JAEA-Conf 2011-002 - 日本原子力研究開発機構

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JAEA-Conf 2011-002 For providing materials to make a decision of IFMIF construction, Engineering Validation and Engineering Design Activities (EVEDA) under the Broader Approach (BA) agreement have been started in June 2007. , the acceleration tests up to 9MeV by employing the deuteron beam of 125 mA, are planned at the BA site in Rokkasho, Aomori, Japan [4].
JAEA-Conf 2011-002
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JAEA-Conf 2011-002 Proceedings of t
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JAEA-Conf 2011-002 31. Preliminary
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6.2 Measurement of neutron-induced
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JAEA-Conf 2011-002 Table 1 Comparis
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JAEA-Conf 2011-002 (T1/2=8,900,000
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JAEA-Conf 2011-002 Though words too
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JENDL-3.3 showed better applicabili
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ENDF. Thus this cross section store
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Acknowledgement JAEA-Conf 2011-002
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In the MALIBU program, isotope conc
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some minor actinides. For major act
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JAEA-Conf 2011-002 code MVP-BURN an
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JAEA-Conf 2011-002 [3] Measurements
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3.1 Experimental Set up JAEA-Conf 2
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References JAEA-Conf 2011-002 [1] N
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JAEA-Conf 2011-002 was large. The a
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JAEA-Conf 2011-002 4. Results and D
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Acknowledgments Present study inclu
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Fig. 1 A conceptural picture of the
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4. Theoretical studies Theoretical
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JAEA-Conf 2011-002 Fig.9 Comparison
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Ion source JAEA-Conf 2011-002 LE
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JAEA-Conf 2011-002 3. Readiness
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JAEA-Conf 2011-002
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JAEA-Conf 2011-002 Figure 1. An exa
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JAEA-Conf 2011-002 Figure 6. Compar
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JAEA-Conf 2011-002 calculation of d
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JAEA-Conf 2011-002 equilibrium emis
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JAEA-Conf 2011-002 Cowley et al. [1
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4. Conclusions We have compared nuc
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of MeV region with highest cosmic-r
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JAEA-Conf 2011-002 events can be id
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JAEA-Conf 2011-002 models and its p
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JAEA-Conf 2011-002
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JAEA-Conf 2011-002
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JAEA-Conf 2011-002 xx
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JAEA-Conf 2011-002 1. The recent ac
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JAEA-Conf 2011-002 4. Conceptual de
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The Institute's staff of about 280
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3. Nuclear Theory Laboratory JAEA-C
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JAEA-Conf 2011-002 References [1] P
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JAEA-Conf 2011-002 reaction 6 Li +
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Using the approximated distribution
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momentum of the constituents of P.
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dσ/dΩ (mb/sr) c.m. scattering ang
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JAEA-Conf 2011-002 [2] N. Austern,
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moderating fast neutrons emitted fr
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JAEA-Conf 2011-002 3. Results and d
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JAEA-Conf 2011-002 the detection de
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Fig.1. Experimental arrangement for
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in this work was confirmed. (2) 153
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Neutron Capture Cross Section of 15
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ENDF resonance parameters are based
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sample changer. The measured flux s
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REFERENCES JAEA-Conf 2011-002 [1] W
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JAEA-Conf 2011-002 Fig. 4: The rela
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Fig. 10: The PHITS2 calculation geo
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for such a low energy region should
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MCNPX calculation was performed bas
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JAEA-Conf 2011-002 We measured dou
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1mm-thick carbon target 22mm in dia
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JAEA-Conf 2011-002 Figure 2 shows e
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The double-differential (n,xp) and
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JAEA-Conf 2011-002 forward angles.
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Fig.3. Two-dimensional plot of PI v
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JAEA-Conf 2011-002 Fig. 7. Deuteron
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JAEA-Conf 2011-002 The new detector
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4. Off line data analysis Double di
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eports of data of carbon-ion incide
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Count [-] 4 10 3 10 2 10 10 1 Charg
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Acknowledgement We are grateful to
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Beam Line BM1 Copper Target BM2 5×
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Page 162 and 163: References [1] K. Ishibashi, H. Tak
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Page 172 and 173: We described our formalism for calc
Page 174 and 175: 2. Model
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Page 180 and 181: JAEA-Conf 2011-002 reactions. Figur
Page 182 and 183: JAEA-Conf 2011-002 Fig. 3. The angu
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Page 192 and 193: analysis of integral experiments [6
Page 194 and 195: A modified SRAC library was prepare
Page 196 and 197: JAEA-Conf 2011-002 approximately 0.
Page 198 and 199: JAEA-Conf 2011-002 constructing the
Page 200 and 201: Fig.9 Spectrum of gamma-ray followi
Page 204 and 205: JAEA-Conf 2011-002 in the same way
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Page 218 and 219: components, the 0.56Wt% for hydroge
Page 222 and 223: Sensitivities of curium isotope con
Page 224 and 225: decreases of (n,g) reaction rates,
Page 226 and 227: 5. Conclusion JAEA-Conf 2011-002 Wi
Page 228 and 229: 2. Foundation of sensitivity analys
Page 230 and 231: JAEA-Conf 2011-002 where f g and f
Page 232 and 233: Fig.1 Sensitivity coefficient of th
Page 234 and 235: An outline of core configurations o
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Page 238 and 239: To clarify what nuclides and reacti
Page 240 and 241: Calculation was performed by the MV
Page 242 and 243: among these libraries, and the diff
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