ENTRY M0355 20180218 M095M035500000001 SUBENT M0355001 20180218 M095M035500100001 BIB 13 48 M035500100002 TITLE Fast-photoneutron spectra due to 55-85-MeV photons. M035500100003 AUTHOR (N.N.Kaushal,E.J.Winhold,P.F.Yergin,H.A.Medicus, M035500100004 R.H.Augustson) M035500100005 INSTITUTE (1USARPI) M035500100006 REFERENCE (J,PR,175,(4),1330,1968) M035500100007 FACILITY (LINAC,1USARPI) M035500100008 INC-SOURCE (BRST). A 0.010-in.-thick tantalum foil was used. M035500100009 SAMPLE Solid samples were circular disks of 3/4 in. or 1 in. M035500100010 diam. oriented so that the disk axis coincided with M035500100011 the photon beam axis. Disk thicknesses were 1/8 in. M035500100012 or 3/16 in. for heavier nuclei (z>20) and between 1 M035500100013 and 2 2 in. for lighter elements. Water and liquid M035500100014 nitrogen in thin-walled aluminium containers were M035500100015 used as the samples for the studies of oxygen and M035500100016 nitrogen. M035500100017 METHOD (TOF) Flight path = 100 m, time resolution = 0.4 M035500100018 ns/m. M035500100019 DETECTOR (STANK).Liquid scintillator tank of 5 in. in M035500100020 thickness and 20 in. in diameter viewed by seven M035500100021 Philips 58 AVP photomultipliers was used. M035500100022 CORRECTION Energy spectra were corrected for: M035500100023 (a) the photon attenuation in the samples, M035500100024 (b) the scattering of the outgoing neutrons in the M035500100025 samples, M035500100026 (c) the detector efficiency. M035500100027 ADD-RES (COMP) The quasideuteron model was used. M035500100028 COMMENT Energy spectra of fast photoneutrons from eighteen M035500100029 elements were measured. Measurements of the spectra M035500100030 from each target at bremsstrahlung energies of both M035500100031 55 and 85 MeV permitted extraction of neutron M035500100032 difference spectra effectively due to photons M035500100033 between 55 and 85 MeV. M035500100034 Difference spectra were obtained for neutron energies M035500100035 greater than 10 MeV. The experimental data were M035500100036 compared to the predictions of the quasideuteron M035500100037 model with secondary-neutron effects estimated by M035500100038 Monte Carlo calculations. Good agreement was M035500100039 obtained for the absolute-neutron-production cross M035500100040 sections and the shapes of the neutron energy M035500100041 spectra over the range of targets studied. M035500100042 HISTORY (19900205C) Compiled in the SCJAD of Saratov State M035500100043 University. M035500100044 (19930125A) SUBENTs 26,27 rearranged to SUBENTs M035500100045 26 - 59. M035500100046 (20180218A) Corrected by SD and VV: new date formats, M035500100047 lower case, PART-DET deleted, NOSUBENT for 002 - 007 M035500100048 and 043 - 059 (not relevant to EXFOR), REACTION M035500100049 free text, ANALYSIS. M035500100050 ENDBIB 48 0 M035500100051 COMMON 1 3 M035500100052 ANG M035500100053 ADEG M035500100054 67.5 M035500100055 ENDCOMMON 3 0 M035500100056 ENDSUBENT 55 0 M035500199999 NOSUBENT M0355002 20180218 M095M035500200001 NOSUBENT M0355003 20180218 M095M035500300001 NOSUBENT M0355004 20180218 M095M035500400001 NOSUBENT M0355005 20180218 M095M035500500001 NOSUBENT M0355006 20180218 M095M035500600001 NOSUBENT M0355007 20180218 M095M035500700001 SUBENT M0355008 20180218 M095M035500800001 BIB 6 20 M035500800002 REACTION (3-LI-0(G,X)0-NN-1,,DA/DE,,BRA/FCT) M035500800003 The data were obtained by dividing the effective M035500800004 double differential cross section by the sum M035500800005 rule factor N*Z/A. M035500800006 MONITOR (1-H-2(G,N)1-H-1,,DA,N) M035500800007 ANALYSIS The neutron spectra obtained at bremsstrahlung M035500800008 endpoint energies of 55 and 85 MeV were normalized M035500800009 for equal numbers of photons at the giant-resonance M035500800010 peak energy. The neutron difference spectrum was M035500800011 calculated by means of subtraction of 55-MeV neutron M035500800012 spectrum from 85 MeV neutron spectrum. The photon M035500800013 difference spectrum was calculated as the difference M035500800014 between 85- and 55-MeV bremsstrahlung spectra. The M035500800015 effective double differential cross section was M035500800016 obtained by dividing the neutron difference spectrum M035500800017 by the photon difference spectrum. M035500800018 ERR-ANALYS (ERR-S) Statistical errors of measurement. M035500800019 STATUS (CURVE) Data from Fig. 6. M035500800020 HISTORY (20180218A) Corrected by SD and VV: REACTION, M035500800021 ANALYSIS, STATUS, EN-MIN, ERR-S. M035500800022 ENDBIB 20 0 M035500800023 COMMON 2 3 M035500800024 EN-MIN EN-MAX M035500800025 MEV MEV M035500800026 55. 85. M035500800027 ENDCOMMON 3 0 M035500800028 DATA 3 13 M035500800029 E DATA ERR-S M035500800030 MEV MUB/SR/MEV MUB/SR/MEV M035500800031 12. 1.59 0.18 M035500800032 16. 1.30 0.13 M035500800033 19. 1.37 0.09 M035500800034 21. 1.15 0.13 M035500800035 24. 1.41 0.11 M035500800036 25. 1.22 0.08 M035500800037 28. 1.17 0.07 M035500800038 32. 1.02 M035500800039 33. 1.00 M035500800040 37. 0.70 M035500800041 41. 0.39 M035500800042 48. 0.24 M035500800043 53. 0.07 M035500800044 ENDDATA 15 0 M035500800045 ENDSUBENT 44 0 M035500899999 SUBENT M0355009 20180218 M095M035500900001 BIB 6 20 M035500900002 REACTION (4-BE-9(G,X)0-NN-1,,DA/DE,,BRA/FCT) M035500900003 The data were obtained by dividing the effective M035500900004 double differential cross section by the sum M035500900005 rule factor N*Z/A. M035500900006 MONITOR (1-H-2(G,N)1-H-1,,DA,N) M035500900007 ANALYSIS The neutron spectra obtained at bremsstrahlung M035500900008 endpoint energies of 55 and 85 MeV were normalized M035500900009 for equal numbers of photons at the giant-resonance M035500900010 peak energy. The neutron difference spectrum was M035500900011 calculated by means of subtraction of 55-MeV neutron M035500900012 spectrum from 85 MeV neutron spectrum. The photon M035500900013 difference spectrum was calculated as the difference M035500900014 between 85- and 55-MeV bremsstrahlung spectra. The M035500900015 effective double differential cross section was M035500900016 obtained by dividing the neutron difference spectrum M035500900017 by the photon difference spectrum. M035500900018 ERR-ANALYS (ERR-S) Statistical errors of measurement. M035500900019 STATUS (CURVE) Data from Fig. 6. M035500900020 HISTORY (20180218A) Corrected by SD and VV: REACTION, M035500900021 ANALYSIS, STATUS, EN-MIN, ERR-S. M035500900022 ENDBIB 20 0 M035500900023 COMMON 2 3 M035500900024 EN-MIN EN-MAX M035500900025 MEV MEV M035500900026 55. 85. M035500900027 ENDCOMMON 3 0 M035500900028 DATA 3 14 M035500900029 E DATA ERR-S M035500900030 MEV MUB/SR/MEV MUB/SR/MEV M035500900031 12. 1.20 0.17 M035500900032 16. 1.30 0.15 M035500900033 19. 1.22 0.15 M035500900034 21. 1.15 0.15 M035500900035 23. 1.26 0.17 M035500900036 25. 1.09 0.13 M035500900037 27. 1.04 0.13 M035500900038 31. 0.91 0.07 M035500900039 33. 0.93 0.07 M035500900040 37. 1.07 M035500900041 41. 0.48 M035500900042 47. 0.28 M035500900043 53. 0.11 M035500900044 61. 