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Session JC Nuclear Reaction Models Room: Empire East at 10:30 AM Ormand, W. A Modern Code System for Hauser-Feshbach Modeling Based on a Monte Carlo Framework Bouland, O. The Impact of Intermediate Structure on the Average Fission Cross Section Calculations Avrigeanu, M. Unitary Account of Nuclear Reaction Mechanisms for Deuteron-Induced Activation at Low and Medium Energies Guo, H. Application of the Continuum Discretized Coupled Channels Method to Nucleon-Induced Reactions on 6,7 Li for Energies up to 150 MeV Session JD Space Applications Room: Empire West at 10:30 AM Wender, S. Accelerator Testing for Neutron-Induced Failures in Semiconductor Devices Watanabe, Y. Nuclear Reaction Models Responsible for Simulation of Neutron-Induced Soft Errors in Microelectronics Oishi, K. Benchmark Experiment of Dose Rate Distribution Around Gamma Knife Medical Apparatus Nichols, A. Nuclear Data Requirements for Medical Applications - Recent Contributions and Future Requirements as Formulated Under the Auspices of the International Atomic Energy Agency Session JE Fusion Room: Central Park West at 10:30 AM Fischer, U. The Activities of the European Consortium on Nuclear Data Development and Analysis for Fusion Avrigeanu, V. Consistent Account of Fast Neutron Induced α-particle Emission Forrest, R. IAEA Coordinated Research Project: FENDL-3 Sawan, M. Benchmarking of the FENDL-3 Neutron Cross-Section Data Starter Library for Fusion Applications Session JF Neutron Cross Section Measurements Room: Central Park East at 10:30 AM Nayak, B. Measurement of Neutron Induced Fission Cross Sections by Surrogate Methods Ducasse, Q. Neutron-induced Capture Cross Sections of Actinides via the Surrogate-Reaction Method Chiba, S. Surrogate Research at JAEA/Tokyo Tech Cizewski, J. Validating (d,pγ ) as a Surrogate for Neutron Capture on Unstable Nuclei Session KA Dissemination and International Colaboration Room: Met East at 1:30 PM Dupont, E. Working Party on International Nuclear Data Evaluation Co-operation (WPEC) Beck, B. International Effort to Define a New Nuclear Data Structure Otsuka, N. Toward More Complete and Accurate Experimental Nuclear Reaction Data Library (EXFOR) - International Collaboration Between Nuclear Reaction Data Centres (NRDC) Patel, N. Structure for Storing Properties of Particles (POP) 10
Session KC Evaluated Nuclear Data Libraries Room: Empire East at 1:30 PM Trkov, A. Current Status of Evaluated Nuclear Data of Mn-55 Kunieda, S. R-matrix Analysis for n+ 16 O Cross-Sections up to En = 6.0 MeV with Covariance Iwamoto, O. Progress in Developing Nuclear Reaction Calculation Code CCONE for Higher Energy Nuclear Data Evaluation Blokhin, A. Development of the Fission-Product Yield Library for BROND-3 Session KD Fission Yields Room: Empire West at 1:30 PM Mills, R. Uncertainty Propagation of Fission Product Yield Data in Spent Fuel Inventory Calculations Kim, G. Mass Yield Distribution in the 45- and 80-MeV Bremsstrahlung-Induced Fission of 232 Th Pentilla, H. Independent Isotopic Product Yields in 25 MeV and 50 MeV Charged Particle Induced Fission of 238 U and 232 Th Tovesson, F. SPIDER: A New Instrument for Fission Fragment Yield Measurements Session KE Integral Experiments Room: Central Park West at 1:30 PM Bess, J. What If Lady Godiva Was Wrong? Ene, D. Shielding Design Calculations for the ESS Target Station High Activated Components Hammer, B. Distribution of Radionuclides in MEGAPIE, a Proton Irradiated LBE Target Jansky, B. Measured and Calculated Iron Filtered Neutron Spectra Using Different Data Libraries for Calculation Session KF Neutron Cross Section Measurements Room: Central Park East at 1:30 PM Wallner, A. Neutron-Induced Reactions on U and Th - New Cross-Section Measurements via AMS Youinou, G. MANTRA: An Integral Reactor Physics Experiment to Infer the Capture Cross-Sections of Actinides and Fission Products in Fast and Epithermal Neutron Spectra Hori, J. Measurements of Capture Gamma Rays from the Neutron Resonances of 74 Se and 77 Se at J- PARC/MLF/ANNRI Lee, J. Measurements of Thermal Neutron Capture Cross Sections of 136 Ce, 144 Sm, 156,158 Dy, and 168 Yb Session LA Neutron Cross Section Measurements Room: Met East at 3:30 PM Lestone, J. Plutonium and Uranium Prompt-Fission-Neutron Energy Spectra (PFNS) from the Analysis of Neutron Data from two US Nuclear Explosions Williams, D. A New Measurement of the Neutron Capture Cross Section of 235 U Below 5 keV Ullmann, J. Neutron Capture Cross Sections and Gamma Emission Spectra from Neutron Capture on 234,236,238 U measured with DANCE. Laptev, A. Neutron-Induced Fission Cross Section Measurements at LANSCE Bielewicz, M. Measurements relevant to high energy neutron spectrum (> 10 MeV) by using Yttrium threshold detectors 11
Page 1 and 2: ND2013 2013 International Nuclear D
Page 3 and 4: Session BF Evaluated Nuclear Data L
Page 5 and 6: Session DD Nuclear Structure and De
Page 7 and 8: Hale, G. n+ 12 C Cross Sections fro
Page 9: Domula, A. New Nuclear Structure an
Page 13 and 14: MacCormick, M. Survey and Evaluatio
Page 15 and 16: ments. Ivanova, T. Uncertainty Asse
Page 17 and 18: Arnold, C. Precision Velocity Measu
Page 19 and 20: 19 Abridged Agenda Sunday March 4,
Page 21 and 22: 21 Tuesday March 5, 2013 Time Met E
Page 23 and 24: 23 Thursday March 7, 2013 Time Met
Page 26 and 27: Book of Abstracts Session AA ND2013
Page 28 and 29: multi-foil Parallel Plate Avalanche
Page 30 and 31: A Regional Coupled-channel Dispersi
Page 32 and 33: show the versatility of the code in
Page 34 and 35: [h] Table 1: Comparison of all the
Page 36 and 37: step was to determine which detecto
Page 38 and 39: In an effort to maintain the qualit
Page 40 and 41: Advances in Reactor Physics Linking
Page 42 and 43: sponsored the work presented in thi
Page 44 and 45: A revolutionary nuclear data system
Page 46 and 47: done in Ref. [1]. We demonstrate th
Page 48 and 49: CD 4 2:40 PM Development of a Syste
Page 50 and 51: with a central cavity where small s
Page 52 and 53: C. Arnold, E. Bond, T. Bredeweg, M.
