Druck-Materie 20b.qxd - JUWEL - Forschungszentrum Jülich

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List of participants Ansell, Stuart s.ansell@rl.ac.uk G39, ISIS, Rutherford Appleton Laboratories; Chilton, Didcot OX11 0QX; UK Bauer, Günter g.bauer@fz-juelich.de Institut für Festkörperforschung, Forschungszentrum Jülich; DE-52425 Jülich GERMANY Bayer, Norbert n.bayer@fz-juelich.de Zentralabteilung Technologie, Forschungszentrum Jülich; DE-52425 Jülich GERMANY Bennington, Stephen s.m.bennington@rl.ac.uk ISIS Facility, Rutherford Appleton Laboratories; Chilton, Didcot OX11 0QX; UK Bernnat, Wolfgang bernnat@ike.uni-stuttgart.de IKE, Universität Stuttgart; Pfaffenwaldring 31, DE-70569 Stuttgart, GERMANY Butzek, Michael m.butzek@fz-juelich.de Zentralabteilung Technologie, Forschungszentrum Jülich; DE-52425 Jülich GERMANY Carpenter, John M. Jmcarpenter@anl.gov Argonne National Laboratory, 9700 S. Cass Avenue, Bldg. 360; Argonne, IL 60439; USA Clausen, Kurt kurt.clausen@psi.ch Paul-Scherrer-Institut; CH-5232 Villigen SWITZERLAND Conrad, Harald h.conrad@fz-juelich.de Institut für Festkörperforschung, Forschungszentrum Jülich; DE-52425 Jülich GERMANY Corradi, Giacomo Istituto di Fisica Applicata “Nello Carrara”, Via Panciatichi 56/30; I-50127 Firenze ITALY Glückler, Harald h.glückler@fz-juelich.de Zentralabteilung Technologie, Forschungszentrum Jülich; DE-52425 Jülich GERMANY Granada, José Rolando granada@cnea.gov.ar Comisión Nacional de Energía Atómica; 8400 Bariloche (RN) ARGENTINA Hansen, Günter g.hansen@fz-juelich.de Zentralabteilung Technologie, Forschungszentrum Jülich; DE-52425 Jülich GERMANY Hinssen, Hans-Klemens h.-k.hinssen@fz-juelich.de Sicherheitsf. und Reaktortechnik, Forschungszentrum Jülich; DE-52425 Jülich GERMANY Iverson, Erik B. Iversoneb@ornl.gov Spallation Neutron Source, 701 Scarboro Road, Oak Ridge, TN 37830 USA Jahn, Wilfried w.jahn@fz-juelich.de Sicherheitsf. und Reaktortechnik, Forschungszentrum Jülich; DE-52425 Jülich GERMANY Jung, Peter p.jung@fz-juelich.de Institut für Festkörperforschung, Forschungszentrum Jülich; DE-52425 Jülich GERMANY Kiyanagi, Yoshiaki kiyanagi@qe.eng.hokudai.ac.jp Grad. School of Eng.; Hokkaido Univ.; Kita-13, Nishi-8, Kita-ku, Sapporo 060-8628 JAPAN 3
Page 1 and 2: ACoM - 6 6th 6 International Worksh
Page 3 and 4: Forschungszentrum Jülich GmbH Inst
Page 5: Preface These are the Proceedings o
Page 9 and 10: Alphabetical Author List Androsov A
Page 11 and 12: Contents Preface 1 List of Particip
Page 13 and 14: ABSTRACT ACoM - 6 6 th Meeting of t
Page 15 and 16: tion, which is the base to generate
Page 17 and 18: Table 2. Generated Scattering Law f
Page 19 and 20: Neutron Flux Spectrum (arbitrary un
Page 21 and 22: Figure 8. Continuous part of the fr
Page 23 and 24: 2.4 Conclusions for H2O For light w
Page 25 and 26: Figure 12. Frequency Distributions
Page 27 and 28: • Matrix-Elements 1 2 2 n µ κ
Page 29 and 30: Figure 15. Partial Neutron Scatteri
Page 31 and 32: Over a wide energy range our data a
Page 33 and 34: Figure 20. UCN Production Rate in S
Page 35 and 36: 4. SOLID METHANE AS A COLD MODERATO
Page 37 and 38: Neutron Flux Spectrum (arbitrary un
Page 39 and 40: 6. TRANSPORT CALCULATIONS FOR COLD
Page 41 and 42: Al He Figure 32. UCN - Source (Soli
Page 43 and 44: For fcc Al the incoherent inelastic
Page 45 and 46: [17] Reinsch,C.: Messung des differ
Page 47 and 48: ACoM - 6 6 th Meeting of the Collab
Page 49 and 50: To describe the slow-neutron cross
Page 51 and 52: Q0 denotes the (modulus of) momentu
Page 53 and 54: There is a difference in the inelas
Page 55 and 56: ABSTRACT ACoM-6 6 th Meeting of the
Page 57 and 58:
where nH 3 (nH) is the molecular de
Page 59 and 60:
Figure 1. Equilibrium ortho-hydroge
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e up to 0.30 with low levels of sys
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ABSTRACT ACoM - 6 6 th Meeting of t
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para transition energy. Liquid hydr
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The results for the composite moder
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Figure 6. Plots of the FWHM pulse w
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Neutron flight path Groove Vertical
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7.2 The optimum moderator for instr
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ather than neutronic considerations
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However, this cannot be used in MCN
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The results show the system of mult
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ent velocities and temperature fiel
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truding horizontally approximately
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ing high volume fractions indicate
