, Smirnov A.N. 1, Soloviev S.M.
More informationSurrogate-reaction studies by the CENBG collaboration: status and perspectives
Surrogate-reaction studies by the CENBG collaboration: status and perspectives Beatriz Jurado, Centre d Etudes Nucleaires de Bordeaux-Gradignan (CENBG), France The CENBG collaboration M.Aiche, G. Barreau,
More informationHigh-energy neutron-induced fission cross sections in
EFNUDAT Workshop, May 2010 (Paris, France) High-energy neutron-induced fission cross sections in Pb and nat 209 Bi D. Tarrío1,*, L. Tassan Got2, L. Audouin2, I. Durán1, and C. Paradela1 on behalf of the
More informationCross-section section measurements of neutron threshold reactions in various materials
Nuclear Physics Institute, Academy of Sciences of Czech Republic Department of Nuclear Reactors, Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague Cross-section
More informationNeutron Facilities. X. Ledoux. Ganil, Caen, France
Neutron Facilities X. Ledoux Ganil, Caen, France 1 Neutron Facilities X. Ledoux Ganil, Caen, France Very Wide subject : 250 research reactors are operational 164 accelerators in the IAEA database IAEA
More informationIntegral of--nuclear plus interference components. of the elastic scattering cross section. Sum of binary (p,n ) and (p,x) reactions
EVALUATION OF p + 3Si CROSS SECTIONS FOR THE ENERGY RANGE 1 to 15 MeV M. B. Chadwick and P. G. Young 1 July 1997 This evaluation provides a. complete representation of the nuclear data needed for transport,
More informationdiscovery 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 informationFast neutron inelastic scattering Roland Beyer, Forschungszentrum Dresden-Rossendorf
Fast neutron inelastic scattering Roland Beyer, Forschungszentrum Dresden-Rossendorf Institute of Radiation Physics Roland Beyer www.fzd.de Member of the Leibniz Association Data needs for transmutation
More informationHiRA: Science and Design Considerations
HiRA: Science and Design Considerations Scientific Program: Astrophysics: Transfer reactions Resonance spectroscopy Nuclear Structure: Inelastic scattering Transfer reactions Resonance spectroscopy Breakup
More informationBenchmark of Spallation Models. Introduction. Sylvie LERAY. CEA/Saclay, IRFU/SPhN. Sylvie Leray (CEA/Saclay) AccApp09, Vienna, May 4-8,
Benchmark of Spallation Models Introduction Sylvie LERAY CEA/Saclay, IRFU/SPhN Sylvie Leray (CEA/Saclay) AccApp09, Vienna, May 4-8, 2009 1 Spallation reaction applications Spallation neutron sources ADS
More informationStatus Report of the NFS collaboration
Status Report of the NFS collaboration TITLE of the Project: Neutrons For Science (NFS) Spokespersons (maximum 3) with one corresponding spokesperson: Xavier Ledoux, CEA/DIF/DPTA/SPN Bruyères-le-Châtel,
More informationELASTIC NEUTRON SCATTERING STUDIES AT 96 MeV ON ELEMENTS OF INTEREST FOR TRANSMUTATION
ELASTIC NEUTRON SCATTERING STUDIES AT 96 MeV ON ELEMENTS OF INTEREST FOR TRANSMUTATION 1, J. Blomgren 1, M. Hayashi 1,4, J. Klug 1,5, P. Mermod 1, L. Nilsson 1, S. Pomp 1, A. Öhrn 1, A.V. Prokofiev 2,
More informationMEASUREMENTS OF (N, XN) CROSS SECTIONS FOR HYBRID SYSTEMS
MEASUREMENTS OF (N, XN) CROSS SECTIONS FOR HYBRID SYSTEMS M. Kerveno, P. Baumann, A. Nachab, G. Rudolf IReS - Strasbourg (IN2P3/CNRS), France A. Pavlik Institut für Isotopenforschung und Kernphysik - Wien,
More informationStudy and comparison of the decay modes of the systems formed in the reactions
CNR*11 Third International Workshop on Compound Nuclear Reactions and Related Topics September 19-23, 2011 Prague Study and comparison of the decay modes of the systems formed in the reactions 78 Kr+ 40