Page 54 and 55: DA 3 4:20 PM Characterization and P
Page 56 and 57: detectors at the newly constructed
Page 58 and 59: Lead and lead-based alloys are - am
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of the setup. One option explored i
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DC 2 4:00 PM Improved Capture Gamma
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DC 5 5:00 PM Thermal Neutron Cross
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M.R. Gilbert, L.W. Packer, S. Lille
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Correlations Between Nuclear Charge
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Community’s 7th Framework Program
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we achieve very good separation of
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analysis of neutron leakage spectru
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a lower nuclear temperature than th
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Tungsten occurs naturally in five i
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for the combined use of integral ex
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in XUNDL and bibliographic informat
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former case, more realistic covaria
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WInfried Zwermann, Kiril Velkov, An
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LA-UR-12-23712 The ENDF/B-VII.1 [1,
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comparison of results C/E of fissio
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Session GA Evaluated Nuclear Data L
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Session GC accelerator applications
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Session GD Antineutrinos Tuesday Ma
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M. Fallot, S. Cormon, M.Estienne, V
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for extraction of very rare isotope
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and neutron multiplicity, informati
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as Monte Carlo simulations, and inc
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on its surface. The amplification t
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direction was recently used at n TO
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were chemically separated and the 2
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Strontium-82 Production at ARRONAX
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A. Guertin, C. Duchemin, F. Haddad,
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expected via an (n,γ) reaction. Pr
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Shinsuke Nakayama, Shouhei Araki, Y
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specific feature of the procedure e
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good timing characteristics.Example
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Materials and Measurements, Retiese
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derive reliable covariances from ta
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Concerns about the limits of worldw
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Accurate and reliable nuclear data
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Facility (HRIBF) at Oak Ridge Natio
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CALIFA, a Calorimeter for the R3B/F
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a modified Lorentzian model (MLO) o
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enchmark for existing atomic mass p
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A significant breakthrough in our t
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and the neutron and proton emission
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horizontal plane, the measured posi
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The high precision of recent measur
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Session JF Neutron Cross Section Me
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Alamos National Laboratory, Los Ala
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During more than four decades since
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KC 2 2:00 PM R-matrix Analysis for
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new covariance contributions to the
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importance in nuclear technology, a
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source SINQ (Swiss Spallation Neutr
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KF 2 2:00 PM MANTRA: An Integral Re
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J. P. Lestone, E. F. Shores Los Ala
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LA 5 5:00 PM Measurements relevant
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elow the neutron separation energy
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The A = 130 Solar-System r-process
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espectively, and identified approxi
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W. Zwermann Gesellschaft fuer Anlag
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LC 5 5:00 PM Uncertainty Study of N
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solving the quantum three-body prob
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Session LE Evaluated Nuclear Data L
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LE 5 5:00 PM Method of Best Represe
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for 89 fission products (representi
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Impact of the Energy Dependent DDXS
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from non 1/v behavior of nuclei. Mo
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evaluation (including covariances)
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system without isotope separation.
