JENDL-5 (Photonuclear sublibrary) 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 5 128 1451 3 0.000000+0 0.000000+0 0 0 77 4 128 1451 4 1- H - 2 NFD EVAL-AUG95 T.Murata 128 1451 5 DIST-DEC21 128 1451 6 ----JENDL-5 MATERIAL 128 128 1451 7 -----PHOTO-NUCLEAR 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 2020-05 Recompiled with (MF,MT)=(3,50) and (6,50) by N.Iwamoto 128 1451 17 (JAEA) 128 1451 18 2021-12 Taken from IAEA/PD-2019 128 1451 19 128 1451 20 MF=1 General Information 128 1451 21 MT=451 Descriptive data and Dictionary 128 1451 22 Details of the evaluation are given in Ref./1/ 128 1451 23 128 1451 24 MF=3 Photon Cross Sections 128 1451 25 MT=3 Total photo-absorption cross section 128 1451 26 Incident energy below 10 MeV : 128 1451 27 Experimental cross sections/2/ were analyzed with a 128 1451 28 simplified Marshall & Guth model/3/. 128 1451 29 Incident energy above 10 MeV : 128 1451 30 Partovi/4/ gave theoretical cross section which reproduced 128 1451 31 experimental values fairly well. The theoretical results 128 1451 32 were basically fitted with the same model as described 128 1451 33 above. 128 1451 34 128 1451 35 MT=50 (g,n0) cross section 128 1451 36 Same as the data of MT=3. 128 1451 37 128 1451 38 MF=6 Energy-Angular Distribution of secondary particles 128 1451 39 MT=50 Particle production data 128 1451 40 Incident energy below 10 MeV : 128 1451 41 CM system angular distributions were calculated with the 128 1451 42 Marshall & Guth model/3/ plus magnetic dipole term. 128 1451 43 Incident energy above 10 MeV : 128 1451 44 CM system angular distributions given by Partovi/4/ were 128 1451 45 adopted. 128 1451 46 Confirming the agreement with experimental distributions 128 1451 47 /5/, the CM system distributions were transformed to LAB 128 1451 48 system with the relativistic kinematics/6/. Coefficients 128 1451 49 of Legendre polynomial expansion are given (L<=4). 128 1451 50 In IAEA/PD library 2019, coefficients which gave negative 128 1451 51 probabilities were corrected by PREPRO/LEGEND code. 128 1451 52 128 1451 53 References 128 1451 54 1) Murata, T. : JAERI-M 94-019, p.330 (1994). 128 1451 55 2) Allen, L.Jr.: Phys. Rev. 98, 705 (1955), 128 1451 56 Alexandrov, I.A.et al.: Soviet Phys. JETP 6, 472 (1958), 128 1451 57 Whalin, B.A. et al.: Phys. Rev. 101, 377 (1956), 128 1451 58 Barns, J.H. et al.: Phys. Rev. 86, 359 (1952), 128 1451 59 Galey, J.A.: Phys. Rev. 117, 763 (1960), 128 1451 60 Phillips, J.A. et al.: Phys. Rev. 80, 326 (1950), 128 1451 61 Keck, J.C. et al.: Phys. Rev. 101, 360 (1956), 128 1451 62 