ENTRY C2669 20211015 C210C266900000001 SUBENT C2669001 20211015 C210C266900100001 BIB 8 11 C266900100002 TITLE Properties of gamma-ray transitions in 56Co from 56Ni C266900100003 decay and 56Fe(p,n gamma)56Co C266900100004 AUTHOR (L.E.Samuelson,W.H.Kelly,R.R.Todd,R.A.Warner, C266900100005 Wm.C.McHarris, F.M.Bernthal,E.M.Bernstein,R.Shamu) C266900100006 INSTITUTE (1USAMSU,1USAWMU) C266900100007 FACILITY (CYCLO,1USAMSU) C266900100008 REFERENCE (J,PR/C,7,2379,1973) C266900100009 #doi:10.1103/PhysRevC.7.2379 C266900100010 METHOD (GSPEC) C266900100011 ADD-RES (STRUC) C266900100012 HISTORY (20211015C) OG C266900100013 ENDBIB 11 0 C266900100014 NOCOMMON 0 0 C266900100015 ENDSUBENT 14 0 C266900199999 SUBENT C2669002 20211015 C210C266900200001 BIB 9 31 C266900200002 REACTION (26-FE-56(P,N)27-CO-56,PAR,SIG,,REL) C266900200003 EN-SEC (E-LVL,27-CO-56) C266900200004 LEVEL-PROP (27-CO-56,E-LVL=0.158,SPIN=3.,PARITY=+1.) C266900200005 (27-CO-56,E-LVL=0.577,SPIN=5.,PARITY=+1.) C266900200006 (27-CO-56,E-LVL=0.830,SPIN=4.,PARITY=+1.) C266900200007 (27-CO-56,E-LVL=0.970,SPIN=2.,PARITY=+1.) C266900200008 (27-CO-56,E-LVL=1.009,SPIN=5.,PARITY=+1.) C266900200009 (27-CO-56,E-LVL=1.115,SPIN=3.,PARITY=+1.) C266900200010 (27-CO-56,E-LVL=1.451,SPIN=0.,PARITY=+1.) C266900200011 (27-CO-56,E-LVL=1.720,SPIN=1.,PARITY=+1.) C266900200012 DETECTOR (GELI) A 2.5%-efficient Ge(Li) detector at C266900200013 approximately 125 degrees from the beam direction and C266900200014 at 5 cm from the target. C266900200015 SAMPLE (26-FE-56,ENR=0.994) The target was a 0.90-mg/cm2 C266900200016 iron foil. C266900200017 CORRECTION Dead-time and amplifier pileup corrections, and C266900200018 run-to-run normalizations. C266900200019 ANALYSIS Excitation functions for the first eight excited C266900200020 states of 56Co were taken at 125 degrees in order to C266900200021 minimize angular distribution effects. C266900200022 ERR-ANALYS (DATA-ERR) The errors arise from uncertainties in threeC266900200023 different quantities: C266900200024 1) the y-ray peak areas, C266900200025 2) the detector relative gamma-ray efficiency C266900200026 corrections, C266900200027 3) the run-to-run normalization. C266900200028 Error values taken from the figure. For data without C266900200029 given errors the errors are smaller than the data-pointC266900200030 symbols (about 6%). C266900200031 STATUS (CURVE) Fig.8 (p.2392) in Phys.Rev.C,7,2379,1973 was C266900200032 digitized by GSYS2.4.7. C266900200033 ENDBIB 31 0 C266900200034 NOCOMMON 0 0 C266900200035 DATA 4 109 C266900200036 E-LVL EN DATA DATA-ERR C266900200037 MEV MEV ARB-UNITS ARB-UNITS C266900200038 0.158 5.609 1.038E-01 C266900200039 0.158 5.639 1.336E+01 C266900200040 0.158 5.743 2.745E+01 C266900200041 0.158 5.839 1.923E+01 C266900200042 0.158 5.947 3.770E+01 C266900200043 0.158 6.043 3.734E+01 C266900200044 0.158 6.144 4.460E+01 C266900200045 0.158 6.243 3.064E+01 C266900200046 0.158 6.347 3.591E+01 C266900200047 0.158 6.445 4.571E+01 C266900200048 0.158 6.548 4.208E+01 C266900200049 0.158 6.646 3.212E+01 C266900200050 0.158 6.754 3.444E+01 C266900200051 0.158 6.850 3.529E+01 C266900200052 0.158 6.949 4.499E+01 C266900200053 0.158 7.052 3.776E+01 2.504E+00 C266900200054 0.158 7.151 3.502E+01 2.728E+00 