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NC 3 11:20 AM Propagation of Nuclea
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Results of the first complete compi
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Arjan Koning and Dimitri Rochman Nu
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calculating their mathematical mome
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The 33 S(n,α) cross section is of
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OA 2 2:00 PM Event-by-Event Fission
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available for ENDF/B-VII. The obser
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egions: the resolved resonances ran
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y the screening potential predicted
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[1] Y. Kojima et al., Nucl. Instr.
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y the emitted neutron. The Versatil
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enchmarking, the excitation functio
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PA 1 3:30 PM Investigation of Neutr
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as well as for a variety of Minor A
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Society, Vol. 59, No. 2, August 201
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A. Hermanne, R. Adam-Rebeles Cyclot
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We measured the isomeric yield rati
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the trends in the experimental data
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However, experiments often measure
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Statistical description of the gamm
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fragments formed are highly neutron
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F. Farget, J. Pancin GANIL, Caen, F
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ZPR-6/10 cores were applied as comp
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each nucleus in agreement with unce
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atios) is performed. In relation to
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school in science or engineering. I
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programs demanding only one compuls
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gamma-ray spectra will be theoretic
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RA 3 11:20 AM A Microscopic Theory
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Laboratory, Oak Ridge, Tenn., Novem
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Session RD Safeguards and Security
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Seeking Reproducibility in Fast Cri
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RE 4 11:40 AM Verification of Curre
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that a lot of them generally descri
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R. Hirschi, A. Hungerford, G. Magko
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- a density of levels too low for w
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the MONTEBURNS(1.0)-MCNP5-ORIGEN(2.
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The Nuclear Science References (NSR
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and applications using statistical
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Shielding objects are assembled fro
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The knowledge of neutron-induced re
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thus for the second time after the
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the global children health and cons
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Lawrence Livermore National Laborat
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The Russian Nuclear Data Library fo
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OECD Nuclear Energy Agency consider
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For experimental determination of t
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The European Activation SYstem has
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Neutron capture measurements of dys
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[1] H. Penttilä, P. Karvonen, T. E
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Measurement of Activation Cross Sec
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PR 66 Processing and Validation of
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law of the temperature ratio (RT =
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PR 74 Resonance Analysis of the 233
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Study of Various Potentials in Heav
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experimental data and for the produ
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fuel cycle impose tight requirement
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they do not satisfy (for example, b
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Differential Cross Sections for the
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extends the previous evaluation and
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various benchmark tests. The mainly
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PR 104 Evaluations for n+ 54,56,57,
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PR 109 Recent LAQGSM Developments a
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PR 113 Modelling of Spallation Sour
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Jagiellonian University, Reymonta 4
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PR 120 Coupled-Channel Models of Di
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PR 124 Nuclear Data Evaluation and
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physicist. - There is no perfect se
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Manturov, M.N. Nikolaev, A.M. Tsibo
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Vasiliev, W. Wieselquist and H. Fer
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Author Index 1, Vojtěch Rypar, PR
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HF 5, KD 4, LA 3, LA 6, LA 7, LA 8,
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Dunn, M. E., BF 4, RC 3 Dupont, Emm
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Gulliford, Jim, CE 1 Gunsing, Frank
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Kahl, David, HD 7 Kahler, A. C., CA
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Lehaut, G., PD 6 Leinweber, Greg, L
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Munkhsaikhan, J., HC 7 Mura, Luis F
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Prael, Richard E., PE 5 Praena, Jav
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Sheets, S., CF 2 Shen, Qingbiao, PC
Page 352 and 353:
Typel, S., JA 3 Tyutyunnikov, S., L
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