diff --git a/Projects/Dali/PPCROSSSECTION.txt b/Projects/Dali/PPCROSSSECTION.txt new file mode 100644 index 0000000000000000000000000000000000000000..76839018280f93ec5485158d889ac64a197709d1 --- /dev/null +++ b/Projects/Dali/PPCROSSSECTION.txt @@ -0,0 +1,4081 @@ +Retrieved by E4-Web: 2019/01/09,13:35:27 1 0 0 0 + 1.001000+3 9.991700-1 -1 0 0 1 125 1451 1 + 0.000000+0 0.000000+0 0 0 0 6 125 1451 2 + 9.986200-1 1.500000+8 0 0 10010 8 125 1451 3 + 0.000000+0 0.000000+0 0 0 32 2 125 1451 4 + 1-H - 1 LANL EVAL-FEB98 G.HALE 125 1451 5 + CH99 DIST-FEB18 20111222 125 1451 6 +----ENDF/B-VIII.0 MATERIAL 125 REVISION 1 125 1451 7 +-----INCIDENT PROTON DATA 125 1451 8 +------ENDF-6 FORMAT 125 1451 9 + 125 1451 10 + **************************************************************** 125 1451 11 + 125 1451 12 + ENDF/B-VI MOD 2 Evaluation, February 1998, G. M. Hale (LANL) 125 1451 13 + 125 1451 14 + Includes p + H1 elastic MT = 2 125 1451 15 + 125 1451 16 + p-p elastic cross sections calculated for Ep between 0 and 125 1451 17 + 150 MeV from an R-matrix analysis of p-p cross-section and 125 1451 18 + polarization data in this energy range. The maximum nuclear 125 1451 19 + partial wave allowed in the fit is l=6, and the resulting 125 1451 20 + chi-squared per degree of freedom is 1.8. 125 1451 21 + 125 1451 22 + **************************************************************** 125 1451 23 + 125 1451 24 + ENDF/B-VI MOD 1 Evaluation, October 1987, D. Dodder (LANL) 125 1451 25 + 125 1451 26 + Completely replaced by MOD 2 evaluation. 125 1451 27 + 125 1451 28 +**************************************************************** 125 1451 29 + 125 1451 30 +REFERENCES 125 1451 31 + 125 1451 32 +[Ch99] M.B. Chadwick, P G. Young, G. M. Hale, et al., Los Alamos 125 1451 33 + National Laboratory report, LA-UR-99-1222 (1999) 125 1451 34 + 125 1451 35 + ************************ C O N T E N T S ************************ 125 1451 36 + 1 451 39 1 125 1451 37 + 6 2 661 1 125 1451 38 + 0.000000+0 0.000000+0 0 0 0 0 125 1 099999 + 0.000000+0 0.000000+0 0 0 0 0 125 0 0 0 + 1.001000+3 9.991700-1 0 2 1 0 125 6 2 1 + 1.001000+3 9.966200-1 0 5 1 2 125 6 2 2 + 2 2 125 6 2 3 + 1.000000+3 1.000000+0 1.500000+8 1.000000+0 125 6 2 4 + 5.000000-1 0.000000+0 1 0 1 131 125 6 2 5 + 131 2 125 6 2 6 + 0.000000+0 1.000000+3 1 0 21 6 125 6 2 7 + 0.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0 125 6 2 8 + 0.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0 125 6 2 9 + 0.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0 125 6 2 10 + 0.000000+0 0.000000+0 0.000000+0 125 6 2 11 + 0.000000+0 2.000000+4 1 0 21 6 125 6 2 12 + 4.913300-5-1.84640-12 2.43950-19-1.66800-20-1.91330-20 2.71050-20 125 6 2 13 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1.247500-3 8.521700-4 9.208800-4 3.320700-4 125 6 2 644 + 3.183500-5 6.849900-4 7.374800-5-1.161000-4-5.685200-6 6.128200-5 125 6 2 645 + 6.862100-6-3.663800-5-2.642300-6 125 6 2 646 + 0.000000+0 1.300000+8 1 0 21 6 125 6 2 647 + 8.002800-3 3.667700-4 4.729400-5-7.285600-6 7.595700-6 2.559800-6 125 6 2 648 + 4.599200-7 2.204000-3 8.829400-4 9.832300-4 9.835900-4 4.082100-4 125 6 2 649 + 4.515100-5 3.495900-4 3.528300-5-7.667200-5-3.957500-6 3.957000-5 125 6 2 650 + 3.451800-6-2.616200-5-1.852200-6 125 6 2 651 + 0.000000+0 1.400000+8 1 0 21 6 125 6 2 652 + 8.012900-3 3.019100-4 3.066000-5-5.307700-6-1.458800-6 6.215000-7 125 6 2 653 + 3.520700-9 1.730700-3 5.577300-4 1.060000-3 1.079100-3 5.510900-4 125 6 2 654 + 7.677100-5-8.305300-5 1.640700-6-1.535200-5-9.084600-7 2.810500-5 125 6 2 655 + 2.128200-6-2.205500-6-1.594900-7 125 6 2 656 + 0.000000+0 1.500000+8 1 0 21 6 125 6 2 657 + 9.283100-3 4.540700-4 2.309700-4 1.386200-4 4.412100-5 4.820100-6 125 6 2 658 + 1.252100-6 1.239400-3 2.931600-4 1.053000-3 1.209400-3 7.707700-4 125 6 2 659 + 1.445700-4-5.740300-4-2.038600-7 6.595800-5 4.754900-6 6.237400-5 125 6 2 660 + 7.335900-6 4.016600-5 3.133500-6 125 6 2 661 + 0.000000+0 0.000000+0 0 0 0 0 125 6 099999 + 0.000000+0 0.000000+0 0 0 0 0 125 0 0 0 + 0.000000+0 0.000000+0 0 0 0 0 0 0 0 0 + 1.001000+3 9.991700-1 -1 0 0 2 125 1451 1 + 0.000000+0 0.000000+0 0 0 0 6 125 1451 2 + 9.986200-1 1.500000+8 1 0 10010 7 125 1451 3 + 0.000000+0 0.000000+0 0 0 32 2 125 1451 4 + 1-H - 1 LANL EVAL-FEB98 G.HALE 125 1451 5 + CH99 DIST-DEC06 REV1- 20111222 125 1451 6 +----ENDF/B-VII.1 MATERIAL 125 REVISION 1 125 1451 7 +-----INCIDENT PROTON DATA 125 1451 8 +------ENDF-6 FORMAT 125 1451 9 + 125 1451 10 + **************************************************************** 125 1451 11 + 125 1451 12 + ENDF/B-VI MOD 2 Evaluation, February 1998, G. M. Hale (LANL) 125 1451 13 + 125 1451 14 + Includes p + H1 elastic MT = 2 125 1451 15 + 125 1451 16 + p-p elastic cross sections calculated for Ep between 0 and 125 1451 17 + 150 MeV from an R-matrix analysis of p-p cross-section and 125 1451 18 + polarization data in this energy range. The maximum nuclear 125 1451 19 + partial wave allowed in the fit is l=6, and the resulting 125 1451 20 + chi-squared per degree of freedom is 1.8. 125 1451 21 + 125 1451 22 + **************************************************************** 125 1451 23 + 125 1451 24 + ENDF/B-VI MOD 1 Evaluation, October 1987, D. Dodder (LANL) 125 1451 25 + 125 1451 26 + Completely replaced by MOD 2 evaluation. 