0.04 M035500900045 ENDDATA 16 0 M035500900046 ENDSUBENT 45 0 M035500999999 SUBENT M0355010 20180218 M095M035501000001 BIB 6 21 M035501000002 REACTION (5-B-0(G,X)0-NN-1,,DA/DE,,BRA/FCT) M035501000003 The data were obtained by dividing the effective M035501000004 double differential cross section by the sum M035501000005 rule factor N*Z/A. M035501000006 MONITOR (1-H-2(G,N)1-H-1,,DA,N) M035501000007 ANALYSIS The neutron spectra obtained at bremsstrahlung M035501000008 endpoint energies of 55 and 85 MeV were normalized M035501000009 for equal numbers of photons at the giant-resonance M035501000010 peak energy. The neutron difference spectrum was M035501000011 calculated by means of subtraction of 55-MeV neutron M035501000012 spectrum from 85 MeV neutron spectrum. The photon M035501000013 difference spectrum was calculated as the difference M035501000014 between 85- and 55-MeV bremsstrahlung spectra. The M035501000015 effective double differential cross section was M035501000016 obtained by dividing the neutron difference spectrum M035501000017 by the photon difference spectrum. M035501000018 ERR-ANALYS (ERR-S) statistical errors of measurement. M035501000019 STATUS (CURVE) Data from Fig. 6. M035501000020 HISTORY (20180218A) Corrected by SD and VV: REACTION, M035501000021 ANALYSIS, STATUS, EN-MIN, ERR-S. DATA substituted M035501000022 (39 MeV, 0.58). M035501000023 ENDBIB 21 0 M035501000024 COMMON 2 3 M035501000025 EN-MIN EN-MAX M035501000026 MEV MEV M035501000027 55. 85. M035501000028 ENDCOMMON 3 0 M035501000029 DATA 3 11 M035501000030 E DATA ERR-S M035501000031 MEV MUB/SR/MEV MUB/SR/MEV M035501000032 12. 0.59 0.22 M035501000033 16. 1.04 0.20 M035501000034 20. 0.91 0.13 M035501000035 24. 0.76 0.09 M035501000036 30. 1.15 0.07 M035501000037 36. 0.83 0.07 M035501000038 39. 0.58 M035501000039 43. 0.39 M035501000040 49. 0.20 M035501000041 55. 0.04 M035501000042 60. 0.04 M035501000043 ENDDATA 13 0 M035501000044 ENDSUBENT 43 0 M035501099999 SUBENT M0355011 20180218 M095M035501100001 BIB 6 20 M035501100002 REACTION (6-C-0(G,X)0-NN-1,,DA/DE,,BRA/FCT) M035501100003 The data were obtained by dividing the effective M035501100004 double differential cross section by the sum M035501100005 rule factor N*Z/A. M035501100006 MONITOR (1-H-2(G,N)1-H-1,,DA,N) M035501100007 ANALYSIS The neutron spectra obtained at bremsstrahlung M035501100008 endpoint energies of 55 and 85 MeV were normalized M035501100009 for equal numbers of photons at the giant-resonance M035501100010 peak energy. The neutron difference spectrum was M035501100011 calculated by means of subtraction of 55-MeV neutron M035501100012 spectrum from 85 MeV neutron spectrum. The photon M035501100013 difference spectrum was calculated as the difference M035501100014 between 85- and 55-MeV bremsstrahlung spectra. The M035501100015 effective double differential cross section was M035501100016 obtained by dividing the neutron difference spectrum M035501100017 by the photon difference spectrum. M035501100018 ERR-ANALYS (ERR-S) statistical errors of measurement. M035501100019 STATUS (CURVE) Data from Fig. 6. M035501100020 HISTORY (20180218A) Corrected by SD and VV: REACTION, M035501100021 ANALYSIS, STATUS, EN-MIN, ERR-S. M035501100022 ENDBIB 20 0 M035501100023 COMMON 2 3 M035501100024 EN-MIN EN-MAX M035501100025 MEV MEV M035501100026 55. 85. M035501100027 ENDCOMMON 3 0 M035501100028 DATA 3 12 M035501100029 E DATA ERR-S M035501100030 MEV MUB/SR/MEV MUB/SR/MEV M035501100031 12. 1.13 0.13 M035501100032 16. 1.26 0.13 M035501100033 20. 1.20 0.09 M035501100034 24. 1.28 0.10 M035501100035 27. 1.26 0.09 M035501100036 32. 1.30 M035501100037 33. 1.15 M035501100038 37. 0.83 M035501100039 42. 0.61 M035501100040 47. 0.24 M035501100041 53. 0.09 M035501100042 61. 0.07 M035501100043 ENDDATA 14 0 M035501100044 ENDSUBENT 43 0 M035501199999 SUBENT M0355012 20180218 M095M035501200001 BIB 6 20 M035501200002 REACTION (7-N-0(G,X)0-NN-1,,DA/DE,,BRA/FCT) M035501200003 The data were obtained by dividing the effective M035501200004 double differential cross section by the sum M035501200005 rule factor N*Z/A. M035501200006 MONITOR (1-H-2(G,N)1-H-1,,DA,N) M035501200007 ANALYSIS The neutron spectra obtained at bremsstrahlung M035501200008 endpoint energies of 55 and 85 MeV were normalized M035501200009 for equal numbers of photons at the giant-resonance M035501200010 peak energy. The neutron difference spectrum was M035501200011 calculated by means of subtraction of 55-MeV neutron M035501200012 spectrum from 85 MeV neutron spectrum. The photon M035501200013 difference spectrum was calculated as the difference M035501200014 between 85- and 55-MeV bremsstrahlung spectra. The M035501200015 effective double differential cross section was M035501200016 obtained by dividing the neutron difference spectrum M035501200017 by the photon difference spectrum. M035501200018 ERR-ANALYS (ERR-S) Statistical errors of measurement. M035501200019 STATUS (CURVE) Data from Fig. 6. M035501200020 HISTORY (20180218A) Corrected by SD and VV: REACTION, M035501200021 ANALYSIS, STATUS, EN-MIN, ERR-S. M035501200022 ENDBIB 20 0 M035501200023 COMMON 2 3 M035501200024 EN-MIN EN-MAX M035501200025 MEV MEV M035501200026 55. 85. M035501200027 ENDCOMMON 3 0 M035501200028 DATA 3 8 M035501200029 E DATA ERR-S M035501200030 MEV MUB/SR/MEV MUB/SR/MEV M035501200031 27. 1.04 0.11 M035501200032 32. 1.07 0.09 M035501200033 33. 0.85 0.09 M035501200034 37. 0.83 0.07 M035501200035 41. 0.50 M035501200036 47. 0.26 M035501200037 53. 0.04 M035501200038 61. 0.00 M035501200039 ENDDATA 10 0 M035501200040 ENDSUBENT 39 0 M035501299999 SUBENT M0355013 20180218 M095M035501300001 BIB 6 20 M035501300002 REACTION (8-O-0(G,X)0-NN-1,,DA/DE,,BRA/FCT) M035501300003 The data were obtained by dividing the effective M035501300004 double differential cross section by the sum M035501300005 rule factor N*Z/A. M035501300006 MONITOR (1-H-2(G,N)1-H-1,,DA,N) M035501300007 ANALYSIS The neutron spectra obtained at bremsstrahlung M035501300008 endpoint energies of 55 and 85 MeV were normalized M035501300009 for equal numbers of photons at the giant-resonance M035501300010 peak energy. The neutron difference spectrum was M035501300011 calculated by means of subtraction of 55-MeV neutron M035501300012 spectrum from 85 MeV neutron spectrum. The photon M035501300013 difference spectrum was calculated as the difference M035501300014 between 85- and 55-MeV bremsstrahlung spectra. The M035501300015 effective double differential cross section was M035501300016 obtained by dividing the neutron difference spectrum M035501300017 by the photon difference spectrum. M035501300018 ERR-ANALYS (ERR-S) Statistical errors of measurement. M035501300019 STATUS (CURVE) Data from Fig. 6. M035501300020 HISTORY (20180218A) Corrected by SD and VV: REACTION, M035501300021 ANALYSIS, STATUS, EN-MIN, ERR-S. M035501300022 ENDBIB 20 0 M035501300023 COMMON 2 3 M035501300024 EN-MIN EN-MAX M035501300025 MEV MEV M035501300026 55. 85. M035501300027 ENDCOMMON 3 0 M035501300028 DATA 3 14 M035501300029 E DATA ERR-S M035501300030 MEV MUB/SR/MEV MUB/SR/MEV M035501300031 13. 