The Livermore Atomic Relaxation Data Library (EADL) 6000 0 0 0 2.000000+3 3.96821463 -1 0 0 0 200 1451 1 0.000000+0 0.000000+0 0 0 0 6 200 1451 2 0.000000+0 0.000000+0 0 0 6 6 200 1451 3 0.000000+0 0.000000+0 0 0 59 2 200 1451 4 2-He- 0 LLNL Eval-Dec90 D.E.Cullen 200 1451 5 UCRL-50400,Vol.30 Dist-Nov01 200 1451 6 ----ENDF/B-VI MATERIAL 100 200 1451 7 -----ATOMIC RELAXATION DATA 200 1451 8 ------ENDF-6 FORMAT 200 1451 9 ================================================================== 200 1451 10 The Livermore Evaluated Atomic Data Library (EADL) in the 200 1451 11 ENDF-6 Format. Translated from the Livermore ENDL format 200 1451 12 to the ENDF-6 Format by Bob MacFarlane (Los Alamos). 200 1451 13 ================================================================== 200 1451 14 Contents 200 1451 15 ================================================================== 200 1451 16 MF/MT Description 200 1451 17 ================================================================== 200 1451 18 28/533 Atomic Relaxation Data for Electrons and Photons 200 1451 19 ================================================================== 200 1451 20 Warning 200 1451 21 ================================================================== 200 1451 22 MF/MT combinations used to define ALL electron interaction data 200 1451 23 are newly defined MF/MT numbers for ENDF/B-VI that did not exist 200 1451 24 in earlier versions of ENDF/B. 200 1451 25 ================================================================== 200 1451 26 Definition of Data 200 1451 27 ================================================================== 200 1451 28 Atomic Relaxation Data for Electrons and Photons 200 1451 29 ================================================================== 200 1451 30 1) An atom can be ionized by a photon or an electron interaction. 200 1451 31 2) The atomic relaxation data included here describes how a 200 1451 32 singly ionized atom returns to neutrality, by emitting photons 200 1451 33 (x-rays) and/or electrons (Auger, Coster-Kronig). 200 1451 34 3) Data is given to define the transition probabilities between 200 1451 35 subshells for radiative (x-ray emission) and non-radiative 200 1451 36 (Auger, Coster-Kronig) transitions. 200 1451 37 4) The complete spectrum of emitted photons and electrons can be 200 1451 38 calculated using the data included here, e.g., see ref. 2, 200 1451 39 below, for am example of a computer code that analytically 200 1451 40 calculates these spectra. 200 1451 41 ================================================================== 200 1451 42 References 200 1451 43 ================================================================== 200 1451 44 1) S.T. Perkins, D.E. Cullen, etal., "Tables and Graphs of Atomic 200 1451 45 Subshell and Relaxation Data Derived from the LLNL Evaluated 200 1451 46 Atomic Data Library (EADL), Z = 1 - 100", UCRL-50400, Vol. 30, 200 1451 47 Lawrence Livermore National Laboratory (1991). 200 1451 48 2) D.E. Cullen "Program RELAX: A Code Designed to Calculate X-Ray 200 1451 49 and Electron Emission Spectra as Singly Charged Atoms Relax 200 1451 50 Back to Neutrality", UCRL-ID-110438, Lawrence Livermore 200 1451 51 National Laboratory (1992). 200 1451 52 200 1451 53 These are the primary references to the contents of this library 200 1451 54 and they contain a complete list of references to the sources 200 1451 55 of data used in this library, methods of evaluation, accuracy 200 1451 56 of the data, etc. 200 1451 57 ================================================================== 200 1451 58 History 200 1451 59 ================================================================== 200 1451 60 (1) November, 1991 - Initial release in the ENDL format. 200 1451 61 (2) November, 2001 - Initial release in the ENDF-6 format. 200 1451 62 ================================================================== 200 1451 63 1 451 65 0 200 1451 64 28 533 3 0 200 1451 65 200 1 0 66 200 0 0 67 2.000000+3 3.96821463 0 0 1 0 20028533 68 1.000000+0 0.000000+0 0 0 6 0 20028533 69 2.342000+1 2.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0 20028533 70 20028 0 71 200 0 0 72 0 0 0 73 -1 0 0 74