125 1451 27 + 125 1451 28 +**************************************************************** 125 1451 29 + 125 1451 30 +REFERENCES 125 1451 31 + 125 1451 32 +[Ch99] M.B. Chadwick, P G. Young, G. M. Hale, et al., Los Alamos 125 1451 33 + National Laboratory report, LA-UR-99-1222 (1999) 125 1451 34 + 125 1451 35 + ************************ C O N T E N T S ************************ 125 1451 36 + 1 451 39 1 125 1451 37 + 6 2 661 1 125 1451 38 + 0.000000+0 0.000000+0 0 0 0 0 125 1 099999 + 0.000000+0 0.000000+0 0 0 0 0 125 0 0 0 + 1.001000+3 9.991700-1 0 2 1 0 125 6 2 1 + 1.001000+3 9.966200-1 0 5 1 2 125 6 2 2 + 2 2 125 6 2 3 + 1.000000+3 1.000000+0 1.500000+8 1.000000+0 125 6 2 4 + 5.000000-1 0.000000+0 1 0 1 131 125 6 2 5 + 131 2 125 6 2 6 + 0.000000+0 1.000000+3 1 0 21 6 125 6 2 7 + 0.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0 125 6 2 8 + 0.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0 125 6 2 9 + 0.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0 125 6 2 10 + 0.000000+0 0.000000+0 0.000000+0 125 6 2 11 + 0.000000+0 2.000000+4 1 0 21 6 125 6 2 12 + 4.913300-5-1.84640-12 2.43950-19-1.66800-20-1.91330-20 2.71050-20 125 6 2 13 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1.247500-3 8.521700-4 9.208800-4 3.320700-4 125 6 2 644 + 3.183500-5 6.849900-4 7.374800-5-1.161000-4-5.685200-6 6.128200-5 125 6 2 645 + 6.862100-6-3.663800-5-2.642300-6 125 6 2 646 + 0.000000+0 1.300000+8 1 0 21 6 125 6 2 647 + 8.002800-3 3.667700-4 4.729400-5-7.285600-6 7.595700-6 2.559800-6 125 6 2 648 + 4.599200-7 2.204000-3 8.829400-4 9.832300-4 9.835900-4 4.082100-4 125 6 2 649 + 4.515100-5 3.495900-4 3.528300-5-7.667200-5-3.957500-6 3.957000-5 125 6 2 650 + 3.451800-6-2.616200-5-1.852200-6 125 6 2 651 + 0.000000+0 1.400000+8 1 0 21 6 125 6 2 652 + 8.012900-3 3.019100-4 3.066000-5-5.307700-6-1.458800-6 6.215000-7 125 6 2 653 + 3.520700-9 1.730700-3 5.577300-4 1.060000-3 1.079100-3 5.510900-4 125 6 2 654 + 7.677100-5-8.305300-5 1.640700-6-1.535200-5-9.084600-7 2.810500-5 125 6 2 655 + 2.128200-6-2.205500-6-1.594900-7 125 6 2 656 + 0.000000+0 1.500000+8 1 0 21 6 125 6 2 657 + 9.283100-3 4.540700-4 2.309700-4 1.386200-4 4.412100-5 4.820100-6 125 6 2 658 + 1.252100-6 1.239400-3 2.931600-4 1.053000-3 1.209400-3 7.707700-4 125 6 2 659 + 1.445700-4-5.740300-4-2.038600-7 6.595800-5 4.754900-6 6.237400-5 125 6 2 660 + 7.335900-6 4.016600-5 3.133500-6 125 6 2 661 + 0.000000+0 0.000000+0 0 0 0 0 125 6 099999 + 0.000000+0 0.000000+0 0 0 0 0 125 0 0 0 + 0.000000+0 0.000000+0 0 0 0 0 0 0 0 0 + 1.001000+3 9.991700-1 -1 0 0 2 125 1451 1 + 0.000000+0 0.000000+0 0 0 0 6 125 1451 2 + 9.986200-1 1.500000+8 6 0 10010 7 125 1451 3 + 0.000000+0 0.000000+0 0 0 32 2 125 1451 4 + 1-H - 1 LANL EVAL-FEB98 G.HALE 125 1451 5 + CH99 DIST-DEC06 REV1- 19990907 125 1451 6 +----ENDF/B-VII MATERIAL 125 REVISION 1 125 1451 7 +-----INCIDENT PROTON DATA 125 1451 8 +------ENDF-6 FORMAT 125 1451 9 + 125 1451 10 + **************************************************************** 125 1451 11 + 125 1451 12 + ENDF/B-VI MOD 2 Evaluation, February 1998, G. M. Hale (LANL) 125 1451 13 + 125 1451 14 + Includes p + H1 elastic MT = 2 125 1451 15 + 125 1451 16 + p-p elastic cross sections calculated for Ep between 0 and 125 1451 17 + 150 MeV from an R-matrix analysis of p-p cross-section and 125 1451 18 + polarization data in this energy range. The maximum nuclear 125 1451 19 + partial wave allowed in the fit is l=6, and the resulting 125 1451 20 + chi-squared per degree of freedom is 1.8. 125 1451 21 + 125 1451 22 + **************************************************************** 125 1451 23 + 125 1451 24 + ENDF/B-VI MOD 1 Evaluation, October 1987, D. Dodder (LANL) 125 1451 25 + 125 1451 26 + Completely replaced by MOD 2 evaluation. 125 1451 27 + 125 1451 28 +**************************************************************** 125 1451 29 + 125 1451 30 +REFERENCES 125 1451 31 + 125 1451 32 +[Ch99] M.B. Chadwick, P G. Young, G. M. Hale, et al., Los Alamos 125 1451 33 + National Laboratory report, LA-UR-99-1222 (1999) 125 1451 34 + 125 1451 35 + ************************ C O N T E N T S ************************ 125 1451 36 + 1 451 39 1 125 1451 37 + 6 2 661 1 125 1451 38 + 0.000000+0 0.000000+0 0 0 0 0 125 1 099999 + 0.000000+0 0.000000+0 0 0 0 0 125 0 0 0 + 1.001000+3 9.991700-1 0 2 1 0 125 6 2 1 + 1.001000+3 9.966200-1 0 5 1 2 125 6 2 2 + 2 2 125 6 2 3 + 1.000000+3 1.000000+0 1.500000+8 1.000000+0 125 6 2 4 + 5.000000-1 0.000000+0 1 0 1 131 125 6 2 5 + 131 2 125 6 2 6 + 0.000000+0 1.000000+3 1 0 21 6 125 6 2 7 + 0.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0 125 6 2 8 + 0.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0 125 6 2 9 + 0.