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RULER - Reduced Electromagnetic Transition Strengths and Recommended Upper Limits T. Kibèdi (ANL) F.G. Kondev (ANU) Tibor Kibèdi, Dep. of Nuclear Physics,

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Presentation on theme: "RULER - Reduced Electromagnetic Transition Strengths and Recommended Upper Limits T. Kibèdi (ANL) F.G. Kondev (ANU) Tibor Kibèdi, Dep. of Nuclear Physics,"— Presentation transcript:

1 RULER - Reduced Electromagnetic Transition Strengths and Recommended Upper Limits T. Kibèdi (ANL) F.G. Kondev (ANU) Tibor Kibèdi, Dep. of Nuclear Physics, Australian National UniversityND2010, Jeju Island, Korea, 26-30-Apr-2010

2 Relative strengths Definitions Weisskopf single particle estimates: Tibor Kibèdi, Dep. of Nuclear Physics, Australian National UniversityNSDD 2015, IAEA, 20-24-Apr-2015 isomer  exp  j

3 Mixed transitions Empirical transition strength Tibor Kibèdi, Dep. of Nuclear Physics, Australian National UniversityNSDD 2015, IAEA, 20-24-Apr-2015 Partial  -ray half-life: isomer  exp  j

4 Current issues with RULER Tibor Kibèdi, Dep. of Nuclear Physics, Australian National UniversityNSDD 2015, IAEA, 20-24-Apr-2015 NSDD/IAEA: 3.2a (Aug-6-2007; T.W. Burrows) Isomer evaluation (ANU/ANL): 4.1c (12-Jun-2014) Problems:  Complicated logic  Related parameters stored at different places  Uncertainty propagation: analytical approach; ad hock, nested branches based on numerical values Modifications  ENSDF type: Value, uncertainties (numerical and character) stored together  Simplified logic  Added functionality:  ICC calculated for mixed and pure multipolarities to deduce B(  L) and B(  ’L’)  LaTex output for ADNDT

5 Value = f(X) Uncertainty calculated as: |Df L | = |f(X)-f(DX L )| |Df U | = |f(X)-f(DX L )| Uncertainty propagation Tibor Kibèdi, Dep. of Nuclear Physics, Australian National UniversityNSDD 2015, IAEA, 20-24-Apr-2015 isomer  exp  j Partial  -ray half-life: X X X-DX L X-DX U f(X)

6 Uncertainty propagation Tibor Kibèdi, Dep. of Nuclear Physics, Australian National UniversityNSDD 2015, IAEA, 20-24-Apr-2015 isomer  exp  j Partial  -ray half-life: X X X-DX L X-DX U f(X) Value = stat. mean Uncertainty calculated from distribution of f(x)

7 Uncertainty propagation using Monte Carlo Tibor Kibèdi, Dep. of Nuclear Physics, Australian National UniversityNSDD 2015, IAEA, 20-24-Apr-2015 Probability Density Functions  NORMAL (symmetric)  Skewed Gaussian (asymmetric)  Square (limits; constant prob.)  X ≤ 3 : -∞ ≤ X ≤ 3  X ≤ -3 : -∞ ≤ X ≤ -3 but  X ≤ +3 : 0 ≤ X ≤ +3 Program library based on NPL report MS 7 (2010 Cox) Part of NS_lib (FORTRAN 90) shared with BrIcc, BrIccMixing, BrIccEmis, NEW Ruler ….


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