0.26 0.17 M035501300032 18. 0.70 0.15 M035501300033 23. 0.72 0.13 M035501300034 25. 0.93 0.11 M035501300035 29. 1.00 0.07 M035501300036 32. 1.09 0.07 M035501300037 36. 1.02 M035501300038 37. 0.78 M035501300039 39. 0.61 M035501300040 43. 0.43 M035501300041 45. 0.22 M035501300042 50. 0.07 M035501300043 56. 0.04 M035501300044 60. 0.04 M035501300045 ENDDATA 16 0 M035501300046 ENDSUBENT 45 0 M035501399999 SUBENT M0355014 20180218 M095M035501400001 BIB 6 20 M035501400002 REACTION (13-AL-27(G,X)0-NN-1,,DA/DE,,BRA/FCT) M035501400003 The data were obtained by dividing the effective M035501400004 double differential cross section by the sum M035501400005 rule factor N*Z/A. M035501400006 MONITOR (1-H-2(G,N)1-H-1,,DA,N) M035501400007 ANALYSIS The neutron spectra obtained at bremsstrahlung M035501400008 endpoint energies of 55 and 85 MeV were normalized M035501400009 for equal numbers of photons at the giant-resonance M035501400010 peak energy. The neutron difference spectrum was M035501400011 calculated by means of subtraction of 55-MeV neutron M035501400012 spectrum from 85 MeV neutron spectrum. The photon M035501400013 difference spectrum was calculated as the difference M035501400014 between 85- and 55-MeV bremsstrahlung spectra. The M035501400015 effective double differential cross section was M035501400016 obtained by dividing the neutron difference spectrum M035501400017 by the photon difference spectrum. M035501400018 ERR-ANALYS (ERR-S) Statistical errors of measurement. M035501400019 STATUS (CURVE) Data from Fig. 6. M035501400020 HISTORY (20180218A) Corrected by SD and VV: REACTION, M035501400021 ANALYSIS, STATUS, EN-MIN, ERR-S. M035501400022 ENDBIB 20 0 M035501400023 COMMON 2 3 M035501400024 EN-MIN EN-MAX M035501400025 MEV MEV M035501400026 55. 85. M035501400027 ENDCOMMON 3 0 M035501400028 DATA 3 13 M035501400029 E DATA ERR-S M035501400030 MEV MUB/SR/MEV MUB/SR/MEV M035501400031 12. 1.61 0.15 M035501400032 16. 1.13 0.15 M035501400033 19. 0.96 0.17 M035501400034 21. 1.13 0.11 M035501400035 23. 1.13 0.11 M035501400036 25. 1.13 0.09 M035501400037 29. 0.78 0.07 M035501400038 31. 0.78 0.07 M035501400039 35. 0.63 M035501400040 39. 0.43 M035501400041 44. 0.26 M035501400042 49. 0.13 M035501400043 55. 0.07 M035501400044 ENDDATA 15 0 M035501400045 ENDSUBENT 44 0 M035501499999 SUBENT M0355015 20180218 M095M035501500001 BIB 6 20 M035501500002 REACTION (16-S-0(G,X)0-NN-1,,DA/DE,,BRA/FCT) M035501500003 The data were obtained by dividing the effective M035501500004 double differential cross section by the sum M035501500005 rule factor N*Z/A. M035501500006 MONITOR (1-H-2(G,N)1-H-1,,DA,N) M035501500007 ANALYSIS The neutron spectra obtained at bremsstrahlung M035501500008 endpoint energies of 55 and 85 MeV were normalized M035501500009 for equal numbers of photons at the giant-resonance M035501500010 peak energy. The neutron difference spectrum was M035501500011 calculated by means of subtraction of 55-MeV neutron M035501500012 spectrum from 85 MeV neutron spectrum. The photon M035501500013 difference spectrum was calculated as the difference M035501500014 between 85- and 55-MeV bremsstrahlung spectra. The M035501500015 effective double differential cross section was M035501500016 obtained by dividing the neutron difference spectrum M035501500017 by the photon difference spectrum. M035501500018 ERR-ANALYS (ERR-S) Statistical errors of measurement. M035501500019 STATUS (CURVE) Data from Fig. 6. M035501500020 HISTORY (20180218A) Corrected by SD and VV: REACTION, M035501500021 ANALYSIS, STATUS, EN-MIN, ERR-S. M035501500022 ENDBIB 20 0 M035501500023 COMMON 2 3 M035501500024 EN-MIN EN-MAX M035501500025 MEV MEV M035501500026 55. 85. M035501500027 ENDCOMMON 3 0 M035501500028 DATA 3 12 M035501500029 E DATA ERR-S M035501500030 MEV MUB/SR/MEV MUB/SR/MEV M035501500031 12. 1.04 0.17 M035501500032 16. 0.52 0.15 M035501500033 19. 0.57 0.15 M035501500034 23. 0.63 0.15 M035501500035 25. 0.70 0.13 M035501500036 27. 0.70 0.11 M035501500037 31. 0.61 0.09 M035501500038 33. 0.52 0.07 M035501500039 38. 0.39 M035501500040 41. 0.30 M035501500041 47. 0.17 M035501500042 65. 0.04 M035501500043 ENDDATA 14 0 M035501500044 ENDSUBENT 43 0 M035501599999 SUBENT M0355016 20180218 M095M035501600001 BIB 6 20 M035501600002 REACTION (26-FE-0(G,X)0-NN-1,,DA/DE,,BRA/FCT) M035501600003 The data were obtained by dividing the effective M035501600004 double differential cross section by the sum M035501600005 rule factor N*Z/A. M035501600006 MONITOR (1-H-2(G,N)1-H-1,,DA,N) M035501600007 ANALYSIS The neutron spectra obtained at bremsstrahlung M035501600008 endpoint energies of 55 and 85 MeV were normalized M035501600009 for equal numbers of photons at the giant-resonance M035501600010 peak energy. The neutron difference spectrum was M035501600011 calculated by means of subtraction of 55-MeV neutron M035501600012 spectrum from 85 MeV neutron spectrum. The photon M035501600013 difference spectrum was calculated as the difference M035501600014 between 85- and 55-MeV bremsstrahlung spectra. The M035501600015 effective double differential cross section was M035501600016 obtained by dividing the neutron difference spectrum M035501600017 by the photon difference spectrum. M035501600018 ERR-ANALYS (ERR-S) Statistical errors of measurement. M035501600019 STATUS (CURVE) Data from Fig. 6. M035501600020 HISTORY (20180218A) Corrected by SD and VV: REACTION, M035501600021 ANALYSIS, STATUS, EN-MIN, ERR-S. M035501600022 ENDBIB 20 0 M035501600023 COMMON 1 3 M035501600024 EN-MAX M035501600025 MEV M035501600026 85. M035501600027 ENDCOMMON 3 0 M035501600028 DATA 3 10 M035501600029 E DATA ERR-S M035501600030 MEV MUB/SR/MEV MUB/SR/MEV M035501600031 16. 0.57 0.26 M035501600032 19. 1.00 0.20 M035501600033 24. 0.61 0.15 M035501600034 29. 0.67 0.15 M035501600035 31. 0.67 0.13 M035501600036 35. 0.48 0.13 M035501600037 39. 0.24 0.07 M035501600038 43. 0.04 M035501600039 49. 0.02 M035501600040 55. 0.00 M035501600041 ENDDATA 12 0 M035501600042 ENDSUBENT 41 0 M035501699999 SUBENT M0355017 20180218 M095M035501700001 BIB 6 21 M035501700002 REACTION (29-CU-0(G,X)0-NN-1,,DA/DE,,BRA/FCT) M035501700003 The data were obtained by dividing the effective M035501700004 double differential cross section by the sum M035501700005 rule factor N*Z/A. M035501700006 The effective double differential cross section. M035501700007 MONITOR (1-H-2(G,N)1-H-1,,DA,N) M035501700008 ANALYSIS The neutron spectra obtained at bremsstrahlung M035501700009 endpoint energies of 55 and 85 MeV were normalized M035501700010 for equal numbers of photons at the giant-resonance M035501700011 peak energy. The neutron difference spectrum was M035501700012 calculated by means of subtraction of 55-MeV neutron M035501700013 spectrum from 85 MeV neutron spectrum. The photon M035501700014 difference spectrum was calculated as the difference M035501700015 between 85- and 55-MeV bremsstrahlung spectra. The M035501700016 effective double differential cross section was M035501700017 obtained by dividing the neutron difference spectrum M035501700018 by the photon difference spectrum. M035501700019 ERR-ANALYS (ERR-S) Statistical errors of measurement. M035501700020 STATUS (CURVE) Data from Fig. 6. M035501700021 HISTORY (20180218A) Corrected by SD and VV: REACTION, M035501700022 ANALYSIS, STATUS, EN-MIN, ERR-S. M035501700023 ENDBIB 21 0 M035501700024 COMMON 2 3 M035501700025 EN-MIN EN-MAX M035501700026 MEV MEV M035501700027 55. 