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0 125 6 2 10 + 0.000000+0 0.000000+0 0.000000+0 125 6 2 11 + 0.000000+0 2.000000+4 1 0 21 6 125 6 2 12 + 4.913300-5-1.84640-12 2.43950-19-1.66800-20-1.91330-20 2.71050-20 125 6 2 13 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1.247500-3 8.521700-4 9.208800-4 3.320700-4 125 6 2 644 + 3.183500-5 6.849900-4 7.374800-5-1.161000-4-5.685200-6 6.128200-5 125 6 2 645 + 6.862100-6-3.663800-5-2.642300-6 125 6 2 646 + 0.000000+0 1.300000+8 1 0 21 6 125 6 2 647 + 8.002800-3 3.667700-4 4.729400-5-7.285600-6 7.595700-6 2.559800-6 125 6 2 648 + 4.599200-7 2.204000-3 8.829400-4 9.832300-4 9.835900-4 4.082100-4 125 6 2 649 + 4.515100-5 3.495900-4 3.528300-5-7.667200-5-3.957500-6 3.957000-5 125 6 2 650 + 3.451800-6-2.616200-5-1.852200-6 125 6 2 651 + 0.000000+0 1.400000+8 1 0 21 6 125 6 2 652 + 8.012900-3 3.019100-4 3.066000-5-5.307700-6-1.458800-6 6.215000-7 125 6 2 653 + 3.520700-9 1.730700-3 5.577300-4 1.060000-3 1.079100-3 5.510900-4 125 6 2 654 + 7.677100-5-8.305300-5 1.640700-6-1.535200-5-9.084600-7 2.810500-5 125 6 2 655 + 2.128200-6-2.205500-6-1.594900-7 125 6 2 656 + 0.000000+0 1.500000+8 1 0 21 6 125 6 2 657 + 9.283100-3 4.540700-4 2.309700-4 1.386200-4 4.412100-5 4.820100-6 125 6 2 658 + 1.252100-6 1.239400-3 2.931600-4 1.053000-3 1.209400-3 7.707700-4 125 6 2 659 + 1.445700-4-5.740300-4-2.038600-7 6.595800-5 4.754900-6 6.237400-5 125 6 2 660 + 7.335900-6 4.016600-5 3.133500-6 125 6 2 661 + 0.000000+0 0.000000+0 0 0 0 0 125 6 099999 + 0.000000+0 0.000000+0 0 0 0 0 125 0 0 0 + 0.000000+0 0.000000+0 0 0 0 0 0 0 0 0 + 1.001000+3 9.991700-1 -1 0 0 2 125 1451 1 + 0.000000+0 0.000000+0 0 0 0 6 125 1451 2 + 9.986200-1 1.500000+8 6 0 10010 6 125 1451 3 + 0.000000+0 0.000000+0 0 0 32 2 125 1451 4 + 1-H - 1 LANL EVAL-FEB98 G.HALE 125 1451 5 + Ch99 DIST-AUG99 REV1- 19990907 125 1451 6 +----ENDF/B-VI MATERIAL 125 REVISION 1 125 1451 7 +-----INCIDENT PROTON DATA 125 1451 8 +------ENDF-6 FORMAT 125 1451 9 + 125 1451 10 + **************************************************************** 125 1451 11 + 125 1451 12 + ENDF/B-VI MOD 2 Evaluation, February 1998, G. M. Hale (LANL) 125 1451 13 + 125 1451 14 + Includes p + H1 elastic MT = 2 125 1451 15 + 125 1451 16 + p-p elastic cross sections calculated for Ep between 0 and 125 1451 17 + 150 MeV from an R-matrix analysis of p-p cross-section and 125 1451 18 + polarization data in this energy range. The maximum nuclear 125 1451 19 + partial wave allowed in the fit is l=6, and the resulting 125 1451 20 + chi-squared per degree of freedom is 1.8. 125 1451 21 + 125 1451 22 + **************************************************************** 125 1451 23 + 125 1451 24 + ENDF/B-VI MOD 1 Evaluation, October 1987, D. Dodder (LANL) 125 1451 25 + 125 1451 26 + Completely replaced by MOD 2 evaluation. 125 1451 27 + 125 1451 28 +**************************************************************** 125 1451 29 + 125 1451 30 +REFERENCES 125 1451 31 + 125 1451 32 +[Ch99] M.B. Chadwick, P G. Young, G. M. Hale, et al., Los Alamos 125 1451 33 + National Laboratory report, LA-UR-99-1222 (1999) 125 1451 34 + 125 1451 35 + ************************ C O N T E N T S ************************ 125 1451 36 + 1 451 39 1 125 1451 37 + 6 2 661 1 125 1451 38 + 0.000000+0 0.000000+0 0 0 0 0 125 1 099999 + 0.000000+0 0.000000+0 0 0 0 0 125 0 0 0 + 1.001000+3 9.991700-1 0 2 1 0 125 6 2 1 + 1.001000+3 9.966200-1 0 5 1 2 125 6 2 2 + 2 2 125 6 2 3 + 1.000000+3 1.000000+0 1.500000+8 1.000000+0 125 6 2 4 + 5.000000-1 0.000000+0 1 0 1 131 125 6 2 5 + 131 2 125 6 2 6 + 0.000000+0 1.000000+3 1 0 21 6 125 6 2 7 + 0.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0 125 6 2 8 + 0.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0 125 6 2 9 + 0.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0 125 6 2 10 + 0.000000+0 0.000000+0 0.000000+0 125 6 2 11 + 0.000000+0 2.000000+4 1 0 21 6 125 6 2 12 + 4.913300-5-1.84640-12 2.43950-19-1.66800-20-1.91330-20 2.71050-20 125 6 2 13 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2.931600-4 1.053000-3 1.209400-3 7.707700-4 125 6 2 659 + 1.445700-4-5.740300-4-2.038600-7 6.595800-5 4.754900-6 6.237400-5 125 6 2 660 + 7.335900-6 4.016600-5 3.133500-6 125 6 2 661 + 0.000000+0 0.000000+0 0 0 0 0 125 6 099999 + 0.000000+0 0.000000+0 0 0 0 0 125 0 0 0 + 0.000000+0 0.000000+0 0 0 0 0 0 0 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 2 125 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 + 6 2 29 1 125 1451 48 + 125 1 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 + 1.001000+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 3.000000+9 1 0 10010 1 125 1451 3 + 0.000000+0 0.000000+0 1 0 53 2 125 1451 4 + 1-H - 1 JAERI EVAL-APR93 S.CHIBA 125 1451 5 +NST33(1996)654 DIST- 125 1451 6 +----JENDL/HE MATERIAL 125 125 1451 7 +-----INCIDENT PROTON DATA 125 1451 8 +------ENDF-6 FORMAT 125 1451 9 +HISTORY 125 1451 10 +93-04 Evaluation was performed by S. Cshiba (JAERI), S. Morioka 125 1451 11 + (CRC) and T. Fukahori for JENDL High Energy File. 125 1451 12 + Details are given in Ref. /1/. 125 1451 13 +03-05 Compiled by T. Fukahori for JENDL/HE. 125 1451 14 +04-02 Reviewed by T. Hino (Hitachi). 125 1451 15 + 125 1451 16 +MF=1 General Information 125 1451 17 + MT=451 Descriptive Data and Dictionary 125 1451 18 + 125 1451 19 +MF=3 Cross Sections 125 1451 20 + MT=2 Elastic Scattering Cross Section 125 1451 21 + Based on phase-shift data of Arndt et al./3,4/. 125 1451 22 + MT=3 Non-elastic Scattering Cross Section 125 1451 23 + Equal to MT=5. 125 1451 24 + MT=5 Inelastic Scattering Cross Section 125 1451 25 + This is a sum of the pion production cross sections. 125 1451 26 + Calculated by the phase-shift data/3,4/. 125 1451 27 + MT=201 Neutron production 125 1451 28 + Data calculated by JAM code. This neutron comes only from 125 1451 29 + H-1(p,nPI+)H-1 and H-1(p,2PI+)2n reactions. 125 1451 30 + MT=203 Proton production 125 1451 31 + Data calculated by JAM code. This proton comes only from 125 1451 32 + H-1(p,PI0)2p reaction. 