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 informationThe Large Area Telescope on-board of the Fermi Gamma-Ray Space Telescope Mission
The Large Area Telescope on-board of the Fermi Gamma-Ray Space Telescope Mission 1 Outline Mainly from 2009 ApJ 697 1071 The Pair Conversion Telescope The Large Area Telescope Charged Background and Events
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 informationFast-Neutron Production via Break-Up of Deuterons and Fast-Neutron Dosimetry
Fast-Neutron Production via Break-Up of Deuterons and Fast-Neutron Dosimetry F. Gutermuth *, S. Beceiro, H. Emling, G. Fehrenbacher, E. Kozlova, T. Radon, T. Aumann, T. Le Bleis, K. Boretzky, H. Johansson,
More informationLA-UR-01-5631 Approved for public release; distribution is unlimited. Title: Development and Validation of the 7 Li(p,n) Nuclear Data Library and Its Application in Monitoring of Intermediate Energy Neutrons
More informationNuclear reactions studies at NFS for improved nuclear data for science and technology
Nuclear reactions studies at NFS for improved nuclear data for science and technology Stephan Pomp stephan.pomp@physics.uu.se Department of physics and astronomy Uppsala University Spiral2 week, November
More informationInvestigating the intra-nuclear cascade process using the reaction 136 Xe on deuterium at 500 AMeV
Investigating the intra-nuclear cascade process using the reaction Xe on deuterium at 500 AMeV J.A Alcántara-Núñez 1), J. Benlliure 1), D. Perez Loureiro 1) and the S184 Collaboration 1) Universidade de
More informationEnergy response for high-energy neutrons of multi-functional electronic personal dosemeter
Energy response for high-energy neutrons of multi-functional electronic personal dosemeter T. Nunomiya 1, T. Ishikura 1, O. Ueda 1, N. Tsujimura 2,, M. Sasaki 2,, T. Nakamura 1,2 1 Fuji Electric Systems
More informationNUCLEAR EMISSIONS FROM TITANIUM HYDRIDE/DEUTERIDE INDUCED BY POWERFUL PICOSECOND LASER BEAM
NUCLEAR EMISSIONS FROM TITANIUM HYDRIDE/DEUTERIDE INDUCED BY POWERFUL PICOSECOND LASER BEAM A. S. ROUSSETSKI P.N. Lebedev Physical Institute Russian Academy of Sciences, 3 Leninsky prospect, 119991 Moscow,
More informationNeutron-Induced Reactions Investigations in the Neutrons Energy Range up to 16 MeV
NUCLEAR THEORY, Vol. 33 (2014) eds. A.I. Georgieva, N. Minkov, Heron Press, Sofia Neutron-Induced Reactions Investigations in the Neutrons Energy Range up to 16 MeV R. Avetisyan, R. Avagyan, G. Bazoyan,
More informationR. P. Redwine. Bates Linear Accelerator Center Laboratory for Nuclear Science Department of Physics Massachusetts Institute of Technology
Pion Physics in the Meson Factory Era R. P. Redwine Bates Linear Accelerator Center Laboratory for Nuclear Science Department of Physics Massachusetts Institute of Technology Bates Symposium 1 Meson Factories
More informationHIRA CSI DETECTOR RESPONSE TO LOW ENERGY PROTONS
HIRA CSI DETECTOR RESPONSE TO LOW ENERGY PROTONS Chelsey Morien Ursinus College Collegeville, PA 09 Aug 07 The High Resolution Array Each of the 20 identical telescopes can be individually placed and aligned,
More informationPoS(FNDA2006)016. A New Neutron Beam Facility at TSL. Alexander V. Prokofiev *, Olle Byström, Curt Ekström, Volker Ziemann
Alexander V. Prokofiev *, Olle Byström, Curt Ekström, Volker Ziemann The Svedberg Laboratory, Uppsala University Box 533, S-751 21 Uppsala, Sweden E-mail: Alexander.Prokofiev@tsl.uu.se Jan Blomgren, Stephan
More informationLow-Energy Photonuclear Reactions A Review
Low-Energy Photonuclear Reactions A Review B.L. Berman Department of Physics The George Washington University Washington, DC 20052, USA International Topical Meeting on Nuclear Research Applications and