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1. The number of volume elements wa
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Also in the lower half of the moder
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4. CONCLUSIONS The objective of thi
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Figure 2. Frequency distribution fu
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We also define: r r r Q = k − k =
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intervals. Thus some excitation ene
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the formula also to the libration m
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By fitting this function to the exp
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ABSTRACT ACoM 6 6 th Meeting of the
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mesitylene-D0, and the IINS spectra
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The intensity of scattered neutrons
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Intensity of scattered neutrons - I
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otations seem to be weaker and the
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ACoM - 6 6 th Meeting of the Collab
Page 119 and 120:
Water ice may still be a candidate
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�� 5 K � 20 K ��
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Figure 6. Inelastic spectra from ic
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The wealth of low lying energy leve
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Page 129 and 130:
After passing through the sub-cooli
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Figure 6. The 1.5 liter Amock moder
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Main results: Radiation effects in
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Irradiation cavity inside the capsu
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Table 2. Data of irradiation of ice
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eleased energy, J/g 120 110 100 90
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methane) an energy storing rate R i
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as adiabatic one. Then, solution of
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4÷÷÷÷5K (see Fig. 8). Saturatio
Page 149 and 150:
Due to insufficient number of irrad
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4. S. Ikeda, N. Watanabe, S. Satoh
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149
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151
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153
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Page 161 and 162:
3. PROTON BEAM MONITORING To normal
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performed with 1 mm layers of cadmi
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Page 167 and 168:
During beam time the target which i
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The moderator vessel including its
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materials. This is possible because
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Step 1: Normal gas is filled in bot
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Figure 6. Experimental energy spect
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Page 181 and 182:
Similar time of flight spectra were
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Table 1. Real moderator temperature
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etween 4 . 10 -3 eV and 2 . 10 -1 e
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tered radicals. But in more sophist
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Due to high dose rate and big volum
Page 193 and 194:
Figure 4. Recommended values of max
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where Ď is absorbed dose rate. Now
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It is interesting to note that σ 2
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11. V.I. Goldanski, E.N. Rumanov, E
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Appendix 197
Page 203 and 204:
Page 205 and 206:
201
Page 207 and 208:
203
Page 209 and 210:
205
Page 211 and 212:
207
Page 213 and 214:
209
Page 215 and 216:
Page 217 and 218:
Experimental Set up 213
Page 219 and 220:
Reaction Path 215
Page 221 and 222:
Comparison with non-hydrate forming
Page 223 and 224:
Mechanical Tests: Conditions 219
Page 225 and 226:
Mechanical Tests: Results 221
Page 227 and 228:
Conclusion • SKD approach is a vi
Page 229 and 230:
Schriften des Forschungszentrums J
Page 231:
Forschungszentrum Jülich in der He
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Druck-Materie 20b.qxd - JUWEL - Forschungszentrum Jülich

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