C266900200055 0.158 7.255 4.409E+01 3.940E+00 C266900200056 0.158 7.356 3.477E+01 3.650E+00 C266900200057 0.158 7.455 3.454E+01 3.625E+00 C266900200058 0.158 7.657 3.885E+01 3.909E+00 C266900200059 0.158 7.758 2.933E+01 4.390E+00 C266900200060 0.577 6.038 1.035E-01 C266900200061 0.577 6.051 1.300E-01 C266900200062 0.577 6.152 9.470E-01 C266900200063 0.577 6.249 1.469E+00 C266900200064 0.577 6.352 1.087E+00 C266900200065 0.577 6.449 2.638E+00 C266900200066 0.577 6.552 2.860E+00 C266900200067 0.577 6.646 2.657E+00 C266900200068 0.577 6.755 3.202E+00 C266900200069 0.577 6.849 3.361E+00 C266900200070 0.577 6.949 4.019E+00 C266900200071 0.577 7.055 6.818E+00 C266900200072 0.577 7.149 6.543E+00 C266900200073 0.577 7.258 5.788E+00 C266900200074 0.577 7.352 7.693E+00 C266900200075 0.577 7.454 4.914E+00 C266900200076 0.577 7.654 8.133E+00 C266900200077 0.577 7.754 7.997E+00 C266900200078 0.830 6.295 1.025E-01 C266900200079 0.830 6.351 3.710E-01 C266900200080 0.830 6.449 1.387E+00 C266900200081 0.830 6.555 2.511E+00 C266900200082 0.830 6.649 3.420E+00 C266900200083 0.830 6.752 4.733E+00 C266900200084 0.830 6.846 4.291E+00 C266900200085 0.830 6.952 6.444E+00 C266900200086 0.830 7.052 8.564E+00 C266900200087 0.830 7.152 9.911E+00 C266900200088 0.830 7.255 1.110E+01 C266900200089 0.830 7.352 1.306E+01 C266900200090 0.830 7.452 1.118E+01 C266900200091 0.830 7.654 9.416E+00 C266900200092 0.830 7.758 1.336E+01 C266900200093 0.970 6.444 1.041E-01 C266900200094 0.970 6.452 2.205E+00 C266900200095 0.970 6.557 2.068E+01 C266900200096 0.970 6.644 2.067E+01 C266900200097 0.970 6.760 1.592E+01 C266900200098 0.970 6.850 2.082E+01 C266900200099 0.970 6.953 1.768E+01 C266900200100 0.970 7.059 2.275E+01 C266900200101 0.970 7.153 2.527E+01 C266900200102 0.970 7.259 3.071E+01 C266900200103 0.970 7.362 3.070E+01 C266900200104 0.970 7.459 2.946E+01 C266900200105 0.970 7.662 2.919E+01 C266900200106 0.970 7.758 2.990E+01 C266900200107 1.009 6.482 1.050E-01 C266900200108 1.009 6.554 3.099E-01 3.338E-02 C266900200109 1.009 6.651 5.989E-01 6.451E-02 C266900200110 1.009 6.755 1.616E+00 1.741E-01 C266900200111 1.009 6.851 1.215E+00 1.484E-01 C266900200112 1.009 6.952 2.697E+00 2.509E-01 C266900200113 1.009 7.058 2.309E+00 2.654E-01 C266900200114 1.009 7.151 2.384E+00 2.741E-01 C266900200115 1.009 7.258 3.884E+00 4.183E-01 C266900200116 1.009 7.354 3.820E+00 4.390E-01 C266900200117 1.009 7.454 4.795E+00 5.164E-01 C266900200118 1.009 7.654 5.197E+00 6.346E-01 C266900200119 1.009 7.754 5.822E+00 6.692E-01 C266900200120 1.115 6.585 1.032E-01 C266900200121 1.115 6.647 9.384E+00 C266900200122 1.115 6.753 7.170E+00 C266900200123 1.115 6.849 1.077E+01 C266900200124 1.115 6.949 9.144E+00 C266900200125 1.115 7.053 1.362E+01 C266900200126 1.115 7.152 1.329E+01 C266900200127 1.115 7.256 2.653E+01 C266900200128 1.115 7.355 1.838E+01 C266900200129 1.115 7.455 1.439E+01 C266900200130 1.115 7.655 1.748E+01 C266900200131 1.115 7.758 1.820E+01 C266900200132 1.451 6.927 1.048E+00 C266900200133 1.451 6.950 1.793E+00 C266900200134 1.451 7.054 6.538E+00 C266900200135 1.451 7.150 5.598E+00 C266900200136 1.451 7.253 5.781E+00 C266900200137 1.451 7.354 1.369E+01 C266900200138 1.451 7.453 7.079E+00 C266900200139 1.451 7.652 6.573E+00 C266900200140 1.451 7.752 