Halpern, J. et al.: Phys. Rev. 91, 934 (1953), 128 1451 63 Hough, P.V.C.: Phys. Rev. 80, 1069 (1950), 128 1451 64 Bishop, G.R. et al.: Phys. Rev. 80, 211 (1950), 128 1451 65 Snell, A.H. et al.: Phys. Rev. 80, 637 (1950), 128 1451 66 McMurray, W.R. et al.: Proc. Phys. Soc. 68A, 181 (1955), 128 1451 67 Barnes, C.A. et al.: Phys. Rev. 86, 359 (1952), 128 1451 68 Waffler, H. et al.: Helv. Phys. Acta 24, 483 (1951), 128 1451 69 Birenbaum, Y. et al.: Phys. Rev. C32, 1825 (1985), 128 1451 70 Moreh, R. et al.: Phys. Rev. C39, 1247 (1989), 128 1451 71 Debevec, P.T. et al.: Phys. Rev. C45, 904 (1992). 128 1451 72 3) Marshall, J.F. and Guth,E.: Phys. Rev. 78, 738 (1950). 128 1451 73 4) Partovi, F.: Ann. Physics 27, 79 (1964). 128 1451 74 5) Smith, F.D.: Nucl. Phys. 465, 429 (1987), 128 1451 75 Shin, Y.M.: Nucl. Phys. 154, 482 (1970), 128 1451 76 Alexandrov, I.A. et al.: Soviet Phys. JETP 6, 472 (1958), 128 1451 77 Keck, J.C. et al.: Phys. Rev. 101, 360 (1956), 128 1451 78 Whalin, B.A. et al.: Phys. Rev. 101, 377 (1956). 128 1451 79 6) Dedrick, K.G.: Rev. Mod. Phys. 34, 429 (1962). 128 1451 80 128 1451 81 1 451 85 1 128 1451 82 3 3 13 0 128 1451 83 3 50 13 0 128 1451 84 6 50 65 0 128 1451 85 128 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 50 1 -2.224000+6-2.224000+6 0 0 1 28 128 3 50 2 28 3 128 3 50 3 2.224000+6 0.000000+0 2.300000+6 6.581000-4 2.600000+6 1.183000-3 128 3 50 4 3.000000+6 1.828000-3 3.500000+6 2.280000-3 4.000000+6 2.454000-3 128 3 50 5 4.500000+6 2.474000-3 5.000000+6 2.416000-3 5.500000+6 2.318000-3 128 3 50 6 6.000000+6 2.205000-3 8.000000+6 1.753000-3 1.000000+7 1.373000-3 128 3 50 7 1.500000+7 8.528000-4 2.000000+7 5.882000-4 2.500000+7 4.350000-4 128 3 50 8 3.000000+7 3.376000-4 3.500000+7 2.714000-4 4.000000+7 2.242000-4 128 3 50 9 4.500000+7 1.893000-4 5.000000+7 1.629000-4 5.500000+7 1.425000-4 128 3 50 10 6.000000+7 1.264000-4 7.000000+7 1.031000-4 8.000000+7 8.744000-5 128 3 50 11 9.000000+7 7.622000-5 1.000000+8 6.764000-5 1.200000+8 5.483000-5 128 3 50 12 1.400000+8 4.558000-5 128 3 50 13 128 3 099999 128 0 0 0 1.002000+3 1.996800+0 0 2 2 0 128 6 50 1 1.000000+0 1.000000+0 0 2 1 2 128 6 50 2 2 3 128 6 50 3 2.224000+6 1.000000+0 1.400000+8 1.000000+0 128 6 50 4 0.000000+0 0.000000+0 0 0 1 28 128 6 50 5 28 3 128 6 50 6 0.000000+0 2.224000+6 0 0 4 4 128 6 50 7 0.000000+0 0.000000+0 0.000000+0 0.000000+0 128 6 50 8 0.000000+0 2.300000+6 0 0 4 4 128 6 50 9 1.942000-1-4.788000-2-1.668300-2-2.544400-3 128 6 50 10 0.000000+0 2.600000+6 0 0 4 4 128 6 50 11 1.113697-1-1.789313-1-3.898214-2-4.678830-3 128 6 50 12 0.000000+0 