JENDL/PD-2016 H - 2 0 0 0 0 1.002000+3 1.996800+0 -1 0 6 0 128 1451 1 0.000000+0 0.000000+0 0 0 0 6 128 1451 2 0.000000+0 1.400000+8 0 0 0 0 128 1451 3 0.000000+0 0.000000+0 0 0 72 4 128 1451 4 1- H - 2 NFD EVAL-Aug95 T.Murata 128 1451 5 DIST-DEC17 128 1451 6 ----JENDL/PD-2016 MATERIAL 128 128 1451 7 -----PHOTONUCLEAR DATA 128 1451 8 ------ENDF-6 FORMAT 128 1451 9 128 1451 10 History 128 1451 11 1995-08 Evaluation was performed by T.Murata (NFD) 128 1451 12 1995-08 Compiled by S. Chiba (JAERI) 128 1451 13 2000-02 Recompiled by T. Fukahori (JAERI) 128 1451 14 2003-06 Recompiled by T. Fukahori (JAERI) 128 1451 15 2003-06 Reviewed by H. Harada (JNC) 128 1451 16 128 1451 17 MF=1 General Information 128 1451 18 MT=451 Descriptive data and Dictionary 128 1451 19 Details of the evaluation are given in Ref./1/ 128 1451 20 128 1451 21 MF=3 Photon Cross Sections 128 1451 22 MT=3 Total photo-absorption cross section 128 1451 23 Incident energy below 10 MeV : 128 1451 24 Experimental cross sections/3/ were analysed with a 128 1451 25 simplified Marshall & Guth model/2/. 128 1451 26 Incident energy above 10 MeV : 128 1451 27 Partovi/4/ gives theoretical cross section which repro- 128 1451 28 duce experimental values fairly well. The theoretical 128 1451 29 results were fitted with the basically same model as des- 128 1451 30 cribed above. 128 1451 31 MT=28 (g,np) reaction cross section 128 1451 32 Same as total photo-absorption cross section (MT=3) 128 1451 33 Also same as (g,n) and (g,p) cross sections (MT=4,103) 128 1451 34 128 1451 35 MF=6 Energy-Angular Distribution of secondary particles 128 1451 36 MT=5 Particle production data 128 1451 37 Incident energy below 10 MeV : 128 1451 38 CM system angular distributions were calculated with the 128 1451 39 Marshall & Guth model/2/ plus magnetic dipole term. 128 1451 40 Incident energy above 10 MeV : 128 1451 41 CM system angular distributions given by Partovi/4/ 128 1451 42 were adopted. 128 1451 43 Confirming the agreement with experimental distributions 128 1451 44 /5/, the CM system distributions were transformed to LAB 128 1451 45 system with the relativistic kinematics/6/. Coefficients 128 1451 46 of Legendre polynomial expansion are given (L<=4). 128 1451 47 128 1451 48 References 128 1451 49 1) Murata, T. : JAERI-M 94-019, p.330 (1994). 128 1451 50 2) Marshall, J.F. and Guth,E.: Phys. Rev. 78, 738 (1950). 128 1451 51 3) Allen, L.Jr.: Phys. Rev. 98, 705 (1955), 128 1451 52 Alexandrov, I.A.et al.: Soviet Phys. JETP 6, 472 (1958), 128 1451 53 Whalin, B.A. et al.: Phys. Rev. 101, 377 (1956), 128 1451 54 Barns, J.H. et al.: Phys. Rev. 86, 359 (1952), 128 1451 55 Galey, J.A.: Phys. Rev. 117, 763 (1960), 128 1451 56 Phillips, J.A. et al.: Phys. Rev. 80, 326 (1950), 128 1451 57 Keck, J.C. et al.: Phys. Rev. 101, 360 (1956), 128 1451 58 Halpern, J. et al.: Phys. Rev. 91, 934 (1953), 128 1451 59 Hough, P.V.C.: Phys. Rev. 80, 1069 (1950), 128 1451 60 Bishop, G.R. et al.: Phys. Rev. 80, 211 (1950), 128 1451 61 Snell, A.H. et al.: Phys. Rev. 80, 637 (1950), 128 1451 62 McMurray, W.R. et al.: Proc. Phys. Soc. 68A, 181 (1955), 128 1451 63 Barnes, C.A. et al.: Phys. Rev. 86, 359 (1952), 128 1451 64 Waffler, H. et al.: Helv. Phys. Acta 24, 483 (1951), 128 1451 65 Birenbaum, Y. et al.: Phys. Rev. C32, 1825 (1985), 128 1451 66 Moreh, R. et al.: Phys. Rev. C39, 1247 (1989), 128 1451 67 Debevec, P.T. et al.: Phys. Rev. C45, 904 (1992). 