85. M035501700028 ENDCOMMON 3 0 M035501700029 DATA 3 13 M035501700030 E DATA ERR-S M035501700031 MEV MUB/SR/MEV MUB/SR/MEV M035501700032 12. 1.20 0.20 M035501700033 16. 1.02 0.17 M035501700034 20. 0.83 0.11 M035501700035 23. 0.67 0.13 M035501700036 25. 0.41 0.13 M035501700037 27. 0.48 0.09 M035501700038 31. 0.30 0.09 M035501700039 33. 0.43 0.09 M035501700040 38. 0.26 0.07 M035501700041 42. 0.24 0.07 M035501700042 48. 0.09 M035501700043 53. 0.04 M035501700044 61. 0.04 M035501700045 ENDDATA 15 0 M035501700046 ENDSUBENT 45 0 M035501799999 SUBENT M0355018 20180218 M095M035501800001 BIB 6 20 M035501800002 REACTION (30-ZN-0(G,X)0-NN-1,,DA/DE,,BRA/FCT) M035501800003 The data were obtained by dividing the effective M035501800004 double differential cross section by the sum M035501800005 rule factor N*Z/A. M035501800006 MONITOR (1-H-2(G,N)1-H-1,,DA,N) M035501800007 ANALYSIS The neutron spectra obtained at bremsstrahlung M035501800008 endpoint energies of 55 and 85 MeV were normalized M035501800009 for equal numbers of photons at the giant-resonance M035501800010 peak energy. The neutron difference spectrum was M035501800011 calculated by means of subtraction of 55-MeV neutron M035501800012 spectrum from 85 MeV neutron spectrum. The photon M035501800013 difference spectrum was calculated as the difference M035501800014 between 85- and 55-MeV bremsstrahlung spectra. The M035501800015 effective double differential cross section was M035501800016 obtained by dividing the neutron difference spectrum M035501800017 by the photon difference spectrum. M035501800018 ERR-ANALYS (ERR-S) Statistical errors of measurement. M035501800019 STATUS (CURVE) Data from Fig. 6. M035501800020 HISTORY (20180218A) Corrected by SD and VV: REACTION, M035501800021 ANALYSIS, STATUS, EN-MIN, ERR-S. M035501800022 ENDBIB 20 0 M035501800023 COMMON 2 3 M035501800024 EN-MIN EN-MAX M035501800025 MEV MEV M035501800026 55. 85. M035501800027 ENDCOMMON 3 0 M035501800028 DATA 3 10 M035501800029 E DATA ERR-S M035501800030 MEV MUB/SR/MEV MUB/SR/MEV M035501800031 12. 1.15 0.24 M035501800032 16. 1.02 0.20 M035501800033 20. 0.87 0.13 M035501800034 23. 0.83 0.17 M035501800035 25. 0.74 0.13 M035501800036 27. 0.52 0.15 M035501800037 31. 0.52 0.15 M035501800038 33. 0.26 0.09 M035501800039 41. 0.17 M035501800040 47. 0.04 M035501800041 ENDDATA 12 0 M035501800042 ENDSUBENT 41 0 M035501899999 SUBENT M0355019 20180218 M095M035501900001 BIB 6 20 M035501900002 REACTION (49-IN-0(G,X)0-NN-1,,DA/DE,,BRA/FCT) M035501900003 The data were obtained by dividing the effective M035501900004 double differential cross section by the sum M035501900005 rule factor N*Z/A. M035501900006 MONITOR (1-H-2(G,N)1-H-1,,DA,N) M035501900007 ANALYSIS The neutron spectra obtained at bremsstrahlung M035501900008 endpoint energies of 55 and 85 MeV were normalized M035501900009 for equal numbers of photons at the giant-resonance M035501900010 peak energy. The neutron difference spectrum was M035501900011 calculated by means of subtraction of 55-MeV neutron M035501900012 spectrum from 85 MeV neutron spectrum. The photon M035501900013 difference spectrum was calculated as the difference M035501900014 between 85- and 55-MeV bremsstrahlung spectra. The M035501900015 effective double differential cross section was M035501900016 obtained by dividing the neutron difference spectrum M035501900017 by the photon difference spectrum. M035501900018 ERR-ANALYS (ERR-S) Statistical errors of measurement. M035501900019 STATUS (CURVE) Data from Fig. 6. M035501900020 HISTORY (20180218A) Corrected by SD and VV: REACTION, M035501900021 ANALYSIS, STATUS, EN-MIN, ERR-S. M035501900022 ENDBIB 20 0 M035501900023 COMMON 2 3 M035501900024 EN-MIN EN-MAX M035501900025 MEV MEV M035501900026 55. 85. M035501900027 ENDCOMMON 3 0 M035501900028 DATA 3 12 M035501900029 E DATA ERR-S M035501900030 MEV MUB/SR/MEV MUB/SR/MEV M035501900031 12. 1.20 0.30 M035501900032 16. 0.93 0.26 M035501900033 20. 0.91 0.17 M035501900034 23. 0.52 0.17 M035501900035 25. 0.43 0.17 M035501900036 29. 0.67 0.13 M035501900037 31. 0.48 0.11 M035501900038 35. 0.33 0.09 M035501900039 39. 0.13 0.07 M035501900040 43. 0.07 0.07 M035501900041 49. 0.04 M035501900042 55. 0.04 M035501900043 ENDDATA 14 0 M035501900044 ENDSUBENT 43 0 M035501999999 SUBENT M0355020 20180218 M095M035502000001 BIB 6 20 M035502000002 REACTION (50-SN-0(G,X)0-NN-1,,DA/DE,,BRA/FCT) M035502000003 The data were obtained by dividing the effective M035502000004 double differential cross section by the sum M035502000005 rule factor N*Z/A. M035502000006 MONITOR (1-H-2(G,N)1-H-1,,DA,N) M035502000007 ANALYSIS The neutron spectra obtained at bremsstrahlung M035502000008 endpoint energies of 55 and 85 MeV were normalized M035502000009 for equal numbers of photons at the giant-resonance M035502000010 peak energy. The neutron difference spectrum was M035502000011 calculated by means of subtraction of 55-MeV neutron M035502000012 spectrum from 85 MeV neutron spectrum. The photon M035502000013 difference spectrum was calculated as the difference M035502000014 between 85- and 55-MeV bremsstrahlung spectra. The M035502000015 effective double differential cross section was M035502000016 obtained by dividing the neutron difference spectrum M035502000017 by the photon difference spectrum. M035502000018 ERR-ANALYS (ERR-S) Statistical errors of measurement. M035502000019 STATUS (CURVE) Data from Fig. 6. M035502000020 HISTORY (20180218A) Corrected by SD and VV: REACTION, M035502000021 ANALYSIS, STATUS, EN-MIN, ERR-S. M035502000022 ENDBIB 20 0 M035502000023 COMMON 2 3 M035502000024 EN-MIN EN-MAX M035502000025 MEV MEV M035502000026 55. 85. M035502000027 ENDCOMMON 3 0 M035502000028 DATA 3 12 M035502000029 E DATA ERR-S M035502000030 MEV MUB/SR/MEV MUB/SR/MEV M035502000031 12. 1.11 0.26 M035502000032 16. 0.87 0.15 M035502000033 20. 0.78 0.09 M035502000034 23. 0.59 0.11 M035502000035 25. 0.48 0.09 M035502000036 27. 0.61 0.07 M035502000037 32. 0.39 0.07 M035502000038 34. 0.39 M035502000039 37. 0.30 0.07 M035502000040 41. 0.13 M035502000041 47. 0.04 M035502000042 52. 