The Livermore Atomic Relaxation Data Library (EADL) 6000 0 0 0 1.000000+4 20.0056471 -1 0 0 01000 1451 1 0.000000+0 0.000000+0 0 0 0 61000 1451 2 0.000000+0 0.000000+0 0 0 6 61000 1451 3 0.000000+0 0.000000+0 0 0 59 21000 1451 4 10-Ne- 0 LLNL Eval-Dec90 D.E.Cullen 1000 1451 5 UCRL-50400,Vol.30 Dist-Nov01 1000 1451 6 ----ENDF/B-VI MATERIAL 100 1000 1451 7 -----ATOMIC RELAXATION DATA 1000 1451 8 ------ENDF-6 FORMAT 1000 1451 9 ==================================================================1000 1451 10 The Livermore Evaluated Atomic Data Library (EADL) in the 1000 1451 11 ENDF-6 Format. Translated from the Livermore ENDL format 1000 1451 12 to the ENDF-6 Format by Bob MacFarlane (Los Alamos). 1000 1451 13 ==================================================================1000 1451 14 Contents 1000 1451 15 ==================================================================1000 1451 16 MF/MT Description 1000 1451 17 ==================================================================1000 1451 18 28/533 Atomic Relaxation Data for Electrons and Photons 1000 1451 19 ==================================================================1000 1451 20 Warning 1000 1451 21 ==================================================================1000 1451 22 MF/MT combinations used to define ALL electron interaction data 1000 1451 23 are newly defined MF/MT numbers for ENDF/B-VI that did not exist1000 1451 24 in earlier versions of ENDF/B. 1000 1451 25 ==================================================================1000 1451 26 Definition of Data 1000 1451 27 ==================================================================1000 1451 28 Atomic Relaxation Data for Electrons and Photons 1000 1451 29 ==================================================================1000 1451 30 1) An atom can be ionized by a photon or an electron interaction. 1000 1451 31 2) The atomic relaxation data included here describes how a 1000 1451 32 singly ionized atom returns to neutrality, by emitting photons 1000 1451 33 (x-rays) and/or electrons (Auger, Coster-Kronig). 1000 1451 34 3) Data is given to define the transition probabilities between 1000 1451 35 subshells for radiative (x-ray emission) and non-radiative 1000 1451 36 (Auger, Coster-Kronig) transitions. 1000 1451 37 4) The complete spectrum of emitted photons and electrons can be 1000 1451 38 calculated using the data included here, e.g., see ref. 2, 1000 1451 39 below, for am example of a computer code that analytically 1000 1451 40 calculates these spectra. 1000 1451 41 ==================================================================1000 1451 42 References 1000 1451 43 ==================================================================1000 1451 44 1) S.T. Perkins, D.E. Cullen, etal., "Tables and Graphs of Atomic 1000 1451 45 Subshell and Relaxation Data Derived from the LLNL Evaluated 1000 1451 46 Atomic Data Library (EADL), Z = 1 - 100", UCRL-50400, Vol. 30, 1000 1451 47 Lawrence Livermore National Laboratory (1991). 1000 1451 48 2) D.E. Cullen "Program RELAX: A Code Designed to Calculate X-Ray 1000 1451 49 and Electron Emission Spectra as Singly Charged Atoms Relax 1000 1451 50 Back to Neutrality", UCRL-ID-110438, Lawrence Livermore 1000 1451 51 National Laboratory (1992). 1000 1451 52 1000 1451 53 These are the primary references to the contents of this library1000 1451 54 and they contain a complete list of references to the sources 1000 1451 55 of data used in this library, methods of evaluation, accuracy 1000 1451 56 of the data, etc. 1000 1451 57 ==================================================================1000 1451 58 History 1000 1451 59 ==================================================================1000 1451 60 (1) November, 1991 - Initial release in the ENDL format. 1000 1451 61 (2) November, 2001 - Initial release in the ENDF-6 format. 1000 1451 62 ==================================================================1000 1451 63 1 451 65 01000 1451 64 28 533 17 01000 1451 65 1000 1 0 66 1000 0 0 67 1.000000+4 20.0056471 0 0 4 0100028533 68 1.000000+0 0.000000+0 0 0 54 8100028533 69 8.581800+2 2.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0100028533 70 3.000000+0 0.000000+0 8.381000+2 4.643290-3 0.000000+0 0.000000+0100028533 71 4.000000+0 0.000000+0 8.382200+2 9.229670-3 0.000000+0 0.000000+0100028533 72 2.000000+0 2.000000+0 7.717200+2 9.305840-2 0.000000+0 0.000000+0100028533 73 2.000000+0 3.000000+0 7.948700+2 9.210240-2 0.000000+0 0.000000+0100028533 74 2.000000+0 4.000000+0 7.949900+2 1.815780-1 0.000000+0 0.000000+0100028533 75 3.000000+0 3.000000+0 8.180200+2 1.456810-2 0.000000+0 0.000000+0100028533 76 3.000000+0 4.000000+0 8.181400+2 3.851310-1 0.000000+0 0.000000+0100028533 77 4.000000+0 4.000000+0 8.182600+2 2.196890-1 0.000000+0 0.000000+0100028533 78 2.000000+0 0.000000+0 0 0 6 0100028533 79 4.323000+1 2.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0100028533 80 3.000000+0 0.000000+0 0 0 6 0100028533 81 2.008000+1 2.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0100028533 82 4.000000+0 0.000000+0 0 0 6 0100028533 83 1.996000+1 4.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0100028533 84 100028 0 85 1000 0 0 86 0 0 0 87 -1 0 0 88