More informationFirst steps towards a target laboratory at GANIL
First steps towards a target laboratory at GANIL C. Stodel, G. Frémont, G. Auger, C. Spitaels To cite this version: C. Stodel, G. Frémont, G. Auger, C. Spitaels. First steps towards a target laboratory
More informationin2p , version 1-28 Nov 2008
Author manuscript, published in "Japanese French Symposium - New paradigms in Nuclear Physics, Paris : France (28)" DOI : 1.1142/S21831391444 November 23, 28 21:1 WSPC/INSTRUCTION FILE oliveira International
More informationEXPERIMENTAL AND CALCULATED NEUTRON PRODUCTION BY DEUTERONS IMPINGING ON BE, C AND U THICK TARGETS (17, 20, 28, 80, 160 AND 200 MEV)
EXPERIMENTAL AND CALCULATED NEUTRON PRODUCTION BY DEUTERONS IMPINGING ON BE, C AND U THICK TARGETS (17, 20, 28, 80, 160 AND 200 MEV) N. Pauwels, F. Clapier, J. Proust Institut de Physique Nucléaire d Orsay
More informationABC Math Student Copy
Page 1 of 17 Physics Week 16(Sem. ) Name The Nuclear Chapter Summary Nuclear Structure Atoms consist of electrons in orbit about a central nucleus. The electron orbits are quantum mechanical in nature.
More informationJosé Antonio Briz Monago, M. Carmona-Gallardo and. M.J.G. Borge, A. Perea, O. Tengblad, M. Turrión
GEANT4 SIMULATIONS FOR THE R3B CALORIMETER José Antonio Briz Monago, M. Carmona-Gallardo and M.J.G. Borge, A. Perea, O. Tengblad, M. Turrión Outline Introduction: FAIR at GSI (Germany) R3B Experiment Requirements
More informationDetekce a spektrometrie neutronů. neutron detection and spectroscopy
Detekce a spektrometrie neutronů neutron detection and spectroscopy 1. Slow neutrons 2. Fast neutrons 1 1. Slow neutrons neutron kinetic energy E a) charged particles are produced, protons, α particle,
More informationTotal fission cross section in proton-induced reactions on 181 Ta measured in inverse kinematics
Total fission cross section in proton-induced reactions on 181 Ta measured in inverse kinematics Yassid Ayyad Universidad de Santiago de Compostela Subactinides fission cross section Pb, W and Ta as a
More informationHigh-spin studies and nuclear structure in three semi-magic regions of the nuclide chart High-seniority states in Sn isotopes
High-spin studies and nuclear structure in three semi-magic regions of the nuclide chart High-seniority states in Sn isotopes Outline: Alain Astier, CSNSM Orsay, France Motivations Experimental conditions
More informationSPIRAL-2 FOR NEUTRON PRODUCTION
SPIRAL-2 FOR NEUTRON PRODUCTION X. Ledoux and the NFS collaboration Outline The SPIRAL-2 facility The Neutrons For Science Facility OUTLINE SPIRAL-2 The Neutrons For Science facility The SPIRAL-2 project
More informationNuclear waste management
Nuclear waste management Permanent staff : G. Ban, F-R. Lecolley, J-L. Lecouey, G. Lehaut, N. Marie-Nourry, J-C. Steckmeyer Emeritus : J-F. Lecolley PhD student: H-E. Thyebault Collaborations : LPSC Grenoble,
More informationSpectroscopy of 252No to Investigate its K-isomer
Spectroscopy of to Investigate its K-isomer Edward Parr Motivation in Superheavies PROTONS Single Particle Energy (MeV) Single Particle Energy (MeV) NEUTRONS Next shell gaps predicted for Superheavy spherical
More informationESS. Get Involved! Patrik Carlsson. Allen Weeks
ESS Get Involved! Patrik Carlsson Allen Weeks What is ESS? A European facility for materials research Lund 2025: The European Spallation Source (5 MW) One of Europe's largest planned research infrastructures
More information(10%) (c) What other peaks can appear in the pulse-height spectrum if the detector were not small? Give a sketch and explain briefly.