6.57E+00 C266900200141 1.720 7.204 1.038E+00 C266900200142 1.720 7.256 5.688E+00 C266900200143 1.720 7.353 7.938E+00 C266900200144 1.720 7.453 1.135E+01 C266900200145 1.720 7.653 1.25E+01 C266900200146 1.720 7.753 1.036E+01 C266900200147 ENDDATA 111 0 C266900200148 ENDSUBENT 147 0 C266900299999 SUBENT C2669003 20220110 C210C266900300001 BIB 8 22 C266900300002 REACTION (26-FE-56(P,N)27-CO-56,PAR,DA,G,REL) C266900300003 DETECTOR (GELI) A 2.5%-efficient Ge(Li) detector was rigidly C266900300004 mounted on the goniometer arm with the face of C266900300005 the detector 12.7 cm from the target. The detector C266900300006 subtended approximately 10 degrees of arc. C266900300007 (SIBAR) The monitor of proton beam C266900300008 SAMPLE A thin strip of iron foil measuring 1 mm by 10 mm C266900300009 was carefully positioned on the axis of rotation of a C266900300010 high angular precision goniometer. C266900300011 CORRECTION Dead-time and amplifier pileup corrections, and C266900300012 run-to-run normalizations. C266900300013 ADD-RES Least-squares fits to the experimental gamma-ray C266900300014 angular distributions using the computer code GADFIT C266900300015 were made; the even order Legendre polynomial C266900300016 equation was used, the fitting parameters and mixing C266900300017 ratio were defined. C266900300018 ANALYSIS Angular distributions of 56Co gamma rays has been C266900300019 normalized to 1 at 90 degrees. C266900300020 ERR-ANALYS (DATA-ERR) The major uncertainties are in the gamma-rayC266900300021 peak areas and the angle-to-angle normalizations. C266900300022 STATUS (CURVE) Fig.11 (p.2396) in Phys.Rev.C,7,2379,1973 was C266900300023 digitized by GSYS2.4.7. C266900300024 ENDBIB 22 0 C266900300025 COMMON 2 3 C266900300026 EN E C266900300027 MEV KEV C266900300028 5.77 158.4 C266900300029 ENDCOMMON 3 0 C266900300030 DATA 3 10 C266900300031 ANG DATA DATA-ERR C266900300032 ADEG ARB-UNITS ARB-UNITS C266900300033 1.099 0.860 0.012 C266900300034 11.143 0.843 0.018 C266900300035 21.001 0.854 0.015 C266900300036 31.038 0.864 0.014 C266900300037 41.422 0.917 0.019 C266900300038 51.197 0.930 0.017 C266900300039 61.488 0.971 0.015 C266900300040 71.689 1.042 0.019 C266900300041 81.359 1.012 0.013 C266900300042 91.615 0.944 0.014 C266900300043 ENDDATA 12 0 C266900300044 ENDSUBENT 43 0 C266900399999 SUBENT C2669004 20220110 C210C266900400001 BIB 8 22 C266900400002 REACTION (26-FE-56(P,N)27-CO-56,PAR,DA,G,REL) C266900400003 DETECTOR (GELI) A 2.5%-efficient Ge(Li) detector was rigidly C266900400004 mounted on the goniometer arm with the face of C266900400005 the detector 12.7 cm from the target. The detector C266900400006 subtended approximately 10 degrees of arc. C266900400007 (SIBAR) The monitor of proton beam C266900400008 SAMPLE A thin strip of iron foil measuring 1 mm by 10 mm C266900400009 was carefully positioned on the axis of rotation of a C266900400010 high angular precision goniometer. C266900400011 CORRECTION Dead-time and amplifier pileup corrections, and C266900400012 run-to-run normalizations. C266900400013 ADD-RES Least-squares fits to the experimental gamma-ray C266900400014 angular distributions using the computer code GADFIT C266900400015 were made; the even order Legendre polynomial C266900400016 