125 1451 33 + MT=208 Positive pion production 125 1451 34 + Data calculated by JAM code. 125 1451 35 + MT=209 Non-charge pion production 125 1451 36 + Data calculated by JAM code. 125 1451 37 + MT=210 Negative pion production 125 1451 38 + Data calculated by JAM code. 125 1451 39 + Sum of MT=208-210 is normalized to MT=5. 125 1451 40 + 125 1451 41 +MF=6 Double-differential cross section 125 1451 42 + MT=2 125 1451 43 + Based on phase-shift data of Arndt et al./3,4/. 125 1451 44 + MT=201 Neutron production 125 1451 45 + Data calculated by JAM code. This neutron comes only from 125 1451 46 + H-1(p,nPI+)H-1 and H-1(p,2PI+)2n reactions. 125 1451 47 + MT=203 Proton production 125 1451 48 + Data calculated by JAM code. This proton comes only from 125 1451 49 + H-1(p,PI0)2p reaction. 125 1451 50 + MT=208 Positive pion production 125 1451 51 + Data calculated by JAM code. 125 1451 52 + MT=209 Non-charge pion production 125 1451 53 + Data calculated by JAM code. 125 1451 54 + MT=210 Negative pion production 125 1451 55 + Data calculated by JAM code. 125 1451 56 + 125 1451 57 + 1 451 69 0 125 1451 58 + 6 2 85 1 125 1451 59 + 125 1 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 24 125 6 2 2 + 24 2 0 0 0 0 125 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 3.000000+8 2.465400-2 4.000000+8 2.546600-2 125 6 2 6 + 4.500000+8 2.599500-2 5.000000+8 2.634100-2 5.500000+8 2.647200-2 125 6 2 7 + 6.000000+8 2.591100-2 6.500000+8 2.519000-2 7.000000+8 2.515900-2 125 6 2 8 + 7.500000+8 2.579200-2 8.000000+8 2.521500-2 8.500000+8 2.474600-2 125 6 2 9 + 9.000000+8 2.442200-2 9.500000+8 2.335000-2 9.990000+8 2.430500-2 125 6 2 10 + 1.050000+9 2.433900-2 1.100000+9 2.446200-2 3.000000+9 2.446200-2 125 6 2 11 + 5.000000-1 0.000000+0 1 0 1 24 125 6 2 12 + 24 22 0 0 0 0 125 6 2 13 + 0.00000+00 1.00000+03 2 0 7 6 125 6 2 14 + 1.24660-01 4.34000-04 3.10110-05-1.67860-05 1.78150-06 6.78030-07 125 6 2 15 + 0.00000+00 125 6 2 16 + 0.00000+00 1.00000+07 2 0 7 6 125 6 2 17 + 1.24660-01 4.34000-04 3.10110-05-1.67860-05 1.78150-06 6.78030-07 125 6 2 18 + 0.00000+00 125 6 2 19 + 0.00000+00 2.50000+07 2 0 7 6 125 6 2 20 + 4.49640-02 4.84990-04 1.56230-05-5.19380-05 8.77660-06 3.63650-06 125 6 2 21 + 0.00000+00 125 6 2 22 + 0.00000+00 5.00000+07 2 0 7 6 125 6 2 23 + 2.05440-02 4.83310-04 3.66580-05-6.17960-05 2.05030-05 8.54450-06 125 6 2 24 + 8.63270-09 125 6 2 25 + 0.00000+00 1.00000+08 2 0 7 6 125 6 2 26 + 1.07770-02 4.13600-04 1.26550-04-5.60270-05 3.93160-05 1.59470-05 125 6 2 27 + 1.07900-07 125 6 2 28 + 0.00000+00 1.50000+08 2 0 7 6 125 6 2 29 + 8.70780-03 3.39640-04 1.47420-04-5.74430-05 4.38590-05 2.02860-05 125 6 2 30 + 2.87750-07 125 6 2 31 + 0.00000+00 2.00000+08 2 0 7 6 125 6 2 32 + 8.04610-03 2.17080-04 1.44300-04-6.18590-05 4.65750-05 2.23380-05 125 6 2 33 + 5.18490-07 125 6 2 34 + 0.00000+00 3.00000+08 2 0 7 6 125 6 2 35 + 7.84760-03 1.35750-04 1.49270-04-6.60780-05 5.65910-05 2.24340-05 125 6 2 36 + 1.01030-06 125 6 2 37 + 0.00000+00 4.00000+08 2 0 7 6 125 6 2 38 + 8.10620-03 2.60050-04 1.62550-04-5.24020-05 5.42150-05 2.27490-05 125 6 2 39 + 1.56090-06 125 6 2 40 + 0.00000+00 4.50000+08 2 0 7 6 125 6 2 41 + 8.27450-03 3.65950-04 1.82620-04-2.17570-05 5.89210-05 2.19650-05 125 6 2 42 + 1.86270-06 125 6 2 43 + 0.00000+00 5.00000+08 2 0 7 6 125 6 2 44 + 8.38460-03 5.42320-04 1.57030-04-1.92110-05 5.57520-05 2.38560-05 125 6 2 45 + 2.12690-06 125 6 2 46 + 0.00000+00 5.50000+08 2 0 7 6 125 6 2 47 + 8.42610-03 8.36400-04 1.16150-04 1.66420-05 6.22960-05 2.52880-05 125 6 2 48 + 2.39620-06 125 6 2 49 + 0.00000+00 6.00000+08 2 0 7 6 125 6 2 50 + 8.24760-03 1.23640-03 1.16500-04 1.85370-05 5.75800-05 2.53870-05 125 6 2 51 + 2.75990-06 125 6 2 52 + 0.00000+00 6.50000+08 2 0 7 6 125 6 2 53 + 8.01820-03 1.63770-03 1.76100-04 5.15680-05 6.41320-05 2.74140-05 125 6 2 54 + 3.04790-06 125 6 2 55 + 0.00000+00 7.00000+08 2 0 7 6 125 6 2 56 + 8.00840-03 2.17850-03 2.75180-04 3.28800-05 5.21860-05 2.70880-05 125 6 2 57 + 3.35060-06 125 6 2 58 + 0.00000+00 7.50000+08 2 0 7 6 125 6 2 59 + 8.21000-03 2.69270-03 4.00940-04 6.93580-05 6.23030-05 2.90430-05 125 6 2 60 + 3.67460-06 125 6 2 61 + 0.00000+00 8.00000+08 2 0 7 6 125 6 2 62 + 8.02620-03 2.91540-03 4.60460-04 6.61940-05 6.40430-05 3.19010-05 125 6 2 63 + 4.02670-06 125 6 2 64 + 0.00000+00 8.50000+08 2 0 7 6 125 6 2 65 + 7.87710-03 3.19380-03 6.16110-04 9.95190-05 6.55370-05 3.25550-05 125 6 2 66 + 4.41870-06 125 6 2 67 + 0.00000+00 9.00000+08 2 0 7 6 125 6 2 68 + 7.77380-03 3.38300-03 7.09880-04 9.90380-05 7.24630-05 4.14530-05 125 6 2 69 + 6.81050-06 125 6 2 70 + 0.00000+00 9.50000+08 2 0 7 6 125 6 2 71 + 7.43240-03 3.35190-03 7.67020-04 1.39400-04 7.45170-05 3.38890-05 125 6 2 72 + 4.18770-06 125 6 2 73 + 0.00000+00 9.99000+08 2 0 7 6 125 6 2 74 + 7.73650-03 3.66390-03 9.25980-04 1.63350-04 7.04450-05 4.28220-05 125 6 2 75 + 7.49330-06 125 6 2 76 + 0.00000+00 1.05000+09 2 0 7 6 125 6 2 77 + 7.74730-03 3.75850-03 9.84150-04 2.06600-04 1.02700-04 5.37120-05 125 6 2 78 + 8.36170-06 125 6 2 79 + 0.00000+00 1.10000+09 2 0 7 6 125 6 2 80 + 7.78670-03 3.95300-03 1.16590-03 3.28120-04 1.34690-04 4.93790-05 125 6 2 81 + 6.23940-06 125 6 2 82 + 0.000000+0 3.000000+9 2 0 7 6 125 6 2 83 + 7.78670-03 3.95300-03 1.16590-03 3.28120-04 1.34690-04 4.93790-05 125 6 2 84 + 6.23940-06 125 6 2 85 + 125 6 099999 + 125 0 0 0 + 0 0 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 3.000000+9 1 0 10010 1 125 1451 3 + 0.000000+0 0.000000+0 1 0 58 2 125 1451 4 + 1-H - 1 JAERI EVAL-APR93 S.CHIBA 125 1451 5 +NST33(1996)654 DIST- 125 1451 6 +----JENDL/HE MATERIAL 125 125 1451 7 +-----INCIDENT PROTON DATA 125 1451 8 +------ENDF-6 FORMAT 125 1451 9 +HISTORY 125 1451 10 +93-04 Evaluation was performed by S. Cshiba (JAERI), S. Morioka 125 1451 11 + (CRC) and T. Fukahori for JENDL High Energy File. 125 1451 12 + Details are given in Ref. /1/. 