Sample questions for Quiz 3, 22.101 (Fall 2006) Following questions were taken from quizzes given in previous years by S. Yip. They are meant to give you an idea of the kind of questions (what was expected
More informationThe Ring Branch. Nuclear Reactions at. Mass- and Lifetime Measurements. off Exotic Nuclei. Internal Targets. Electron and p. Experiments: Scattering
stochastic cooling Exotic nuclei from Super-FRS Degrader for fast slowing down The Ring Branch TOF Detector MCPs E anode ion B CR Electron cooler NESR secondary electrons Experiments: Mass- and Lifetime
More informationAverage multiplicities of particles emitted in the h-a reactions
Average multiplicities of particles emitted in the h-a reactions Aatos Heikkinen aatos.heikkinen@cern.ch Geant4 Hadronic Physics Working Group Meeting October 22, 2007 Group Meeting, October 22nd, 2007
More informationElastic Recoil Detection Method using DT Neutrons for Hydrogen Isotope Analysis in Fusion Materials. Abstract
Elastic Recoil Detection Method using DT Neutrons for Hydrogen Isotope Analysis in Fusion Materials Naoyoshi Kubota, Kentaro Ochiai, Keitaro Kondo 2 and Takeo Nishitani. :Japan Atomic Energy Research Institute,
More informationNeutron Metrology Activities at CIAE (2009~2010)
Neutron Metrology Activities at CIAE (2009~2010) Ionizing Radiation Metrology Division China Institute of Atomic Energy (P.O.Box 275(20), Beijing 102413, China) 1. Neutron calibration fields So far the
More information(Multi-)nucleon transfer in the reactions 16 O, 3 32 S Pb
Journal of Physics: Conference Series Related content (Multi-)nucleon transfer in the reactions 16 O, 3 32 S + 208 Pb To cite this article: M Evers et al 2013 J. Phys.: Conf. Ser. 420 012129 - Quantum
More informationThe LIONS experimental programme
The LIONS experimental programme and its relevance for nuclear science and applications, or How can NFS help fusion? Alexander V. Prokofiev 1,*, Diego Tarrío 1, Marc O. Fregeau 2, Xavier Ledoux 2, and
More informationDipole Response of Exotic Nuclei and Symmetry Energy Experiments at the LAND R 3 B Setup
Dipole Response of Exotic Nuclei and Symmetry Energy Experiments at the LAND R 3 B Setup Dominic Rossi for the LAND collaboration GSI Helmholtzzentrum für Schwerionenforschung GmbH D 64291 Darmstadt, Germany
More informationNeutrons For Science (NFS) at SPIRAL-2 (Part II: pulsed neutron beam)
Neutrons For Science (NFS) at SPIRAL-2 (Part II: pulsed neutron beam) X. Ledoux 1 and D. Ridikas 2 1) CEA/DIF/DPTA/SPN, BP 12, 91680 Bruyères-le-Châtel, France 2) CEA/DSM/DAPNIA/SPhN, CEA Saclay, 91191
More informationThe Neutrons for Science Facility at SPIRAL2
The Neutrons for Science Facility at SPIRAL2 X. Ledoux, M. Aïche, M. Avrigeanu, V. Avrigeanu, L. Audouin et al. Citation: AIP Conf. Proc. 1412, 55 (2011); doi: 10.1063/1.3665296 View online: http://dx.doi.org/10.1063/1.3665296
More informationNeutron 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 informationNeutrons For Science: A neutron SPIRAL-2
Neutrons For Science: A neutron facility @ SPIRAL-2 X. Ledoux and the NFS collaboration The SPIRAL-2 project NFS description and characteristics Buildings design Physics case SPIRAL-2 deuterons 40MeV;
