JAEA-Conf 2011-002 - 日本原子力研究開発機構

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sample changer. The measured flux shape is usually normalized directly to a saturated capture resonance. This capture yield and its associated statistical uncertainty provided input to the SAMMY data analysis code 13 that extracted the neutron resonance parameters. Experiment Overlap Filter Epithermal Capture Boron cabide Neutron- Producing Target Bare Bounce JAEA-Conf 2011-002 TABLE II Gadolinium Experimental Details Average Beam Current (A) Beam Energy (MeV) Pulse Width (ns) Channel Width (ns) Pulse Repetition Rate (pulse/s) Flight Path Length (m) 17.28 57 18 12.8 225 25 Fig. 1. Layout of the RPI LINAC facility. 3. RESULTS AND CONCLUSIONS Data were dead time corrected, run-summed, beam-monitor-normalized, and background-corrected. Final processed data were reduced to capture yield. The Resonance parameters, neutron width n, radiation width , and resonance energy E0, were extracted from the capture using the SAMMY version 8 multilevel Rmatrix Bayesian code. 7 The resolved resonance energy region for 155 Gd and 157 Gd in the ENDF/B-VII.0 evaluation ends at 180.4 eV and 306.4 eV. As a result, fitting data above 180.4 eV and 306.4 eV were performed with initial estimates for resonance locations width-a challenging task. 155 Gd and 157 Gd were observed new resonance as shown in Figure 2. The details of resonance parameters for Gd isotopes are obtained and will be reported in the separated paper.
JAEA-Conf 2011-002 Fig. 2. An overview of the data and SAMMY fits in 155 Gd and 157 Gd.
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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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Page 110 and 111: JAEA-Conf 2011-002 the detection de
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Ztarget, Atarget are the numbers fo
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We described our formalism for calc
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2. Model
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JAEA-Conf 2011-002 reactions. Figur
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JAEA-Conf 2011-002 Fig. 3. The angu
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analysis of integral experiments [6
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A modified SRAC library was prepare
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JAEA-Conf 2011-002 approximately 0.
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JAEA-Conf 2011-002 constructing the
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Fig.9 Spectrum of gamma-ray followi
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JAEA-Conf 2011-002 in the same way
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JAEA-Conf 2011-002 [7]. For example
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JAEA-Conf 2011-002 For
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JAEA-Conf 2011-002 (5.0-9.0MeV), a
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components, the 0.56Wt% for hydroge
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Sensitivities of curium isotope con
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decreases of (n,g) reaction rates,
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5. Conclusion JAEA-Conf 2011-002 Wi
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2. Foundation of sensitivity analys
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JAEA-Conf 2011-002 where f g and f
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Fig.1 Sensitivity coefficient of th
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An outline of core configurations o
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0.010% 0.000% -0.010% -0.020% -0.03
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To clarify what nuclides and reacti
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Calculation was performed by the MV
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among these libraries, and the diff
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JAEA-Conf 2011-002 - 日本原子力研究開発機構

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