125 1451 13 +03-05 Compiled by T. Fukahori for JENDL/HE. 125 1451 14 +04-02 Reviewed by T. Hino (Hitachi). 125 1451 15 + 125 1451 16 +MF=1 General Information 125 1451 17 + MT=451 Descriptive Data and Dictionary 125 1451 18 + 125 1451 19 +MF=3 Cross Sections 125 1451 20 + MT=2 Elastic Scattering Cross Section 125 1451 21 + Based on phase-shift data of Arndt et al./3,4/. 125 1451 22 + MT=3 Non-elastic Scattering Cross Section 125 1451 23 + Equal to MT=4. 125 1451 24 + MT=4 Total Inelastic Scattering Cross Section 125 1451 25 + Equal to MT=51. 125 1451 26 + MT=51 Inelastic Scattering Cross Section 125 1451 27 + This is a sum of the pion production cross sections. 125 1451 28 + Calculated by the phase-shift data/3,4/. 125 1451 29 + MT=201 Neutron production 125 1451 30 + Data calculated by JAM code. This neutron comes only from 125 1451 31 + H-1(p,nPI+)H-1 and H-1(p,2PI+)2n reactions. 125 1451 32 + MT=203 Proton production 125 1451 33 + Data calculated by JAM code. This proton comes only from 125 1451 34 + H-1(p,PI0)2p reaction. 125 1451 35 + MT=208 Positive pion production 125 1451 36 + Data calculated by JAM code. 125 1451 37 + MT=209 Non-charge pion production 125 1451 38 + Data calculated by JAM code. 125 1451 39 + MT=210 Negative pion production 125 1451 40 + Data calculated by JAM code. 125 1451 41 + Sum of MT=208-210 is normalized to MT=51 (or MT=4). 125 1451 42 + 125 1451 43 +MF=6 Double-differential cross section 125 1451 44 + MT=2 125 1451 45 + Based on phase-shift data of Arndt et al./3,4/. 125 1451 46 + MT=51 Inelastic Scattering Cross Section 125 1451 47 + This is a sum of the pion production cross sections. 125 1451 48 + Calculated by the phase-shift data/3,4/. 125 1451 49 + MT=201 Neutron production 125 1451 50 + Data calculated by JAM code. This neutron comes only from 125 1451 51 + H-1(p,nPI+)H-1 and H-1(p,2PI+)2n reactions. 125 1451 52 + MT=203 Proton production 125 1451 53 + Data calculated by JAM code. This proton comes only from 125 1451 54 + H-1(p,PI0)2p reaction. 125 1451 55 + MT=208 Positive pion production 125 1451 56 + Data calculated by JAM code. 125 1451 57 + MT=209 Non-charge pion production 125 1451 58 + Data calculated by JAM code. 125 1451 59 + MT=210 Negative pion production 125 1451 60 + Data calculated by JAM code. 125 1451 61 + 125 1451 62 + 1 451 79 1 125 1451 63 + 6 2 109 1 125 1451 64 + 125 1 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 24 125 6 2 2 + 24 2 0 0 0 0 125 6 2 3 + 1.000000-5 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 3.000000+8 2.465400-2 4.000000+8 2.546600-2 125 6 2 6 + 4.500000+8 2.599500-2 5.000000+8 2.634100-2 5.500000+8 2.647200-2 125 6 2 7 + 6.000000+8 2.591100-2 6.500000+8 2.519000-2 7.000000+8 2.515900-2 125 6 2 8 + 7.500000+8 2.579200-2 8.000000+8 2.521500-2 8.500000+8 2.474600-2 125 6 2 9 + 9.000000+8 2.442200-2 9.500000+8 2.335000-2 9.990000+8 2.430500-2 125 6 2 10 + 1.050000+9 2.433900-2 1.100000+9 2.446200-2 3.000000+9 2.446200-2 125 6 2 11 + 5.000000-1 0.000000+0 1 0 1 24 125 6 2 12 + 24 22 0 0 0 0 125 6 2 13 + 0.000000+0 1.000000-5 2 0 13 12 125 6 2 14 + 1.000000+0 0.000000+0 3.481400-3 0.000000+0 2.487600-4 0.000000+0 125 6 2 15 +-1.346500-4 0.000000+0 1.429100-5 0.000000+0 5.439000-6 0.000000+0 125 6 2 16 + 0.000000+0 125 6 2 17 + 0.000000+0 1.000000+7 2 0 13 12 125 6 2 18 + 1.000000+0 0.000000+0 3.481400-3 0.000000+0 2.487600-4 0.000000+0 125 6 2 19 +-1.346500-4 0.000000+0 1.429100-5 0.000000+0 5.439000-6 0.000000+0 125 6 2 20 + 0.000000+0 125 6 2 21 + 0.000000+0 2.500000+7 2 0 13 12 125 6 2 22 + 1.000000+0 0.000000+0 1.078600-2 0.000000+0 3.474600-4 0.000000+0 125 6 2 23 +-1.155100-3 0.000000+0 1.951900-4 0.000000+0 8.087500-5 0.000000+0 125 6 2 24 + 0.000000+0 125 6 2 25 + 0.000000+0 5.000000+7 2 0 13 12 125 6 2 26 + 1.000000+0 0.000000+0 2.352600-2 0.000000+0 1.784400-3 0.000000+0 125 6 2 27 +-3.008000-3 0.000000+0 9.980300-4 0.000000+0 4.159200-4 0.000000+0 125 6 2 28 + 4.202100-7 125 6 2 29 + 0.000000+0 1.000000+8 2 0 13 12 125 6 2 30 + 1.000000+0 0.000000+0 3.837700-2 0.000000+0 1.174200-2 0.000000+0 125 6 2 31 +-5.198700-3 0.000000+0 3.648100-3 0.000000+0 1.479700-3 0.000000+0 125 6 2 32 + 1.001200-5 125 6 2 33 + 0.000000+0 1.500000+8 2 0 13 12 125 6 2 34 + 1.000000+0 0.000000+0 3.900400-2 0.000000+0 1.692900-2 0.000000+0 125 6 2 35 +-6.596700-3 0.000000+0 5.036700-3 0.000000+0 2.329600-3 0.000000+0 125 6 2 36 + 3.304500-5 125 6 2 37 + 0.000000+0 2.000000+8 2 0 13 12 125 6 2 38 + 1.000000+0 0.000000+0 2.697900-2 0.000000+0 1.793400-2 0.000000+0 125 6 2 39 +-7.688100-3 0.000000+0 5.788500-3 0.000000+0 2.776300-3 0.000000+0 125 6 2 40 + 6.444000-5 125 6 2 41 + 0.000000+0 3.000000+8 2 0 13 12 125 6 2 42 + 1.000000+0 0.000000+0 1.729800-2 0.000000+0 1.902100-2 0.000000+0 125 6 2 43 +-8.420200-3 0.000000+0 7.211300-3 0.000000+0 2.858700-3 0.000000+0 