More informationNeutron Irradiation Facility of the. N.C.S.R. Demokritos. Tandem
Neutron Irradiation Facility of the N.C.S.R. Demokritos Tandem Michail Axiotis Tandem Accelerator Laboratory, N.C.S.R. Demokritos The 5.5 MV VdG Tandem accelerator @ I.N.P.P. 5.5 MV Tandem Accelerator
More informationCalculations of Neutron Yield and Gamma Rays Intensity by GEANT4
Armenian Journal of Physics, 2016, vol. 9, issue 4, pp. 315-323 Calculations of Neutron Yield and Gamma Rays Intensity by GEANT4 R. Avagyan, R. Avetisyan, V. Ivanyan*, I. Kerobyan A.I. Alikhanyan National
More informationUpdate on Calibration Studies of the Canadian High-Energy Neutron Spectrometry System (CHENSS)
Update on Calibration Studies of the Canadian High-Energy Neutron Spectrometry System (CHENSS) K. Garrow 1, B.J. Lewis 2, L.G.I. Bennett 2, M.B. Smith, 1 H. Ing, 1 R. Nolte, 3 S. Röttger, R 3 R. Smit 4
More informationFrench-Ukrainian Workshop on the instrumentation developments for high energy physics. ProRad. An electron-proton scattering experiment
French-Ukrainian Workshop on the instrumentation developments for high energy physics ProRad An electron-proton scattering experiment @ Mostafa HOBALLAH on behalf of the ProRad collaboration hoballah@ipno.in2p3.fr
More informationLight ion recoil detector
Light ion recoil detector Overall design The detector for light (target-like) particles is a substantial part of the R3B setup. It allows registration of recoils in coincidence with the heavy fragments,
More informationAt low excitation, the compound nucleus de-excites by statistical emission of light particles (n,p,α)
Does the α cluster structure in light nuclei persist through the fusion process? Justin Vadas, T.K. Steinbach, J. Schmidt, V. Singh, S. Hudan, R.T. de Souza; Indiana University L. Baby, S. Kuvin, I. Wiedenhover;
More informationTowards 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 informationCalibration of the Modular Neutron Array (MoNA)
Calibration of the Modular Neutron Array (MoNA) Robert Pepin Gonzaga University ~1~ Calibration of the Modular Neutron Array (MoNA): Figure 1 - A rendering of the Modular Neutron Array In recent years
More informationExperimental Investigation of Few-Nucleon Dynamics at Medium Energies
Experimental Investigation of Few-Nucleon Dynamics at Medium Energies by Ghanshyam Khatri 1 \ 22 Outline Introduction Three-body (3N) force Experimental tools BINA Detector and it s status at CCB (Krakow)
More informationThermodynamical coordinates of excited nuclear systems:
Thermodynamical coordinates of excited nuclear systems: 4,48 Ca + 58,64 Ni and 4 Ca + 58 Fe reactions M. Bruno, F. Cannata, M.D Agostino, J. De Sanctis, S. Fabbri, E.Geraci, B. Guiot, G.Vannini Department
More informationDISCLAIMER. and opinions of authors e x p d herein do not necessarily state or reflect those of the United States Government or any agency thereof.
DISCLAIMER 2 0 34) This report was prepared as an account of work sponsored by an agency of the United States Government. Neither the United States Government nor any agency thereof, nor any of their employees,
More information