0.02 M035502000043 ENDDATA 14 0 M035502000044 ENDSUBENT 43 0 M035502099999 SUBENT M0355021 20180218 M095M035502100001 BIB 6 20 M035502100002 REACTION (73-TA-181(G,X)0-NN-1,,DA/DE,,BRA/FCT) M035502100003 The data were obtained by dividing the effective M035502100004 double differential cross section by the sum M035502100005 rule factor N*Z/A. M035502100006 MONITOR (1-H-2(G,N)1-H-1,,DA,N) M035502100007 ANALYSIS The neutron spectra obtained at bremsstrahlung M035502100008 endpoint energies of 55 and 85 MeV were normalized M035502100009 for equal numbers of photons at the giant-resonance M035502100010 peak energy. The neutron difference spectrum was M035502100011 calculated by means of subtraction of 55-MeV neutron M035502100012 spectrum from 85 MeV neutron spectrum. The photon M035502100013 difference spectrum was calculated as the difference M035502100014 between 85- and 55-MeV bremsstrahlung spectra. The M035502100015 effective double differential cross section was M035502100016 obtained by dividing the neutron difference spectrum M035502100017 by the photon difference spectrum. M035502100018 ERR-ANALYS (ERR-S) Statistical errors of measurement. M035502100019 STATUS (CURVE) Data from Fig. 6. M035502100020 HISTORY (20180218A) Corrected by SD and VV: REACTION, M035502100021 ANALYSIS, STATUS, EN-MIN, ERR-S. M035502100022 ENDBIB 20 0 M035502100023 COMMON 2 3 M035502100024 EN-MIN EN-MAX M035502100025 MEV MEV M035502100026 55. 85. M035502100027 ENDCOMMON 3 0 M035502100028 DATA 3 12 M035502100029 E DATA ERR-S M035502100030 MEV MUB/SR/MEV MUB/SR/MEV M035502100031 12. 1.00 0.22 M035502100032 16. 0.96 0.22 M035502100033 20. 0.83 0.13 M035502100034 23. 0.65 0.17 M035502100035 25. 0.57 0.13 M035502100036 29. 0.43 0.13 M035502100037 31. 0.39 0.11 M035502100038 35. 0.24 0.09 M035502100039 39. 0.17 0.09 M035502100040 43. 0.15 0.09 M035502100041 49. 0.09 0.09 M035502100042 55. 0.04 M035502100043 ENDDATA 14 0 M035502100044 ENDSUBENT 43 0 M035502199999 SUBENT M0355022 20180218 M095M035502200001 BIB 6 20 M035502200002 REACTION (81-TL-0(G,X)0-NN-1,,DA/DE,,BRA/FCT) M035502200003 The data were obtained by dividing the effective M035502200004 double differential cross section by the sum M035502200005 rule factor N*Z/A. M035502200006 MONITOR (1-H-2(G,N)1-H-1,,DA,N) M035502200007 ANALYSIS The neutron spectra obtained at bremsstrahlung M035502200008 endpoint energies of 55 and 85 MeV were normalized M035502200009 for equal numbers of photons at the giant-resonance M035502200010 peak energy. The neutron difference spectrum was M035502200011 calculated by means of subtraction of 55-MeV neutron M035502200012 spectrum from 85 MeV neutron spectrum. The photon M035502200013 difference spectrum was calculated as the difference M035502200014 between 85- and 55-MeV bremsstrahlung spectra. The M035502200015 effective double differential cross section was M035502200016 obtained by dividing the neutron difference spectrum M035502200017 by the photon difference spectrum. M035502200018 ERR-ANALYS (ERR-S) Statistical errors of measurement. M035502200019 STATUS (CURVE) Data from Fig. 6. M035502200020 HISTORY (20180218A) Corrected by SD and VV: REACTION, M035502200021 ANALYSIS, STATUS, EN-MIN, ERR-S. M035502200022 ENDBIB 20 0 M035502200023 COMMON 2 3 M035502200024 EN-MIN EN-MAX M035502200025 MEV MEV M035502200026 55. 85. M035502200027 ENDCOMMON 3 0 M035502200028 DATA 3 12 M035502200029 E DATA ERR-S M035502200030 MEV MUB/SR/MEV MUB/SR/MEV M035502200031 12. 1.26 0.22 M035502200032 16. 0.96 0.17 M035502200033 20. 0.41 0.11 M035502200034 24. 0.50 0.09 M035502200035 27. 0.46 0.09 M035502200036 31. 0.22 0.09 M035502200037 34. 0.22 0.09 M035502200038 37. 0.17 0.09 M035502200039 41. 0.11 M035502200040 48. 0.07 M035502200041 54. 0.02 M035502200042 62. 0.00 M035502200043 ENDDATA 14 0 M035502200044 ENDSUBENT 43 0 M035502299999 SUBENT M0355023 20180218 M095M035502300001 BIB 6 31 M035502300002 REACTION (82-PB-0(G,X)0-NN-1,,DA/DE,,BRA/FCT) M035502300003 The data were obtained by dividing the effective M035502300004 double differential cross section by the sum M035502300005 rule factor N*Z/A. M035502300006 The neutron spectra obtained at bremsstrahlung M035502300007 endpoint energies of 55 and 85 MeV were normalized M035502300008 for equal numbers of photons at the giant-resonance M035502300009 peak energy. The neutron difference spectrum was M035502300010 calculated by means of subtraction of 55-MeV neutron M035502300011 spectrum from 85 MeV neutron spectrum. The photon M035502300012 difference spectrum was calculated as the difference M035502300013 between 85- and 55-MeV bremsstrahlung spectra. The M035502300014 effective double differential cross section was M035502300015 obtained by dividing the neutron difference spectrum M035502300016 by the photon difference spectrum. M035502300017 MONITOR (1-H-2(G,N)1-H-1,,DA,N) M035502300018 ANALYSIS The neutron spectra obtained at bremsstrahlung M035502300019 endpoint energies of 55 and 85 MeV were normalized M035502300020 for equal numbers of photons at the giant-resonance M035502300021 peak energy. The neutron difference spectrum was M035502300022 calculated by means of subtraction of 55-MeV neutron M035502300023 spectrum from 85 MeV neutron spectrum. The photon M035502300024 difference spectrum was calculated as the difference M035502300025 between 85- and 55-MeV bremsstrahlung spectra. The M035502300026 effective double differential cross section was M035502300027 obtained by dividing the neutron difference spectrum M035502300028 by the photon difference spectrum. M035502300029 ERR-ANALYS (ERR-S) Statistical errors of measurement. M035502300030 STATUS (CURVE) Data from Fig. 6. M035502300031 HISTORY (20180218A) Corrected by SD and VV: REACTION, M035502300032 ANALYSIS, STATUS, EN-MIN, ERR-S. M035502300033 ENDBIB 31 0 M035502300034 COMMON 2 3 M035502300035 EN-MIN EN-MAX M035502300036 MEV MEV M035502300037 55. 85. M035502300038 ENDCOMMON 3 0 M035502300039 DATA 3 12 M035502300040 E DATA ERR-S M035502300041 MEV MUB/SR/MEV MUB/SR/MEV M035502300042 12. 0.65 0.17 M035502300043 16. 0.67 0.17 M035502300044 20. 0.41 0.13 M035502300045 25. 0.39 0.09 M035502300046 28. 0.24 0.09 M035502300047 31. 0.30 0.09 M035502300048 34. 0.24 0.07 M035502300049 38. 0.13 M035502300050 41. 0.22 M035502300051 48. 0.11 M035502300052 52. 0.04 M035502300053 61. 0.04 M035502300054 ENDDATA 14 0 M035502300055 ENDSUBENT 54 0 M035502399999 SUBENT M0355024 20180218 M095M035502400001 BIB 6 20 M035502400002 REACTION (83-BI-209(G,X)0-NN-1,,DA/DE,,BRA/FCT) M035502400003 The data were obtained by dividing the effective M035502400004 double differential cross section by the sum M035502400005 rule factor N*Z/A. M035502400006 MONITOR (1-H-2(G,N)1-H-1,,DA,N) M035502400007 ANALYSIS The neutron spectra obtained at bremsstrahlung M035502400008 endpoint energies of 55 and 85 MeV were normalized M035502400009 for equal numbers of photons at the giant-resonance M035502400010 peak energy. The neutron difference spectrum was M035502400011 calculated by means of subtraction of 55-MeV neutron M035502400012 spectrum from 85 MeV neutron spectrum. The photon M035502400013 difference spectrum was calculated as the difference M035502400014 between 85- and 55-MeV bremsstrahlung spectra. The M035502400015 effective double differential cross section was M035502400016 obtained by dividing the neutron difference spectrum M035502400017 by the photon difference spectrum. M035502400018 ERR-ANALYS (ERR-S) Statistical errors of measurement. M035502400019 STATUS (CURVE) Data from Fig. 6. M035502400020 HISTORY (20180218A) Corrected by SD and VV: REACTION, M035502400021 ANALYSIS, STATUS, EN-MIN, ERR-S. M035502400022 ENDBIB 20 0 M035502400023 COMMON 2 3 M035502400024 EN-MIN EN-MAX M035502400025 MEV MEV M035502400026 55. 