Determination of Resonance Parameters and their Covariances from Neutron Induced Reaction Cross Section Data

被引:113
作者
Schillebeeckx, P. [1 ]
Becker, B. [1 ]
Danon, Y. [2 ]
Guber, K. [3 ]
Harada, H. [4 ]
Heyse, J. [1 ]
Junghans, A. R. [5 ]
Kopecky, S. [1 ]
Massimi, C. [6 ,7 ]
Moxon, M. C.
Otuka, N. [8 ]
Sirakov, I. [9 ]
Volev, K. [1 ]
机构
[1] EC JRC IRMM, B-2440 Geel, Belgium
[2] Rensselaer Polytech Inst, Troy, NY 12180 USA
[3] Oak Ridge Natl Lab, Oak Ridge, TN 37831 USA
[4] Japan Atom Energy Agcy, Naka, Ibaraki 3191195, Japan
[5] Helmholtz Zentrum Dresden Rossendorf, D-01314 Dresden, Germany
[6] Univ Bologna, I-40126 Bologna, Italy
[7] Sez INFN Bologna, I-40126 Bologna, Italy
[8] IAEA, IAEA Nucl Data Sect, A-1400 Vienna, Austria
[9] Bulgarian Acad Sci, Inst Nucl Res & Nucl Energy, BG-1784 Sofia, Bulgaria
关键词
ENERGY REGION 0.02; OF-FLIGHT METHOD; N-TOF; CAPTURE MEASUREMENTS; RADIATIVE-CAPTURE; RESOLUTION MEASUREMENT; IONIZATION-CHAMBER; 1.15-KEV RESONANCE; WEIGHTING FUNCTION; DATA-ACQUISITION;
D O I
10.1016/j.nds.2012.11.005
中图分类号
O57 [原子核物理学、高能物理学];
学科分类号
070202 ;
摘要
Cross section data in the resolved and unresolved resonance region are represented by nuclear reaction formalisms using parameters which are determined by fitting them to experimental data. Therefore, the quality of evaluated cross sections in the resonance region strongly depends on the experimental data used in the adjustment process and an assessment of the experimental covariance data is of primary importance in determining the accuracy of evaluated cross section data. In this contribution, uncertainty components of experimental observables resulting from total and reaction cross section experiments are quantified by identifying the metrological parameters involved in the measurement, data reduction and analysis process. In addition, different methods that can be applied to propagate the covariance of the experimental observables (i.e. transmission and reaction yields) to the covariance of the resonance parameters are discussed and compared. The methods being discussed are: conventional uncertainty propagation, Monte Carlo sampling and marginalization. It is demonstrated that the final covariance matrix of the resonance parameters not only strongly depends on the type of experimental observables used in the adjustment process, the experimental conditions and the characteristics of the resonance structure, but also on the method that is used to propagate the covariances. Finally, a special data reduction concept and format is presented, which offers the possibility to store the full covariance information of experimental data in the EXFOR library and provides the information required to perform a full covariance evaluation.
引用
收藏
页码:3054 / 3100
页数:47
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