125 6 2 44 + 1.287400-4 125 6 2 45 + 0.000000+0 4.000000+8 2 0 13 12 125 6 2 46 + 1.000000+0 0.000000+0 3.208000-2 0.000000+0 2.005200-2 0.000000+0 125 6 2 47 +-6.464400-3 0.000000+0 6.688000-3 0.000000+0 2.806300-3 0.000000+0 125 6 2 48 + 1.925500-4 125 6 2 49 + 0.000000+0 4.500000+8 2 0 13 12 125 6 2 50 + 1.000000+0 0.000000+0 4.422700-2 0.000000+0 2.207000-2 0.000000+0 125 6 2 51 +-2.629400-3 0.000000+0 7.120800-3 0.000000+0 2.654500-3 0.000000+0 125 6 2 52 + 2.251200-4 125 6 2 53 + 0.000000+0 5.000000+8 2 0 13 12 125 6 2 54 + 1.000000+0 0.000000+0 6.468000-2 0.000000+0 1.872800-2 0.000000+0 125 6 2 55 +-2.291200-3 0.000000+0 6.649300-3 0.000000+0 2.845200-3 0.000000+0 125 6 2 56 + 2.536700-4 125 6 2 57 + 0.000000+0 5.500000+8 2 0 13 12 125 6 2 58 + 1.000000+0 0.000000+0 9.926200-2 0.000000+0 1.378500-2 0.000000+0 125 6 2 59 + 1.975000-3 0.000000+0 7.393200-3 0.000000+0 3.001100-3 0.000000+0 125 6 2 60 + 2.843800-4 125 6 2 61 + 0.000000+0 6.000000+8 2 0 13 12 125 6 2 62 + 1.000000+0 0.000000+0 1.499100-1 0.000000+0 1.412500-2 0.000000+0 125 6 2 63 + 2.247600-3 0.000000+0 6.981400-3 0.000000+0 3.078100-3 0.000000+0 125 6 2 64 + 3.346300-4 125 6 2 65 + 0.000000+0 6.500000+8 2 0 13 12 125 6 2 66 + 1.000000+0 0.000000+0 2.042500-1 0.000000+0 2.196300-2 0.000000+0 125 6 2 67 + 6.431300-3 0.000000+0 7.998300-3 0.000000+0 3.419000-3 0.000000+0 125 6 2 68 + 3.801200-4 125 6 2 69 + 0.000000+0 7.000000+8 2 0 13 12 125 6 2 70 + 1.000000+0 0.000000+0 2.720300-1 0.000000+0 3.436100-2 0.000000+0 125 6 2 71 + 4.105700-3 0.000000+0 6.516400-3 0.000000+0 3.382500-3 0.000000+0 125 6 2 72 + 4.183900-4 125 6 2 73 + 0.000000+0 7.500000+8 2 0 13 12 125 6 2 74 + 1.000000+0 0.000000+0 3.279800-1 0.000000+0 4.883500-2 0.000000+0 125 6 2 75 + 8.448000-3 0.000000+0 7.588700-3 0.000000+0 3.537500-3 0.000000+0 125 6 2 76 + 4.475700-4 125 6 2 77 + 0.000000+0 8.000000+8 2 0 13 12 125 6 2 78 + 1.000000+0 0.000000+0 3.632300-1 0.000000+0 5.737000-2 0.000000+0 125 6 2 79 + 8.247200-3 0.000000+0 7.979200-3 0.000000+0 3.974600-3 0.000000+0 125 6 2 80 + 5.016900-4 125 6 2 81 + 0.000000+0 8.500000+8 2 0 13 12 125 6 2 82 + 1.000000+0 0.000000+0 4.054500-1 0.000000+0 7.821600-2 0.000000+0 125 6 2 83 + 1.263400-2 0.000000+0 8.320000-3 0.000000+0 4.132900-3 0.000000+0 125 6 2 84 + 5.609600-4 125 6 2 85 + 0.000000+0 9.000000+8 2 0 13 12 125 6 2 86 + 1.000000+0 0.000000+0 4.351800-1 0.000000+0 9.131800-2 0.000000+0 125 6 2 87 + 1.274000-2 0.000000+0 9.321500-3 0.000000+0 5.332400-3 0.000000+0 125 6 2 88 + 8.760900-4 125 6 2 89 + 0.000000+0 9.500000+8 2 0 13 12 125 6 2 90 + 1.000000+0 0.000000+0 4.509800-1 0.000000+0 1.032000-1 0.000000+0 125 6 2 91 + 1.875600-2 0.000000+0 1.002600-2 0.000000+0 4.559700-3 0.000000+0 125 6 2 92 + 5.634400-4 125 6 2 93 + 0.000000+0 9.990000+8 2 0 13 12 125 6 2 94 + 1.000000+0 0.000000+0 4.735900-1 0.000000+0 1.196900-1 0.000000+0 125 6 2 95 + 2.111400-2 0.000000+0 9.105500-3 0.000000+0 5.535100-3 0.000000+0 125 6 2 96 + 9.685600-4 125 6 2 97 + 0.000000+0 1.050000+9 2 0 13 12 125 6 2 98 + 1.000000+0 0.000000+0 4.851400-1 0.000000+0 1.270300-1 0.000000+0 125 6 2 99 + 2.666700-2 0.000000+0 1.325600-2 0.000000+0 6.933000-3 0.000000+0 125 6 2 100 + 1.079300-3 125 6 2 101 + 0.000000+0 1.100000+9 2 0 13 12 125 6 2 102 + 1.000000+0 0.000000+0 5.076600-1 0.000000+0 1.497300-1 0.000000+0 125 6 2 103 + 4.213900-2 0.000000+0 1.729800-2 0.000000+0 6.341500-3 0.000000+0 125 6 2 104 + 8.012900-4 125 6 2 105 + 0.000000+0 3.000000+9 2 0 13 12 125 6 2 106 + 1.000000+0 0.000000+0 5.076600-1 0.000000+0 1.497300-1 0.000000+0 125 6 2 107 + 4.213900-2 0.000000+0 1.729800-2 0.000000+0 6.341500-3 0.000000+0 125 6 2 108 + 8.012900-4 125 6 2 109 + 125 6 099999 + 125 0 0 0 + 0 0 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 3.000000+9 1 0 10010 1 125 1451 3 + 0.000000+0 0.000000+0 1 0 53 2 125 1451 4 + 1-H - 1 JAERI EVAL-APR93 S.CHIBA 125 1451 5 +NST33(1996)654 DIST- 125 1451 6 +----JENDL-1 MATERIAL 125 125 1451 7 +-----INCIDENT PROTON DATA 125 1451 8 +------ENDF-6 FORMAT 125 1451 9 +HISTORY 125 1451 10 +93-04 Evaluation was performed by S. Cshiba (JAERI), S. Morioka 125 1451 11 + (CRC) and T. Fukahori for JENDL High Energy File. 125 1451 12 + Details are given in Ref. /1/. 125 1451 13 +03-05 Compiled by T. Fukahori for JENDL/HE. 125 1451 14 +04-02 Reviewed by T. Hino (Hitachi). 125 1451 15 + 125 1451 16 +MF=1 General Information 125 1451 17 + MT=451 Descriptive Data and Dictionary 125 1451 18 + 125 1451 19 +MF=3 Cross Sections 125 1451 20 + MT=2 Elastic Scattering Cross Section 125 1451 21 + Based on phase-shift data of Arndt et al./3,4/. 125 1451 22 + MT=3 Non-elastic Scattering Cross Section 125 1451 23 + Equal to MT=5. 125 1451 24 + MT=5 Inelastic Scattering Cross Section 125 1451 25 + This is a sum of the pion production cross sections. 125 1451 26 + Calculated by the phase-shift data/3,4/. 125 1451 27 + MT=201 Neutron production 125 1451 28 + Data calculated by JAM code. This neutron comes only from 125 1451 29 + H-1(p,nPI+)H-1 and H-1(p,2PI+)2n reactions. 125 1451 30 + MT=203 Proton production 125 1451 31 + Data calculated by JAM code. This proton comes only from 125 1451 32 + H-1(p,PI0)2p reaction. 