JENDL-4.0/HE incident proton library 0 0 1.001000+3 9.991670-1 -1 0 6 1 125 1451 1 0.000000+0 0.000000+0 0 0 0 6 125 1451 2 9.986200-1 2.000000+8 1 0 10010 4 125 1451 3 0.000000+0 0.000000+0 1 0 42 3 125 1451 4 1-H - 1 JAERI EVAL-APR93 S.CHIBA 125 1451 5 NST33(1996)654 DIST-Nov20 125 1451 6 ----JENDL-4.0/HE MATERIAL 125 125 1451 7 -----INCIDENT PROTON DATA 125 1451 8 ------ENDF-6 FORMAT 125 1451 9 125 1451 10 ****************************************************** 125 1451 11 125 1451 12 --- JENDL-4.0/HE --- 125 1451 13 125 1451 14 High-energy Evaluation up to 200 MeV 125 1451 15 125 1451 16 ****************************************************** 125 1451 17 125 1451 18 History 125 1451 19 2015-03 Compiled by S.Kunieda 125 1451 20 (Data were taken from JENDL High-energy File 2007 /1/.) 125 1451 21 125 1451 22 References 125 1451 23 1) Watanabe,Y. et al.: J. Korean Phys. Soc., 59, 1443 (2011). 125 1451 24 125 1451 25 125 1451 26 ___________( Comments from JENDL High-energy File 2007 )__________ 125 1451 27 125 1451 28 HISTORY 125 1451 29 93-04 Evaluation was performed by S. Cshiba (JAERI), S. Morioka 125 1451 30 (CRC) and T. Fukahori for JENDL High Energy File. 125 1451 31 Details are given in Ref. /1/. 125 1451 32 03-05 Compiled by T. Fukahori for JENDL/HE. 125 1451 33 04-02 Reviewed by T. Hino (Hitachi). 125 1451 34 125 1451 35 MF=1 General Information 125 1451 36 MT=451 Descriptive Data and Dictionary 125 1451 37 125 1451 38 MF=3 Cross Sections 125 1451 39 MT=2 Elastic Scattering Cross Section 125 1451 40 Based on phase-shift data of Arndt et al./3,4/. 125 1451 41 125 1451 42 MF=6 Double-differential cross section 125 1451 43 MT=2 125 1451 44 Based on phase-shift data of Arndt et al./3,4/. 125 1451 45 125 1451 46 1 451 49 1 125 1451 47 3 2 4 1 125 1451 48 6 2 29 1 125 1451 49 125 1 099999 125 0 0 0 1.001000+3 9.991670-1 0 0 0 0 125 3 2 1 0.000000+0 0.000000+0 0 0 1 2 125 3 2 2 2 2 125 3 2 3 1.000000+3 1.000000+0 2.000000+8 1.000000+0 125 3 2 4 125 3 099999 125 0 0 0 1.001000+3 9.991670-1 0 2 1 0 125 6 2 1 1.001000+3 9.986200-1 0 5 1 7 125 6 2 2 7 2 125 6 2 3 1.000000+3 3.916400-1 1.000000+7 3.916400-1 2.500000+7 1.412600-1 125 6 2 4 5.000000+7 6.454100-2 1.000000+8 3.385800-2 1.500000+8 2.735600-2 125 6 2 5 2.000000+8 2.527700-2 125 6 2 6 5.000000-1 0.000000+0 1 0 1 7 125 6 2 7 7 22 125 6 2 8 0.000000+0 1.000000+3 2 0 7 6 125 6 2 9 1.246600-1 4.340000-4 3.101100-5-1.678600-5 1.781500-6 6.780300-7 125 6 2 10 0.000000+0 125 6 2 11 0.000000+0 1.000000+7 2 0 7 6 125 6 2 12 1.246600-1 4.340000-4 3.101100-5-1.678600-5 1.781500-6 6.780300-7 125 6 2 13 0.000000+0 125 6 2 14 0.000000+0 2.500000+7 2 0 7 6 125 6 2 15 4.496400-2 4.849900-4 1.562300-5-5.193800-5 8.776600-6 3.636500-6 125 6 2 16 0.000000+0 125 6 2 17 0.000000+0 5.000000+7 2 0 7 6 125 6 2 18 2.054400-2 4.833100-4 3.665800-5-6.179600-5 2.050300-5 8.544500-6 125 6 2 19 8.632700-9 125 6 2 20 0.000000+0 1.000000+8 2 0 7 6 125 6 2 21 1.077700-2 4.136000-4 1.265500-4-5.602700-5 3.931600-5 1.594700-5 125 6 2 22 1.079000-7 125 6 2 23 0.000000+0 1.500000+8 2 0 7 6 125 6 2 24 8.707800-3 3.396400-4 1.474200-4-5.744300-5 4.385900-5 2.028600-5 125 6 2 25 2.877500-7 125 6 2 26 0.000000+0 2.000000+8 2 0 7 6 125 6 2 27 8.046100-3 2.170800-4 1.443000-4-6.185900-5 4.657500-5 2.233800-5 125 6 2 28 5.184900-7 125 6 2 29 125 6 099999 125 0 0 0 0 0 0 0 -1 0 0 0