128 1451 68 4) Partovi, F.: Ann. Physics 27, 79 (1964). 128 1451 69 5) Smith, F.D.: Nucl. Phys. 465, 429 (1987), 128 1451 70 Shin, Y.M.: Nucl. Phys. 154, 482 (1970), 128 1451 71 Alexandrov, I.A. et al.: Soviet Phys. JETP 6, 472 (1958), 128 1451 72 Keck, J.C. et al.: Phys. Rev. 101, 360 (1956), 128 1451 73 Whalin, B.A. et al.: Phys. Rev. 101, 377 (1956). 128 1451 74 6) Dedrick, K.G.: Rev. Mod. Phys. 34, 429 (1962). 128 1451 75 128 1451 76 1 451 80 0 128 1451 77 3 3 13 0 128 1451 78 3 28 13 0 128 1451 79 6 28 62 0 128 1451 80 128 1 099999 128 0 0 0 1.002000+3 1.996800+0 0 0 0 0 128 3 3 1 0.000000+0 0.000000+0 0 0 1 28 128 3 3 2 28 3 128 3 3 3 2.224000+6 0.000000+0 2.300000+6 6.581000-4 2.600000+6 1.183000-3 128 3 3 4 3.000000+6 1.828000-3 3.500000+6 2.280000-3 4.000000+6 2.454000-3 128 3 3 5 4.500000+6 2.474000-3 5.000000+6 2.416000-3 5.500000+6 2.318000-3 128 3 3 6 6.000000+6 2.205000-3 8.000000+6 1.753000-3 1.000000+7 1.373000-3 128 3 3 7 1.500000+7 8.528000-4 2.000000+7 5.882000-4 2.500000+7 4.350000-4 128 3 3 8 3.000000+7 3.376000-4 3.500000+7 2.714000-4 4.000000+7 2.242000-4 128 3 3 9 4.500000+7 1.893000-4 5.000000+7 1.629000-4 5.500000+7 1.425000-4 128 3 3 10 6.000000+7 1.264000-4 7.000000+7 1.031000-4 8.000000+7 8.744000-5 128 3 3 11 9.000000+7 7.622000-5 1.000000+8 6.764000-5 1.200000+8 5.483000-5 128 3 3 12 1.400000+8 4.558000-5 128 3 3 13 128 3 099999 1.002000+3 1.996800+0 0 0 0 0 128 3 28 1 -2.224000+6-2.224000+6 0 0 1 28 128 3 28 2 28 3 128 3 28 3 2.224000+6 0.000000+0 2.300000+6 6.581000-4 2.600000+6 1.183000-3 128 3 28 4 3.000000+6 1.828000-3 3.500000+6 2.280000-3 4.000000+6 2.454000-3 128 3 28 5 4.500000+6 2.474000-3 5.000000+6 2.416000-3 5.500000+6 2.318000-3 128 3 28 6 6.000000+6 2.205000-3 8.000000+6 1.753000-3 1.000000+7 1.373000-3 128 3 28 7 1.500000+7 8.528000-4 2.000000+7 5.882000-4 2.500000+7 4.350000-4 128 3 28 8 3.000000+7 3.376000-4 3.500000+7 2.714000-4 4.000000+7 2.242000-4 128 3 28 9 4.500000+7 1.893000-4 5.000000+7 1.629000-4 5.500000+7 1.425000-4 128 3 28 10 6.000000+7 1.264000-4 7.000000+7 1.031000-4 8.000000+7 8.744000-5 128 3 28 11 9.000000+7 7.622000-5 1.000000+8 6.764000-5 1.200000+8 5.483000-5 128 3 28 12 1.400000+8 4.558000-5 128 3 28 13 128 3 099999 128 0 0 0 1.002000+3 1.996800+0 0 1 1 0 128 6 28 1 1.000000+0 1.000000+0 0 1 1 2 128 6 28 2 2 3 128 6 28 3 2.224000+6 1.000000+0 1.400000+8 1.000000+0 128 6 28 4 0.000000+0 0.000000+0 1 1 1 28 128 6 28 5 28 3 128 6 28 6 0.000000+0 2.224000+6 1 4 6 1 128 6 28 7 0.000000+0 1.