125 1451 33 + MT=208 Positive pion production 125 1451 34 + Data calculated by JAM code. 125 1451 35 + MT=209 Non-charge pion production 125 1451 36 + Data calculated by JAM code. 125 1451 37 + MT=210 Negative pion production 125 1451 38 + Data calculated by JAM code. 125 1451 39 + Sum of MT=208-210 is normalized to MT=5. 125 1451 40 + 125 1451 41 +MF=6 Double-differential cross section 125 1451 42 + MT=2 125 1451 43 + Based on phase-shift data of Arndt et al./3,4/. 125 1451 44 + MT=201 Neutron production 125 1451 45 + Data calculated by JAM code. This neutron comes only from 125 1451 46 + H-1(p,nPI+)H-1 and H-1(p,2PI+)2n reactions. 125 1451 47 + MT=203 Proton production 125 1451 48 + Data calculated by JAM code. This proton comes only from 125 1451 49 + H-1(p,PI0)2p reaction. 125 1451 50 + MT=208 Positive pion production 125 1451 51 + Data calculated by JAM code. 125 1451 52 + MT=209 Non-charge pion production 125 1451 53 + Data calculated by JAM code. 125 1451 54 + MT=210 Negative pion production 125 1451 55 + Data calculated by JAM code. 125 1451 56 + 125 1451 57 + 1 451 63 0 125 1451 58 + 6 2 85 1 125 1451 59 + 0.000000+0 0.000000+0 0 0 0 0 125 1 099999 + 0.000000+0 0.000000+0 0 0 0 0 125 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 24 125 6 2 2 + 24 2 0 0 0 0 125 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 3.000000+8 2.465400-2 4.000000+8 2.546600-2 125 6 2 6 + 4.500000+8 2.599500-2 5.000000+8 2.634100-2 5.500000+8 2.647200-2 125 6 2 7 + 6.000000+8 2.591100-2 6.500000+8 2.519000-2 7.000000+8 2.515900-2 125 6 2 8 + 7.500000+8 2.579200-2 8.000000+8 2.521500-2 8.500000+8 2.474600-2 125 6 2 9 + 9.000000+8 2.442200-2 9.500000+8 2.335000-2 9.990000+8 2.430500-2 125 6 2 10 + 1.050000+9 2.433900-2 1.100000+9 2.446200-2 3.000000+9 2.446200-2 125 6 2 11 + 5.000000-1 0.000000+0 1 0 1 24 125 6 2 12 + 24 22 0 0 0 0 125 6 2 13 + 0.00000+00 1.00000+03 2 0 7 6 125 6 2 14 + 1.24660-01 4.34000-04 3.10110-05-1.67860-05 1.78150-06 6.78030-07 125 6 2 15 + 0.00000+00 125 6 2 16 + 0.00000+00 1.00000+07 2 0 7 6 125 6 2 17 + 1.24660-01 4.34000-04 3.10110-05-1.67860-05 1.78150-06 6.78030-07 125 6 2 18 + 0.00000+00 125 6 2 19 + 0.00000+00 2.50000+07 2 0 7 6 125 6 2 20 + 4.49640-02 4.84990-04 1.56230-05-5.19380-05 8.77660-06 3.63650-06 125 6 2 21 + 0.00000+00 125 6 2 22 + 0.00000+00 5.00000+07 2 0 7 6 125 6 2 23 + 2.05440-02 4.83310-04 3.66580-05-6.17960-05 2.05030-05 8.54450-06 125 6 2 24 + 8.63270-09 125 6 2 25 + 0.00000+00 1.00000+08 2 0 7 6 125 6 2 26 + 1.07770-02 4.13600-04 1.26550-04-5.60270-05 3.93160-05 1.59470-05 125 6 2 27 + 1.07900-07 125 6 2 28 + 0.00000+00 1.50000+08 2 0 7 6 125 6 2 29 + 8.70780-03 3.39640-04 1.47420-04-5.74430-05 4.38590-05 2.02860-05 125 6 2 30 + 2.87750-07 125 6 2 31 + 0.00000+00 2.00000+08 2 0 7 6 125 6 2 32 + 8.04610-03 2.17080-04 1.44300-04-6.18590-05 4.65750-05 2.23380-05 125 6 2 33 + 5.18490-07 125 6 2 34 + 0.00000+00 3.00000+08 2 0 7 6 125 6 2 35 + 7.84760-03 1.35750-04 1.49270-04-6.60780-05 5.65910-05 2.24340-05 125 6 2 36 + 1.01030-06 125 6 2 37 + 0.00000+00 4.00000+08 2 0 7 6 125 6 2 38 + 8.10620-03 2.60050-04 1.62550-04-5.24020-05 5.42150-05 2.27490-05 125 6 2 39 + 1.56090-06 125 6 2 40 + 0.00000+00 4.50000+08 2 0 7 6 125 6 2 41 + 8.27450-03 3.65950-04 1.82620-04-2.17570-05 5.89210-05 2.19650-05 125 6 2 42 + 1.86270-06 125 6 2 43 + 0.00000+00 5.00000+08 2 0 7 6 125 6 2 44 + 8.38460-03 5.42320-04 1.57030-04-1.92110-05 5.57520-05 2.38560-05 125 6 2 45 + 2.12690-06 125 6 2 46 + 0.00000+00 5.50000+08 2 0 7 6 125 6 2 47 + 8.42610-03 8.36400-04 1.16150-04 1.66420-05 6.22960-05 2.52880-05 125 6 2 48 + 2.39620-06 125 6 2 49 + 0.00000+00 6.00000+08 2 0 7 6 125 6 2 50 + 8.24760-03 1.23640-03 1.16500-04 1.85370-05 5.75800-05 2.53870-05 125 6 2 51 + 2.75990-06 125 6 2 52 + 0.00000+00 6.50000+08 2 0 7 6 125 6 2 53 + 8.01820-03 1.63770-03 1.76100-04 5.15680-05 6.41320-05 2.74140-05 125 6 2 54 + 3.04790-06 125 6 2 55 + 0.00000+00 7.00000+08 2 0 7 6 125 6 2 56 + 8.00840-03 2.17850-03 2.75180-04 3.28800-05 5.21860-05 2.70880-05 125 6 2 57 + 3.35060-06 125 6 2 58 + 0.00000+00 7.50000+08 2 0 7 6 125 6 2 59 + 8.21000-03 2.69270-03 4.00940-04 6.93580-05 6.23030-05 2.90430-05 125 6 2 60 + 3.67460-06 125 6 2 61 + 0.00000+00 8.00000+08 2 0 7 6 125 6 2 62 + 8.02620-03 2.91540-03 4.60460-04 6.61940-05 6.40430-05 3.19010-05 125 6 2 63 + 4.02670-06 125 6 2 64 + 0.00000+00 8.50000+08 2 0 7 6 125 6 2 65 + 7.87710-03 3.19380-03 6.16110-04 9.95190-05 6.55370-05 3.25550-05 125 6 2 66 + 4.41870-06 125 6 2 67 + 0.00000+00 9.00000+08 2 0 7 6 125 6 2 68 + 7.77380-03 3.38300-03 7.09880-04 9.90380-05 7.24630-05 4.14530-05 125 6 2 69 + 6.81050-06 125 6 2 70 + 0.00000+00 9.50000+08 2 0 7 6 125 6 2 71 + 7.43240-03 3.35190-03 7.67020-04 1.39400-04 7.45170-05 3.38890-05 125 6 2 72 + 4.18770-06 125 6 2 73 + 0.00000+00 9.99000+08 2 0 7 6 125 6 2 74 + 7.73650-03 3.66390-03 9.25980-04 1.63350-04 7.04450-05 4.28220-05 125 6 2 75 + 7.49330-06 125 6 2 76 + 0.00000+00 1.05000+09 2 0 7 6 125 6 2 77 + 7.74730-03 3.75850-03 9.84150-04 2.06600-04 1.02700-04 5.37120-05 125 6 2 78 + 8.36170-06 125 6 2 79 + 0.00000+00 1.10000+09 2 0 7 6 125 6 2 80 + 7.78670-03 3.95300-03 1.16590-03 3.28120-04 1.34690-04 4.93790-05 125 6 2 81 + 6.23940-06 125 6 2 82 + 0.000000+0 3.000000+9 2 0 7 6 125 6 2 83 + 7.78670-03 3.95300-03 1.16590-03 3.28120-04 1.34690-04 4.93790-05 125 6 2 84 + 6.23940-06 125 6 2 85 + 125 6 099999 + 125 0 0 0 + 0 0 0 0 + 1.001000+3 9.991700-1 -1 0 0 2 125 1451 1 + 0.000000+0 0.000000+0 0 0 0 6 125 