The Livermore Atomic Relaxation Data Library (EADL) 6000 0 0 0 1.400000+4 27.8442242 -1 0 0 01400 1451 1 0.000000+0 0.000000+0 0 0 0 61400 1451 2 0.000000+0 0.000000+0 0 0 6 61400 1451 3 0.000000+0 0.000000+0 0 0 59 21400 1451 4 14-Si- 0 LLNL Eval-Dec90 D.E.Cullen 1400 1451 5 UCRL-50400,Vol.30 Dist-Nov01 1400 1451 6 ----ENDF/B-VI MATERIAL 100 1400 1451 7 -----ATOMIC RELAXATION DATA 1400 1451 8 ------ENDF-6 FORMAT 1400 1451 9 ==================================================================1400 1451 10 The Livermore Evaluated Atomic Data Library (EADL) in the 1400 1451 11 ENDF-6 Format. Translated from the Livermore ENDL format 1400 1451 12 to the ENDF-6 Format by Bob MacFarlane (Los Alamos). 1400 1451 13 ==================================================================1400 1451 14 Contents 1400 1451 15 ==================================================================1400 1451 16 MF/MT Description 1400 1451 17 ==================================================================1400 1451 18 28/533 Atomic Relaxation Data for Electrons and Photons 1400 1451 19 ==================================================================1400 1451 20 Warning 1400 1451 21 ==================================================================1400 1451 22 MF/MT combinations used to define ALL electron interaction data 1400 1451 23 are newly defined MF/MT numbers for ENDF/B-VI that did not exist1400 1451 24 in earlier versions of ENDF/B. 1400 1451 25 ==================================================================1400 1451 26 Definition of Data 1400 1451 27 ==================================================================1400 1451 28 Atomic Relaxation Data for Electrons and Photons 1400 1451 29 ==================================================================1400 1451 30 1) An atom can be ionized by a photon or an electron interaction. 1400 1451 31 2) The atomic relaxation data included here describes how a 1400 1451 32 singly ionized atom returns to neutrality, by emitting photons 1400 1451 33 (x-rays) and/or electrons (Auger, Coster-Kronig). 1400 1451 34 3) Data is given to define the transition probabilities between 1400 1451 35 subshells for radiative (x-ray emission) and non-radiative 1400 1451 36 (Auger, Coster-Kronig) transitions. 1400 1451 37 4) The complete spectrum of emitted photons and electrons can be 1400 1451 38 calculated using the data included here, e.g., see ref. 2, 1400 1451 39 below, for am example of a computer code that analytically 1400 1451 40 calculates these spectra. 1400 1451 41 ==================================================================1400 1451 42 References 1400 1451 43 ==================================================================1400 1451 44 1) S.T. Perkins, D.E. Cullen, etal., "Tables and Graphs of Atomic 1400 1451 45 Subshell and Relaxation Data Derived from the LLNL Evaluated 1400 1451 46 Atomic Data Library (EADL), Z = 1 - 100", UCRL-50400, Vol. 30, 1400 1451 47 Lawrence Livermore National Laboratory (1991). 1400 1451 48 2) D.E. Cullen "Program RELAX: A Code Designed to Calculate X-Ray 1400 1451 49 and Electron Emission Spectra as Singly Charged Atoms Relax 1400 1451 50 Back to Neutrality", UCRL-ID-110438, Lawrence Livermore 1400 1451 51 National Laboratory (1992). 1400 1451 52 1400 1451 53 These are the primary references to the contents of this library1400 1451 54 and they contain a complete list of references to the sources 1400 1451 55 of data used in this library, methods of evaluation, accuracy 1400 1451 56 of the data, etc. 1400 1451 57 ==================================================================1400 1451 58 History 1400 1451 59 ==================================================================1400 1451 60 (1) November, 1991 - Initial release in the ENDL format. 1400 1451 61 (2) November, 2001 - Initial release in the ENDF-6 format. 1400 1451 62 ==================================================================1400 1451 63 1 451 65 01400 1451 64 28 533 73 01400 1451 65 1400 1 0 66 1400 0 0 67 1.400000+4 27.8442242 0 0 7 0140028533 68 1.000000+0 0.000000+0 0 0 156 25140028533 69 1.828500+3 2.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0140028533 70 3.000000+0 0.000000+0 1.719830+3 1.597910-2 0.000000+0 0.000000+0140028533 71 4.000000+0 0.000000+0 1.720520+3 3.170520-2 0.000000+0 0.000000+0140028533 72 6.000000+0 0.000000+0 1.821950+3 2.724020-4 0.000000+0 0.000000+0140028533 73 7.000000+0 0.000000+0 1.821980+3 5.404440-4 0.000000+0 0.000000+0140028533 74 2.000000+0 2.000000+0 1.525400+3 7.479540-2 0.000000+0 0.000000+0140028533 75 2.000000+0 3.000000+0 1.568280+3 8.012140-2 0.000000+0 0.000000+0140028533 76 2.000000+0 4.000000+0 1.568970+3 1.561310-1 0.000000+0 0.000000+0140028533 77 2.000000+0 5.000000+0 1.663320+3 1.411240-2 0.000000+0 0.000000+0140028533 78 2.000000+0 6.000000+0 1.670400+3 1.955840-3 0.000000+0 0.000000+0140028533 79 2.000000+0 7.000000+0 1.670430+3 3.815850-3 0.000000+0 0.000000+0140028533 80 3.000000+0 3.000000+0 1.611160+3 1.399050-2 0.000000+0 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