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F. da Cruz, D. Total Monte-Carlo Method Applied to a Pressurized Water Reactor Fuel Assembly - Quantification of Uncertainties due to 235,238 U, 239,240,241 Pu and Fission Products Nuclear Data Uncertainties Session ND Beta delayed neutrons Room: Empire West at 10:30 AM Chiba, G. Sensitivity Analysis for Reactor Stable Period Induced by Positive Reactivity Using One-Point Adjoint Kinetic Equation Singh, B. First Compilation and Evaluation of Beta-Delayed Neutron Emission Probabilities and Associated Half-lives in the Non-Fission Region (A ≤ 72) Miernik, K. Beta-decay Study of Neutron-Rich Isotopes 93 Br and 93 Kr Tain, J. New Beta-Delayed Neutron Measurements in the Light-Mass Fission Group Session NE Benchmark and Testing Room: Central Park West at 10:30 AM Sublet, J. TENDL-2012 Processing, Verification and Validation Steps Arcilla, R. Use of a Continuous Integration and Deployment Software to Automate Nuclear Data Verification and Validation Cornock, M. Benchmarking of ENDF/B-VII and JENDL-4.0 in the Fast Neutron Range Peneliau, Y. 239 Pu Prompt Fission Neutron Spectra Impact on a Set of Criticality and Experimental Reactors Benchmarks Session NF Medical Applications Room: Central Park East at 10:30 AM Ferrari, A. The FLUKA Code: Developments and Challenges for High Energy and Medical Applications Sakama, M. Correlation Between Asian Dust (yellow dust) and Specific Radioactivities of Fission Products Including in Airborne Samples in Tokushima, Shikoku Island, Japan, due to the Fukushima Nuclear Accident Porras, I. 33 S(n,α) Cross Section Measurement at n TOF: Implications in Neutron Capture Therapy Fassbender, M. Production of High Specific Activity 186 Re for Cancer Therapy Using nat,186 WO3 Targets in a Proton Beam Session OA Fission Room: Met East at 1:30 PM Talou, P. Monte Carlo Hauser-Feshbach Calculations of Prompt Fission Neutrons and Gamma Rays Vogt, R. Event-by-Event Fission Modeling of Prompt Neutrons and Photons from Neutron-Induced and Spontaneous Fission with FREYA Litaize, O. Investigation of n+ 238 U Fission Observables Nishio, K. Study for Heavy-Ion Induced Fission for the Heavy Element Synthesis Session OB assimilation Room: Met West at 1:30 PM Palmiotti, G. Progress on Consistent Nuclear Data Assimilation Hoblit, S. Towards unified reaction cross sections through assimilation of integral and differential experi- 14
ments. Ivanova, T. Uncertainty Assessment for fast Reactors Based on Nuclear Data Adjustment Archier, P. New JEFF-3.2 Sodium Neutron Induced Cross-Sections Evaluation for Neutron Fast Reactors Applications: from 0 to 20 MeV Session OC Nuclear Astrophysics Room: Empire East at 1:30 PM Gondolo, P. Wanted! Nuclear Data for Dark Matter Astrophysics Altstadt, S. Experimental Studies of the 13,14 B(n, γ) Rates for Nucleosynthesis Towards the r process Paris, M. R-matrix Analysis of Reactions in the 9 B Compound System Kasagi, J. Astrophysical Sbare(E) Factor of the 6 Li+d and 7 Li+p Reactions Session OD Nuclear Structure and Decay Room: Empire West at 1:30 PM Rubio, B. Determination of absolute Gamow Teller transition probabilities in exotic fp-shell nuclei Kojima, Y. Half-life Measurements of Excited Levels in Fission Products Around a Mass Number of 150 Kroll, J. Scissors Mode Strength in Rare Earth Nuclei Studied from (n,γ) reaction Mougeot, X. Evidence for the Exchange Effect in Low-Energy Beta Decays Session OE Beta delayed neutrons Room: Central Park West at 1:30 PM Grzywacz, R. Beta Delayed Neutron Spectroscopy on the r-process Path McCutchan, E. A New Approach to Estimating the Probability for β Delayed Neutron Emission Scielzo, N. Beta-delayed Neutron Spectroscopy with Trapped Ions Caballero-Folch, R. New Measurements in the Neutron Rich Region Around N=126 for β-decay and βdelayed Neutron Emission Data at GSI-FRS Session OF Cross Section Measurements Room: Central Park East at 1:30 PM Ruan, X. Nuclear Data Measurement Activities at CIAE Gustavsson, C. Measurements of Inelastic Neutron Scattering from Carbon, Iron, Yttrium and Lead at 96 MeV Utsunomiya, H. Partial Photoneutron Cross Sections for 207,208 Pb Siem, S. Experimental Level Densities and Gamma Strength Functions with the Oslo Method Session PA Neutron Cross Section Measurements Room: Met East at 3:30 PM Guerrero, C. Investigation of Neutron-Induced Reactions at n TOF: Overview of the 2009-2012 Experimental <strong>Program</strong> Fraval, K. Analysis of 241 Am(n,γ) Cross Section with C6D6 Detectors at the n TOF facility (CERN) Mosby, S. Neutron Capture Cross Section of 239 Pu Wright, T. High-precision measurement of the 238 U(n,γ) cross section with the Total Absorption Calorimeter (TAC) at nTOF, CERN 15
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 and 10: Domula, A. New Nuclear Structure an
Page 11 and 12: Session KC Evaluated Nuclear Data L
Page 13: MacCormick, M. Survey and Evaluatio
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
Page 60 and 61: of the setup. One option explored i
Page 62 and 63: 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 =
Page 300 and 301:
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
Page 310 and 311:
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
Page 340 and 341:
Gulliford, Jim, CE 1 Gunsing, Frank
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Kahl, David, HD 7 Kahler, A. C., CA
Page 344 and 345:
Lehaut, G., PD 6 Leinweber, Greg, L
Page 346 and 347:
Munkhsaikhan, J., HC 7 Mura, Luis F
Page 348 and 349:
Prael, Richard E., PE 5 Praena, Jav
Page 350 and 351:
Sheets, S., CF 2 Shen, Qingbiao, PC
Page 352 and 353:
Typel, S., JA 3 Tyutyunnikov, S., L
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