1451 2 + 9.986200-1 1.500000+8 1 0 10010 7 125 1451 3 + 0.000000+0 0.000000+0 0 0 32 2 125 1451 4 + 1-H - 1 LANL EVAL-FEB98 G.HALE 125 1451 5 + CH99 DIST-DEC06 REV1- 20111222 125 1451 6 +----ENDF/B-VII.1 MATERIAL 125 REVISION 1 125 1451 7 +-----INCIDENT PROTON DATA 125 1451 8 +------ENDF-6 FORMAT 125 1451 9 + 125 1451 10 + **************************************************************** 125 1451 11 + 125 1451 12 + ENDF/B-VI MOD 2 Evaluation, February 1998, G. M. Hale (LANL) 125 1451 13 + 125 1451 14 + Includes p + H1 elastic MT = 2 125 1451 15 + 125 1451 16 + p-p elastic cross sections calculated for Ep between 0 and 125 1451 17 + 150 MeV from an R-matrix analysis of p-p cross-section and 125 1451 18 + polarization data in this energy range. The maximum nuclear 125 1451 19 + partial wave allowed in the fit is l=6, and the resulting 125 1451 20 + chi-squared per degree of freedom is 1.8. 125 1451 21 + 125 1451 22 + **************************************************************** 125 1451 23 + 125 1451 24 + ENDF/B-VI MOD 1 Evaluation, October 1987, D. Dodder (LANL) 125 1451 25 + 125 1451 26 + Completely replaced by MOD 2 evaluation. 125 1451 27 + 125 1451 28 +**************************************************************** 125 1451 29 + 125 1451 30 +REFERENCES 125 1451 31 + 125 1451 32 +[Ch99] M.B. Chadwick, P G. Young, G. M. Hale, et al., Los Alamos 125 1451 33 + National Laboratory report, LA-UR-99-1222 (1999) 125 1451 34 + 125 1451 35 + ************************ C O N T E N T S ************************ 125 1451 36 + 1 451 39 1 125 1451 37 + 6 2 661 1 125 1451 38 + 0.000000+0 0.000000+0 0 0 0 0 125 1 099999 + 0.000000+0 0.000000+0 0 0 0 0 125 0 0 0 + 1.001000+3 9.991700-1 0 2 1 0 125 6 2 1 + 1.001000+3 9.966200-1 0 5 1 2 125 6 2 2 + 2 2 125 6 2 3 + 1.000000+3 1.000000+0 1.500000+8 1.000000+0 125 6 2 4 + 5.000000-1 0.000000+0 1 0 1 131 125 6 2 5 + 131 2 125 6 2 6 + 0.000000+0 1.000000+3 1 0 21 6 125 6 2 7 + 0.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0 125 6 2 8 + 0.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0 125 6 2 9 + 0.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0 125 6 2 10 + 0.000000+0 0.000000+0 0.000000+0 125 6 2 11 + 0.000000+0 2.000000+4 1 0 21 6 125 6 2 12 + 4.913300-5-1.84640-12 2.43950-19-1.66800-20-1.91330-20 2.71050-20 125 6 2 13 +-1.08420-21 3.193000-2 2.456600-5 1.704500-7-1.529200-6-6.45090-10 125 6 2 14 + 3.04170-10 3.86880-13 1.08180-13-1.76570-18-1.88320-18-3.02160-22 125 6 2 15 +-9.32390-22-2.57440-27 4.68080-26 125 6 2 16 + 0.000000+0 3.000000+4 1 0 21 6 125 6 2 17 + 4.418500-4-2.09530-11 5.34870-18 6.67200-20-1.53060-19 2.37490-19 125 6 2 18 +-1.04080-19 7.818000-2 2.209200-4-4.153400-7-4.533300-6-2.019900-9 125 6 2 19 + 2.105000-9 2.30990-12-5.05480-13-2.16370-17-5.13870-18-1.03320-20 125 6 2 20 +-6.98120-21 5.52570-25 6.90790-25 125 6 2 21 + 0.000000+0 4.000000+4 1 0 21 6 125 6 2 22 + 1.583100-3-7.77440-11 3.92240-17 1.06750-18-2.04090-19 5.16290-19 125 6 2 23 +-5.55110-19 1.281600-1 7.915500-4-2.014600-6-8.482500-6-3.543000-9 125 6 2 24 + 6.195500-9 6.48990-12-3.85640-12-9.24840-17 1.36020-17-6.83790-20 125 6 2 25 +-1.15620-20 5.93050-24 2.71580-24 125 6 2 26 + 0.000000+0 5.000000+4 1 0 21 6 125 6 2 27 + 3.720100-3-1.58880-10 1.72890-16 0.000000+0-8.16340-19 2.06510-18 125 6 2 28 +-9.02060-19 1.757100-1 1.860100-3-4.550400-6-1.285800-5-4.525500-9 125 6 2 29 + 1.282000-8 1.27540-11-1.23330-11-2.48950-16 1.10820-16-2.49180-19 125 6 2 30 + 3.45850-20 2.93390-23 2.84400-24 125 6 2 31 + 0.000000+0 6.000000+4 1 0 21 6 125 6 2 32 + 6.924900-3-1.95810-10 5.60510-16 3.20260-18-2.44900-18 5.78240-19 125 6 2 33 +-3.46940-18 2.188300-1 3.462400-3-7.848000-6-1.735500-5-4.437500-9 125 6 2 34 + 2.194300-8 2.02820-11-2.82140-11-5.15680-16 3.74110-16-6.55910-19 125 6 2 35 + 2.55100-19 9.75220-23-1.54020-23 125 6 2 36 + 0.000000+0 7.000000+4 1 0 21 6 125 6 2 37 + 1.116000-2-6.54170-11 1.45790-15-5.33760-18 4.89800-18-1.48690-18 125 6 2 38 +-1.94290-18 2.571600-1 5.579900-3-1.173700-5-2.180700-5-2.908600-9 125 6 2 39 + 3.341300-8 2.78660-11-5.35300-11-9.01190-16 9.17370-16-1.40460-18 125 6 2 40 + 8.73660-19 2.53160-22-9.47000-23 125 6 2 41 + 0.000000+0 8.000000+4 1 0 21 6 125 6 2 42 + 1.633300-2 4.00010-10 3.25590-15 1.49450-17-1.30610-17 7.93020-18 125 6 2 43 +-3.33070-18 2.909700-1 8.166700-3-1.607600-5-2.612700-5 3.10910-10 125 6 2 44 + 4.704800-8 3.40740-11-9.00520-11-1.39500-15 1.87620-15-2.60560-18 125 6 2 45 + 2.23420-18 5.54600-22-3.19800-22 125 6 2 46 + 0.000000+0 9.000000+4 1 0 21 6 125 6 2 47 + 2.233400-2 1.401300-9 6.57960-15 1.92150-17-9.79610-18 1.38780-17 125 6 2 48 +-4.44090-18 3.207200-1 1.116700-2-2.075300-5-3.027200-5 5.385400-9 125 6 2 49 + 6.265800-8 3.73560-11-1.39320-10-1.96670-15 3.40390-15-4.34440-18 125 6 2 50 + 4.81650-18 1.07280-21-8.35550-22 125 6 2 51 + 0.000000+0 1.000000+5 1 0 21 6 125 6 2 52 + 2.904800-2 3.162300-9 1.22030-14 1.28100-17 9.79610-18 7.59970-18 125 6 2 53 + 1.11020-18 3.469000-1 1.452400-2-2.568100-5-3.422300-5 1.242000-8 125 6 2 54 + 8.007000-8 3.61070-11-2.02670-10-2.56540-15 5.66890-15-6.66280-18 125 6 2 55 + 9.24960-18 1.88570-21-1.86660-21 125 6 2 56 + 0.000000+0 1.200000+5 1 0 21 6 125 6 2 57 + 4.419000-2 9.925000-9 3.46740-14 4.27010-17-3.26540-17 4.29550-17 125 6 2 58 +-2.22040-17 3.903000-1 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