85. M035502400027 ENDCOMMON 3 0 M035502400028 DATA 3 12 M035502400029 E DATA ERR-S M035502400030 MEV MUB/SR/MEV MUB/SR/MEV M035502400031 12. 1.20 0.22 M035502400032 16. 0.70 0.24 M035502400033 20. 0.76 0.17 M035502400034 23. 0.61 0.17 M035502400035 25. 0.37 0.13 M035502400036 29. 0.48 0.13 M035502400037 31. 0.39 0.11 M035502400038 36. 0.30 0.09 M035502400039 39. 0.26 0.09 M035502400040 44. 0.17 0.09 M035502400041 49. 0.22 0.09 M035502400042 55. 0.13 M035502400043 ENDDATA 14 0 M035502400044 ENDSUBENT 43 0 M035502499999 SUBENT M0355025 20180218 M095M035502500001 BIB 6 20 M035502500002 REACTION (92-U-0(G,X)0-NN-1,,DA/DE,,BRA/FCT) M035502500003 The data were obtained by dividing the effective M035502500004 double differential cross section by the sum M035502500005 rule factor N*Z/A. M035502500006 MONITOR (1-H-2(G,N)1-H-1,,DA,N) M035502500007 ANALYSIS The neutron spectra obtained at bremsstrahlung M035502500008 endpoint energies of 55 and 85 MeV were normalized M035502500009 for equal numbers of photons at the giant-resonance M035502500010 peak energy. The neutron difference spectrum was M035502500011 calculated by means of subtraction of 55-MeV neutron M035502500012 spectrum from 85 MeV neutron spectrum. The photon M035502500013 difference spectrum was calculated as the difference M035502500014 between 85- and 55-MeV bremsstrahlung spectra. The M035502500015 effective double differential cross section was M035502500016 obtained by dividing the neutron difference spectrum M035502500017 by the photon difference spectrum. M035502500018 ERR-ANALYS (ERR-S) Statistical errors of measurement. M035502500019 STATUS (CURVE) Data from Fig. 6. M035502500020 HISTORY (20180218A) Corrected by SD and VV: REACTION, M035502500021 ANALYSIS, STATUS, EN-MIN, ERR-S. M035502500022 ENDBIB 20 0 M035502500023 COMMON 2 3 M035502500024 EN-MIN EN-MAX M035502500025 MEV MEV M035502500026 55. 85. M035502500027 ENDCOMMON 3 0 M035502500028 DATA 3 13 M035502500029 E DATA ERR-S M035502500030 MEV MUB/SR/MEV MUB/SR/MEV M035502500031 12. 1.52 0.24 M035502500032 16. 0.80 0.22 M035502500033 20. 0.74 0.15 M035502500034 23. 0.76 0.20 M035502500035 25. 0.59 0.17 M035502500036 27. 0.70 0.13 M035502500037 31. 0.43 0.13 M035502500038 34. 0.35 0.13 M035502500039 37. 0.35 0.11 M035502500040 41. 0.17 0.09 M035502500041 47. 0.13 0.09 M035502500042 53. 0.09 0.07 M035502500043 62. -0.11 M035502500044 ENDDATA 15 0 M035502500045 ENDSUBENT 44 0 M035502599999 SUBENT M0355026 20180218 M095M035502600001 BIB 5 11 M035502600002 REACTION (3-LI-0(G,X)0-NN-1,PAR,DA,,4PI/BRA) M035502600003 ANALYSIS (INTED,4PI1A) M035502600004 ERR-ANALYS (DATA-ERR,8.,10.) Sum of statistical and M035502600005 normalization errors are presented. M035502600006 (ERR-1) in addition all values depend on an absolute M035502600007 normalization in terms of the deuteron M035502600008 photodisintegration cross section, which is known to M035502600009 about 10% at these energies. M035502600010 STATUS (TABLE) Data from Table 1 of PR,175,1330,1968. M035502600011 HISTORY (20180218A) Corrected by S and VV: SF9 = EXP deleted M035502600012 from REACTION code, ERR-1, EN-MIN. M035502600013 ENDBIB 11 0 M035502600014 COMMON 2 3 M035502600015 E-MIN ERR-1 M035502600016 MEV PER-CENT M035502600017 10. 10. M035502600018 ENDCOMMON 3 0 M035502600019 DATA 2 1 M035502600020 EN-MAX DATA M035502600021 MEV MB M035502600022 85. 0.75 M035502600023 ENDDATA 3 0 M035502600024 ENDSUBENT 23 0 M035502699999 SUBENT M0355027 20180218 M095M035502700001 BIB 5 12 M035502700002 REACTION (4-BE-9(G,X)0-NN-1,PAR,DA,,4PI/BRA) M035502700003 ANALYSIS (INTED,4PI1A) M035502700004 ERR-ANALYS (DATA-ERR,8.,10.) M035502700005 Sum of statistical and normalization errors are M035502700006 presented. M035502700007 (ERR-1) In addition all values depend on an absolute M035502700008 normalization in terms of the deuteron M035502700009 photodisintegration cross section, which is known to M035502700010 about 10% at these energies. M035502700011 STATUS (TABLE) Data from Table 1 of PR,175,1330,1968. M035502700012 HISTORY (20180218A) Corrected by S and VV: SF9 = EXP deleted M035502700013 from REACTION code, ERR-1, EN-MIN. M035502700014 ENDBIB 12 0 M035502700015 COMMON 2 3 M035502700016 E-MIN ERR-1 M035502700017 MEV PER-CENT M035502700018 10. 10. M035502700019 ENDCOMMON 3 0 M035502700020 DATA 3 1 M035502700021 EN-MIN EN-MAX DATA M035502700022 MEV MEV MB M035502700023 55. 85. 1.00 M035502700024 ENDDATA 3 0 M035502700025 ENDSUBENT 24 0 M035502799999 SUBENT M0355028 20180218 M095M035502800001 BIB 5 12 M035502800002 REACTION (5-B-0(G,X)0-NN-1,PAR,DA,,4PI/BRA) M035502800003 ANALYSIS (INTED,4PI1A) M035502800004 ERR-ANALYS (DATA-ERR,8.,10.) M035502800005 Sum of statistical and normalization errors are M035502800006 presented. M035502800007 (ERR-1) In addition all values depend on an absolute M035502800008 normalization in terms of the deuteron M035502800009 photodisintegration cross section, which is known to M035502800010 about 10% at these energies. M035502800011 STATUS (TABLE) Data from Table 1 of PR,175,1330,1968. M035502800012 HISTORY (20180218A) Corrected by S and VV: SF9 = EXP deleted M035502800013 from REACTION code, ERR-1, EN-MIN. M035502800014 ENDBIB 12 0 M035502800015 COMMON 2 3 M035502800016 E-MIN ERR-1 M035502800017 MEV PER-CENT M035502800018 10. 10. M035502800019 ENDCOMMON 3 0 M035502800020 DATA 3 1 M035502800021 EN-MIN EN-MAX DATA M035502800022 MEV MEV MB M035502800023 55. 85. 1.00 M035502800024 ENDDATA 3 0 M035502800025 ENDSUBENT 24 0 M035502899999 SUBENT M0355029 20180218 M095M035502900001 BIB 5 12 M035502900002 REACTION (6-C-0(G,X)0-NN-1,PAR,DA,,4PI/BRA) M035502900003 ANALYSIS (INTED,4PI1A) M035502900004 ERR-ANALYS (DATA-ERR,8.,10.) M035502900005 Sum of statistical and normalization errors are M035502900006 presented. M035502900007 (ERR-1) In addition all values depend on an absolute M035502900008 normalization in terms of the deuteron M035502900009 photodisintegration cross section, which is known to M035502900010 about 10% at these energies. M035502900011 STATUS (TABLE) Data from Table 1 of PR,175,1330,1968. M035502900012 HISTORY (20180218A) Corrected by S and VV: SF9 = EXP deleted M035502900013 from REACTION code, ERR-1, EN-MIN. M035502900014 ENDBIB 12 0 M035502900015 COMMON 2 3 M035502900016 E-MIN ERR-1 M035502900017 MEV PER-CENT M035502900018 10. 10. M035502900019 ENDCOMMON 3 0 M035502900020 DATA 3 1 M035502900021 EN-MIN EN-MAX DATA M035502900022 MEV MEV MB M035502900023 55. 85. 