3.000000+6 0 0 4 4 128 6 50 13 9.218945-2-1.889544-1-3.693750-2-3.913578-3 128 6 50 14 0.000000+0 3.500000+6 0 0 4 4 128 6 50 15 8.484821-2-1.917731-1-3.509657-2-3.362872-3 128 6 50 16 0.000000+0 4.000000+6 0 0 4 4 128 6 50 17 8.096341-2-1.930308-1-3.386047-2-2.997693-3 128 6 50 18 0.000000+0 4.500000+6 0 0 4 4 128 6 50 19 7.830288-2-1.938169-1-3.292265-2-2.718400-3 128 6 50 20 0.000000+0 5.000000+6 0 0 4 4 128 6 50 21 7.625356-2-1.943752-1-3.214988-2-2.490253-3 128 6 50 22 0.000000+0 5.500000+6 0 0 4 4 128 6 50 23 7.456932-2-1.948562-1-3.151943-2-2.294137-3 128 6 50 24 0.000000+0 6.000000+6 0 0 4 4 128 6 50 25 7.313255-2-1.952316-1-3.094869-2-2.120552-3 128 6 50 26 0.000000+0 8.000000+6 0 0 4 4 128 6 50 27 6.877957-2-1.964084-1-2.920116-2-1.558624-3 128 6 50 28 0.000000+0 1.000000+7 0 0 4 4 128 6 50 29 6.338896-2-1.964865-1-2.691339-2-1.532684-3 128 6 50 30 0.000000+0 1.500000+7 0 0 4 4 128 6 50 31 5.960450-2-1.968658-1-2.522456-2-1.269960-3 128 6 50 32 0.000000+0 2.000000+7 0 0 4 4 128 6 50 33 5.009273-2-1.979139-1-2.101879-2-5.871210-4 128 6 50 34 0.000000+0 2.500000+7 0 0 4 4 128 6 50 35 4.300550-2-1.982019-1-1.760856-2-1.370930-4 128 6 50 36 0.000000+0 3.000000+7 0 0 4 4 128 6 50 37 4.463486-2-1.971621-1-1.772978-2-2.659250-4 128 6 50 38 0.000000+0 3.500000+7 0 0 4 4 128 6 50 39 4.383209-2-1.967588-1-1.647361-2 2.194340-4 128 6 50 40 0.000000+0 4.000000+7 0 0 4 4 128 6 50 41 3.753255-2-1.971149-1-1.226896-2 1.587730-3 128 6 50 42 0.000000+0 4.500000+7 0 0 4 4 128 6 50 43 3.005005-2-1.967151-1-6.771787-3 3.147031-3 128 6 50 44 0.000000+0 5.000000+7 0 0 4 4 128 6 50 45 2.470219-2-1.945388-1-1.387726-3 4.342924-3 128 6 50 46 0.000000+0 5.500000+7 0 0 4 4 128 6 50 47 2.319630-2-1.903440-1 2.947857-3 4.882628-3 128 6 50 48 0.000000+0 6.000000+7 0 0 4 4 128 6 50 49 2.287300-2-1.710800-1 6.022900-3 4.595600-3 128 6 50 50 0.000000+0 7.000000+7 0 0 4 4 128 6 50 51 2.018700-2-1.312800-1 1.366900-2 4.515600-3 128 6 50 52 0.000000+0 8.000000+7 0 0 4 4 128 6 50 53 1.564700-2-9.176000-2 2.275100-2 5.186700-3 128 6 50 54 0.000000+0 9.000000+7 0 0 4 4 128 6 50 55 1.538700-2-5.876000-2 2.962900-2 5.837800-3 128 6 50 56 0.000000+0 1.000000+8 0 0 4 4 128 6 50 57 1.935300-2-3.290000-2 3.411400-2 6.275600-3 128 6 50 58 0.000000+0 1.200000+8 0 0 4 4 128 6 50 59 2.840700-2 1.068400-2 4.231400-2 6.940000-3 128 6 50 60 0.000000+0 1.400000+8 0 0 4 4 128 6 50 61 3.777300-2 4.272000-2 4.874300-2 7.282200-3 128 6 50 62 1.001000+3 9.986200-1 0 4 1 2 128 6 50 63 2 3 128 6 50 64 2.224000+6 1.000000+0 1.400000+8 1.000000+0 128 6 50 65 128 6 099999 128 0 0 0 0 0 0 0 -1 0 0 0