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0 128 6 28 8 0.000000+0 2.300000+6 1 4 6 1 128 6 28 9 3.800000+4 1.000000+0 1.942000-1-4.788000-2-1.668300-2-2.544400-3 128 6 28 10 0.000000+0 2.600000+6 1 4 6 1 128 6 28 11 1.880000+5 1.000000+0-1.626000-1 2.612400-1 5.691400-2 6.831100-3 128 6 28 12 0.000000+0 3.000000+6 1 4 6 1 128 6 28 13 3.880000+5 1.000000+0-1.628000-1 3.336800-1 6.522900-2 6.911100-3 128 6 28 14 0.000000+0 3.500000+6 1 4 6 1 128 6 28 15 6.380000+5 1.000000+0-1.587300-1 3.587600-1 6.565700-2 6.291100-3 128 6 28 16 0.000000+0 4.000000+6 1 4 6 1 128 6 28 17 8.880000+5 1.000000+0-1.546700-1 3.687600-1 6.468600-2 5.726700-3 128 6 28 18 0.000000+0 4.500000+6 1 4 6 1 128 6 28 19 1.138000+6 1.000000+0-1.511300-1 3.740800-1 6.354300-2 5.246700-3 128 6 28 20 0.000000+0 5.000000+6 1 4 6 1 128 6 28 21 1.388000+6 1.000000+0-1.480700-1 3.774400-1 6.242900-2 4.835600-3 128 6 28 22 0.000000+0 5.500000+6 1 4 6 1 128 6 28 23 1.638000+6 1.000000+0-1.453300-1 3.797600-1 6.142900-2 4.471100-3 128 6 28 24 0.000000+0 6.000000+6 1 4 6 1 128 6 28 25 1.888000+6 1.000000+0-1.429300-1 3.815600-1 6.048600-2 4.144400-3 128 6 28 26 0.000000+0 8.000000+6 1 4 6 1 128 6 28 27 2.888000+6 1.000000+0-1.351300-1 3.858800-1 5.737100-2 3.062200-3 128 6 28 28 0.000000+0 1.000000+7 1 4 6 1 128 6 28 29 3.888000+6 1.000000+0-1.218700-1 3.777600-1 5.174300-2 2.946700-3 128 6 28 30 0.000000+0 1.500000+7 1 4 6 1 128 6 28 31 6.388000+6 1.000000+0-1.116000-1 3.686000-1 4.722900-2 2.377800-3 128 6 28 32 0.000000+0 2.000000+7 1 4 6 1 128 6 28 33 8.888000+6 1.000000+0-8.913300-2 3.521600-1 3.740000-2 1.044700-3 128 6 28 34 0.000000+0 2.500000+7 1 4 6 1 128 6 28 35 1.138800+7 1.000000+0-7.173300-2 3.306000-1 2.937100-2 2.286700-4 128 6 28 36 0.000000+0 3.000000+7 1 4 6 1 128 6 28 37 1.388800+7 1.000000+0-7.053300-2 3.115600-1 2.801700-2 4.202200-4 128 6 28 38 0.000000+0 3.500000+7 1 4 6 1 128 6 28 39 1.638800+7 1.000000+0-6.485300-2 2.911200-1 2.437400-2 3.246700-4 128 6 28 40 0.000000+0 4.000000+7 1 4 6 1 128 6 28 41 1.888800+7 1.000000+0-5.068700-2 2.662000-1 1.656900-2 2.144200-3 128 6 28 42 0.000000+0 4.500000+7 1 4 6 1 128 6 28 43 2.138800+7 1.000000+0-3.654000-2 2.392000-1 8.234300-3 3.826700-3 128 6 28 44 0.000000+0 5.000000+7 1 4 6 1 128 6 28 45 2.388800+7 1.000000+0-2.708700-2 2.133200-1-1.521700-3-4.762200-3 128 6 28 46 0.000000+0 5.500000+7 1 4 6 1 128 6 28 47 2.638800+7 1.000000+0-2.324700-2 1.907600-1-2.954300-3-4.893300-3 128 6 28 48 0.000000+0 6.000000+7 1 4 6 1 128 6 28 49 2.888800+7 1.000000+0 2.287300-2-1.710800-1 6.022900-3 4.595600-3 128 6 28 50 0.000000+0 7.000000+7 1 4 6 1 128 6 28 51 3.388800+7 1.000000+0 2.018700-2-1.312800-1 1.366900-2 4.515600-3 128 6 28 52 0.000000+0 8.000000+7 1 4 6 1 128 6 28 53 3.888800+7 1.000000+0 1.564700-2-9.176000-2 2.275100-2 5.186700-3 128 6 28 54 0.000000+0 9.000000+7 1 4 6 1 128 6 28 55 4.388800+7 1.000000+0 1.538700-2-5.876000-2 2.962900-2 5.837800-3 128 6 28 56 0.000000+0 1.000000+8 1 4 6 1 128 6 28 57 4.888800+7 1.000000+0 1.935300-2-3.290000-2 3.411400-2 6.275600-3 128 6 28 58 0.000000+0 1.200000+8 1 4 6 1 128 6 28 59 5.888800+7 1.000000+0 2.840700-2 1.068400-2 4.231400-2 6.940000-3 128 6 28 60 0.000000+0 1.400000+8 1 4 6 1 128 6 28 61 6.888800+7 1.000000+0 3.777300-2 4.272000-2 4.874300-2 7.282200-3 128 6 28 62 128 6 099999 128 0 0 0 0 0 0 0 -1 0 0 0