1.50 M035502900024 ENDDATA 3 0 M035502900025 ENDSUBENT 24 0 M035502999999 SUBENT M0355030 20180218 M095M035503000001 BIB 5 12 M035503000002 REACTION (8-O-0(G,X)0-NN-1,PAR,DA,,4PI/BRA) M035503000003 ANALYSIS (INTED,4PI1A) M035503000004 ERR-ANALYS (DATA-ERR,8.,10.) M035503000005 Sum of statistical and normalization errors are M035503000006 presented. M035503000007 (ERR-1) In addition all values depend on an absolute M035503000008 normalization in terms of the deuteron M035503000009 photodisintegration cross section, which is known to M035503000010 about 10% at these energies. M035503000011 STATUS (TABLE) Data from Table 1 of PR,175,1330,1968. M035503000012 HISTORY (20180218A) Corrected by S and VV: SF9 = EXP deleted M035503000013 from REACTION code, ERR-1, EN-MIN. M035503000014 ENDBIB 12 0 M035503000015 COMMON 2 3 M035503000016 E-MIN ERR-1 M035503000017 MEV PER-CENT M035503000018 10. 10. M035503000019 ENDCOMMON 3 0 M035503000020 DATA 3 1 M035503000021 EN-MIN EN-MAX DATA M035503000022 MEV MEV MB M035503000023 55. 85. 1.30 M035503000024 ENDDATA 3 0 M035503000025 ENDSUBENT 24 0 M035503099999 SUBENT M0355031 20180218 M095M035503100001 BIB 5 12 M035503100002 REACTION (13-AL-27(G,X)0-NN-1,PAR,DA,,4PI/BRA) M035503100003 ANALYSIS (INTED,4PI1A) M035503100004 ERR-ANALYS (DATA-ERR,8.,10.) M035503100005 Sum of statistical and normalization errors are M035503100006 presented. M035503100007 (ERR-1) In addition all values depend on an absolute M035503100008 normalization in terms of the deuteron M035503100009 photodisintegration cross section, which is known to M035503100010 about 10% at these energies. M035503100011 STATUS (TABLE) Data from Table 1 of PR,175,1330,1968. M035503100012 HISTORY (20180218A) Corrected by S and VV: SF9 = EXP deleted M035503100013 from REACTION code, ERR-1, EN-MIN. M035503100014 ENDBIB 12 0 M035503100015 COMMON 2 3 M035503100016 E-MIN ERR-1 M035503100017 MEV PER-CENT M035503100018 10. 10. M035503100019 ENDCOMMON 3 0 M035503100020 DATA 3 1 M035503100021 EN-MIN EN-MAX DATA M035503100022 MEV MEV MB M035503100023 55. 85. 2.80 M035503100024 ENDDATA 3 0 M035503100025 ENDSUBENT 24 0 M035503199999 SUBENT M0355032 20180218 M095M035503200001 BIB 5 12 M035503200002 REACTION (16-S-0(G,X)0-NN-1,PAR,DA,,4PI/BRA) M035503200003 ANALYSIS (INTED,4PI1A) M035503200004 ERR-ANALYS (DATA-ERR,8.,10.) M035503200005 Sum of statistical and normalization errors are M035503200006 presented. M035503200007 (ERR-1) In addition all values depend on an absolute M035503200008 normalization in terms of the deuteron M035503200009 photodisintegration cross section, which is known to M035503200010 about 10% at these energies. M035503200011 STATUS (TABLE) Data from Table 1 of PR,175,1330,1968. M035503200012 HISTORY (20180218A) Corrected by S and VV: SF9 = EXP deleted M035503200013 from REACTION code, ERR-1, EN-MIN. M035503200014 ENDBIB 12 0 M035503200015 COMMON 2 3 M035503200016 E-MIN ERR-1 M035503200017 MEV PER-CENT M035503200018 10. 10. M035503200019 ENDCOMMON 3 0 M035503200020 DATA 3 1 M035503200021 EN-MIN EN-MAX DATA M035503200022 MEV MEV MB M035503200023 55. 85. 2.10 M035503200024 ENDDATA 3 0 M035503200025 ENDSUBENT 24 0 M035503299999 SUBENT M0355033 20180218 M095M035503300001 BIB 5 12 M035503300002 REACTION (26-FE-0(G,X)0-NN-1,PAR,DA,,4PI/BRA) M035503300003 ANALYSIS (INTED,4PI1A) M035503300004 ERR-ANALYS (DATA-ERR,8.,10.) M035503300005 Sum of statistical and normalization errors are M035503300006 presented. M035503300007 (ERR-1) In addition all values depend on an absolute M035503300008 normalization in terms of the deuteron M035503300009 photodisintegration cross section, which is known to M035503300010 about 10% at these energies. M035503300011 STATUS (TABLE) Data from Table 1 of PR,175,1330,1968. M035503300012 HISTORY (20180218A) Corrected by S and VV: SF9 = EXP deleted M035503300013 from REACTION code, ERR-1, EN-MIN. M035503300014 ENDBIB 12 0 M035503300015 COMMON 2 3 M035503300016 E-MIN ERR-1 M035503300017 MEV PER-CENT M035503300018 10. 10. M035503300019 ENDCOMMON 3 0 M035503300020 DATA 3 1 M035503300021 EN-MIN EN-MAX DATA M035503300022 MEV MEV MB M035503300023 55. 85. 4.20 M035503300024 ENDDATA 3 0 M035503300025 ENDSUBENT 24 0 M035503399999 SUBENT M0355034 20180218 M095M035503400001 BIB 5 12 M035503400002 REACTION (29-CU-0(G,X)0-NN-1,PAR,DA,,4PI/BRA) M035503400003 ANALYSIS (INTED,4PI1A) M035503400004 ERR-ANALYS (DATA-ERR,8.,10.) M035503400005 Sum of statistical and normalization errors are M035503400006 presented. M035503400007 (ERR-1) In addition all values depend on an absolute M035503400008 normalization in terms of the deuteron M035503400009 photodisintegration cross section, which is known to M035503400010 about 10% at these energies. M035503400011 STATUS (TABLE) Data from Table 1 of PR,175,1330,1968. M035503400012 HISTORY (20180218A) Corrected by S and VV: SF9 = EXP deleted M035503400013 from REACTION code, ERR-1, EN-MIN. M035503400014 ENDBIB 12 0 M035503400015 COMMON 2 3 M035503400016 E-MIN ERR-1 M035503400017 MEV PER-CENT M035503400018 10. 10. M035503400019 ENDCOMMON 3 0 M035503400020 DATA 3 1 M035503400021 EN-MIN EN-MAX DATA M035503400022 MEV MEV MB M035503400023 55. 85. 4.30 M035503400024 ENDDATA 3 0 M035503400025 ENDSUBENT 24 0 M035503499999 SUBENT M0355035 20180218 M095M035503500001 BIB 5 12 M035503500002 REACTION (30-ZN-0(G,X)0-NN-1,PAR,DA,,4PI/BRA) M035503500003 ANALYSIS (INTED,4PI1A) M035503500004 ERR-ANALYS (DATA-ERR,8.,10.) M035503500005 Sum of statistical and normalization errors are M035503500006 presented. M035503500007 (ERR-1) In addition all values depend on an absolute M035503500008 normalization in terms of the deuteron M035503500009 photodisintegration cross section, which is known to M035503500010 about 10% at these energies. M035503500011 STATUS (TABLE) Data from Table 1 of PR,175,1330,1968. M035503500012 HISTORY (20180218A) Corrected by S and VV: SF9 = EXP deleted M035503500013 from REACTION code, ERR-1, EN-MIN. M035503500014 ENDBIB 12 0 M035503500015 COMMON 2 3 M035503500016 E-MIN ERR-1 M035503500017 MEV PER-CENT M035503500018 10. 10. M035503500019 ENDCOMMON 3 0 M035503500020 DATA 3 1 M035503500021 EN-MIN EN-MAX DATA M035503500022 MEV MEV MB M035503500023 55. 85. 4.40 M035503500024 ENDDATA 3 0 M035503500025 ENDSUBENT 24 0 M035503599999 SUBENT M0355036 20180218 M095M035503600001 BIB 5 12 M035503600002 REACTION (49-IN-0(G,X)0-NN-1,PAR,DA,,4PI/BRA) M035503600003 ANALYSIS (INTED,4PI1A) M035503600004 ERR-ANALYS (DATA-ERR,8.,10.) M035503600005 Sum of statistical and normalization errors are M035503600006 presented. M035503600007 (ERR-1) In addition all values depend on an absolute M035503600008 normalization in terms of the deuteron M035503600009 photodisintegration cross section, which is known to M035503600010 about 10% at these energies. M035503600011 STATUS (TABLE) Data from Table 1 of PR,175,1330,1968. M035503600012 HISTORY (20180218A) Corrected by S and VV: SF9 = EXP deleted M035503600013 from REACTION code, ERR-1, EN-MIN. M035503600014 ENDBIB 12 0 M035503600015 COMMON 2 3 M035503600016 E-MIN ERR-1 M035503600017 MEV PER-CENT M035503600018 10. 10. M035503600019 ENDCOMMON 3 0 M035503600020 DATA 3 1 M035503600021 EN-MIN EN-MAX DATA M035503600022 MEV MEV MB M035503600023 55. 85. 7.40 M035503600024 ENDDATA 3 0 M035503600025 ENDSUBENT 24 0 M035503699999 SUBENT M0355037 20180218 M095M035503700001 BIB 5 12 M035503700002 REACTION (50-SN-0(G,X)0-NN-1,PAR,DA,,4PI/BRA) M035503700003 ANALYSIS (INTED,4PI1A) M035503700004 ERR-ANALYS (DATA-ERR,8.,10.) M035503700005 Sum of statistical and normalization errors are M035503700006 presented. M035503700007 (ERR-1) In addition all values depend on an absolute M035503700008 normalization in terms of the deuteron M035503700009 photodisintegration cross section, which is known to M035503700010 about 10% at these energies. M035503700011 STATUS (TABLE) Data from Table 1 of PR,175,1330,1968. M035503700012 HISTORY (20180218A) Corrected by S and VV: SF9 = EXP deleted M035503700013 from REACTION code, ERR-1, EN-MIN. M035503700014 ENDBIB 12 0 M035503700015 COMMON 2 3 M035503700016 E-MIN ERR-1 M035503700017 MEV PER-CENT M035503700018 10. 10. M035503700019 ENDCOMMON 3 0 M035503700020 DATA 3 1 M035503700021 EN-MIN EN-MAX DATA M035503700022 MEV MEV MB M035503700023 55. 85. 7.00 M035503700024 ENDDATA 3 0 M035503700025 ENDSUBENT 24 0 M035503799999 SUBENT M0355038 20180218 M095M035503800001 BIB 5 12 M035503800002 REACTION (73-TA-181(G,X)0-NN-1,PAR,DA,,4PI/BRA) M035503800003 ANALYSIS (INTED,4PI1A) M035503800004 ERR-ANALYS (DATA-ERR,8.,10.) M035503800005 Sum of statistical and normalization errors are M035503800006 presented. M035503800007 (ERR-1) In addition all values depend on an absolute M035503800008 normalization in terms of the deuteron M035503800009 photodisintegration cross section, which is known to M035503800010 about 10% at these energies. M035503800011 STATUS (TABLE) Data from Table 1 of PR,175,1330,1968. M035503800012 HISTORY (20180218A) Corrected by S and VV: SF9 = EXP deleted M035503800013 from REACTION code, ERR-1, EN-MIN. M035503800014 ENDBIB 12 0 M035503800015 COMMON 2 3 M035503800016 E-MIN ERR-1 M035503800017 MEV PER-CENT M035503800018 10. 10. M035503800019 ENDCOMMON 3 0 M035503800020 DATA 3 1 M035503800021 EN-MIN EN-MAX DATA M035503800022 MEV MEV MB M035503800023 55. 85. 10.70 M035503800024 ENDDATA 3 0 M035503800025 ENDSUBENT 24 0 M035503899999 SUBENT M0355039 20180218 M095M035503900001 BIB 5 12 M035503900002 REACTION (81-TL-0(G,X)0-NN-1,PAR,DA,,4PI/BRA) M035503900003 ANALYSIS (INTED,4PI1A) M035503900004 ERR-ANALYS (DATA-ERR,8.,10.) M035503900005 Sum of statistical and normalization errors are M035503900006 presented. M035503900007 (ERR-1) In addition all values depend on an absolute M035503900008 normalization in terms of the deuteron M035503900009 photodisintegration cross section, which is known to M035503900010 about 10% at these energies. M035503900011 STATUS (TABLE) Data from Table 1 of PR,175,1330,1968. M035503900012 HISTORY (20180218A) Corrected by S and VV: SF9 = EXP deleted M035503900013 from REACTION code, ERR-1, EN-MIN. M035503900014 ENDBIB 12 0 M035503900015 COMMON 2 3 M035503900016 E-MIN ERR-1 M035503900017 MEV PER-CENT M035503900018 10. 10. M035503900019 ENDCOMMON 3 0 M035503900020 DATA 3 1 M035503900021 EN-MIN EN-MAX DATA M035503900022 MEV MEV MB M035503900023 55. 85. 10.70 M035503900024 ENDDATA 3 0 M035503900025 ENDSUBENT 24 0 M035503999999 SUBENT M0355040 20180218 M095M035504000001 BIB 5 12 M035504000002 REACTION (82-PB-0(G,X)0-NN-1,PAR,DA,,4PI/BRA) M035504000003 ANALYSIS (INTED,4PI1A) M035504000004 ERR-ANALYS (DATA-ERR,8.,10.) M035504000005 Sum of statistical and normalization errors are M035504000006 presented. M035504000007 (ERR-1) In addition all values depend on an absolute M035504000008 normalization in terms of the deuteron M035504000009 photodisintegration cross section, which is known to M035504000010 about 10% at these energies. M035504000011 STATUS (TABLE) Data from Table 1 of PR,175,1330,1968. M035504000012 HISTORY (20180218A) Corrected by S and VV: SF9 = EXP deleted M035504000013 from REACTION code, ERR-1, EN-MIN. M035504000014 ENDBIB 12 0 M035504000015 COMMON 2 3 M035504000016 E-MIN ERR-1 M035504000017 MEV PER-CENT M035504000018 10. 10. M035504000019 ENDCOMMON 3 0 M035504000020 DATA 3 1 M035504000021 EN-MIN EN-MAX DATA M035504000022 MEV MEV MB M035504000023 55. 85. 8.30 M035504000024 ENDDATA 3 0 M035504000025 ENDSUBENT 24 0 M035504099999 SUBENT M0355041 20180218 M095M035504100001 BIB 5 12 M035504100002 REACTION (83-BI-209(G,X)0-NN-1,PAR,DA,,4PI/BRA) M035504100003 ANALYSIS (INTED,4PI1A) M035504100004 ERR-ANALYS (DATA-ERR,8.,10.) M035504100005 Sum of statistical and normalization errors are M035504100006 presented. M035504100007 (ERR-1) In addition all values depend on an absolute M035504100008 normalization in terms of the deuteron M035504100009 photodisintegration cross section, which is known to M035504100010 about 10% at these energies. M035504100011 STATUS (TABLE) Data from Table 1 of PR,175,1330,1968. M035504100012 HISTORY (20180218A) Corrected by S and VV: SF9 = EXP deleted M035504100013 from REACTION code, ERR-1, EN-MIN. M035504100014 ENDBIB 12 0 M035504100015 COMMON 2 3 M035504100016 E-MIN ERR-1 M035504100017 MEV PER-CENT M035504100018 10. 10. M035504100019 ENDCOMMON 3 0 M035504100020 DATA 3 1 M035504100021 EN-MIN EN-MAX DATA M035504100022 MEV MEV MB M035504100023 55. 85. 13.00 M035504100024 ENDDATA 3 0 M035504100025 ENDSUBENT 24 0 M035504199999 SUBENT M0355042 20180218 M095M035504200001 BIB 5 12 M035504200002 REACTION (92-U-0(G,X)0-NN-1,PAR,DA,,4PI/BRA) M035504200003 ANALYSIS (INTED,4PI1A) M035504200004 ERR-ANALYS (DATA-ERR,8.,10.) M035504200005 Sum of statistical and normalization errors are M035504200006 presented. M035504200007 (ERR-1) In addition all values depend on an absolute M035504200008 normalization in terms of the deuteron M035504200009 photodisintegration cross section, which is known to M035504200010 about 10% at these energies. M035504200011 STATUS (TABLE) Data from Table 1 of PR,175,1330,1968. M035504200012 HISTORY (20180218A) Corrected by S and VV: SF9 = EXP deleted M035504200013 from REACTION code, ERR-1, EN-MIN. M035504200014 ENDBIB 12 0 M035504200015 COMMON 2 3 M035504200016 E-MIN ERR-1 M035504200017 MEV PER-CENT M035504200018 10. 10. M035504200019 ENDCOMMON 3 0 M035504200020 DATA 3 1 M035504200021 EN-MIN EN-MAX DATA M035504200022 MEV MEV MB M035504200023 55. 85. 16.00 M035504200024 ENDDATA 3 0 M035504200025 ENDSUBENT 24 0 M035504299999 NOSUBENT M0355043 20180218 M095M035504300001 NOSUBENT M0355044 20180218 M095M035504400001 NOSUBENT M0355045 20180218 M095M035504500001 NOSUBENT M0355046 20180218 M095M035504600001 NOSUBENT M0355047 20180218 M095M035504700001 NOSUBENT M0355048 20180218 M095M035504800001 NOSUBENT M0355049 20180218 M095M035504900001 NOSUBENT M0355050 20180218 M095M035505000001 NOSUBENT M0355051 20180218 M095M035505100001 NOSUBENT M0355052 20180218 M095M035505200001 NOSUBENT M0355053 20180218 M095M035505300001 NOSUBENT M0355054 20180218 M095M035505400001 NOSUBENT M0355055 20180218 M095M035505500001 NOSUBENT M0355056 20180218 M095M035505600001 NOSUBENT M0355057 20180218 M095M035505700001 NOSUBENT M0355058 20180218 M095M035505800001 NOSUBENT M0355059 20180218 M095M035505900001 ENDENTRY 59 0 M035599999999