equation was used, the fitting parameters and mixing C266900400017 ratio were defined. C266900400018 ANALYSIS Angular distributions of 56Co gamma rays has been C266900400019 normalized to 1 at 90 degrees. C266900400020 ERR-ANALYS (DATA-ERR) The major uncertainties are in the gamma-rayC266900400021 peak areas and the angle-to-angle normalizations. C266900400022 STATUS (CURVE) Fig.11 (p.2396) in Phys.Rev.C,7,2379,1973 was C266900400023 digitized by GSYS2.4.7. C266900400024 ENDBIB 22 0 C266900400025 COMMON 2 3 C266900400026 EN E C266900400027 MEV KEV C266900400028 6.65 158.4 C266900400029 ENDCOMMON 3 0 C266900400030 DATA 3 10 C266900400031 ANG DATA DATA-ERR C266900400032 ADEG ARB-UNITS ARB-UNITS C266900400033 1.793 0.929 0.012 C266900400034 11.833 0.932 0.017 C266900400035 21.693 0.924 0.015 C266900400036 32.092 0.916 0.013 C266900400037 42.131 0.921 0.012 C266900400038 52.350 0.939 0.012 C266900400039 62.749 0.971 0.015 C266900400040 72.968 1.041 0.009 C266900400041 83.187 1.011 0.013 C266900400042 92.868 0.944 0.013 C266900400043 ENDDATA 12 0 C266900400044 ENDSUBENT 43 0 C266900499999 SUBENT C2669005 20220110 C210C266900500001 BIB 8 22 C266900500002 REACTION (26-FE-56(P,N)27-CO-56,PAR,DA,G,REL) C266900500003 DETECTOR (GELI) A 2.5%-efficient Ge(Li) detector was rigidly C266900500004 mounted on the goniometer arm with the face of C266900500005 the detector 12.7 cm from the target. The detector C266900500006 subtended approximately 10 degrees of arc. C266900500007 (SIBAR) The monitor of proton beam C266900500008 SAMPLE A thin strip of iron foil measuring 1 mm by 10 mm C266900500009 was carefully positioned on the axis of rotation of a C266900500010 high angular precision goniometer. C266900500011 CORRECTION Dead-time and amplifier pileup corrections, and C266900500012 run-to-run normalizations. C266900500013 ADD-RES Least-squares fits to the experimental gamma-ray C266900500014 angular distributions using the computer code GADFIT C266900500015 were made; the even order Legendre polynomial C266900500016 equation was used, the fitting parameters and mixing C266900500017 ratio were defined. C266900500018 ANALYSIS Angular distributions of 56Co gamma rays has been C266900500019 normalized to 1 at 90 degrees. C266900500020 ERR-ANALYS (DATA-ERR) The major uncertainties are in the gamma-rayC266900500021 peak areas and the angle-to-angle normalizations. C266900500022 STATUS (CURVE) Fig.11 (p.2396) in Phys.Rev.C,7,2379,1973 was C266900500023 digitized by GSYS2.4.7. C266900500024 ENDBIB 22 0 C266900500025 COMMON 2 3 C266900500026 EN E C266900500027 MEV KEV C266900500028 6.65 285.0 C266900500029 ENDCOMMON 3 0 C266900500030 DATA 3 10 C266900500031 ANG DATA DATA-ERR C266900500032 ADEG ARB-UNITS ARB-UNITS C266900500033 0.278 0.758 0.031 C266900500034 10.864 0.748 0.050 C266900500035 20.731 0.740 0.034 C266900500036 30.906 0.846 0.036 C266900500037 40.949 0.845 0.034 C266900500038 51.154 0.885 0.031 C266900500039 61.570 0.851 0.031 C266900500040 71.742 0.963 0.038 C266900500041 81.596 0.986 0.035 C266900500042 91.801 1.024 0.036 C266900500043 ENDDATA 12 0 C266900500044 ENDSUBENT 43 0 C266900599999 SUBENT C2669006 20220110 C210C266900600001 BIB 8 22 C266900600002 REACTION (26-FE-56(P,N)27-CO-56,PAR,DA,G,REL) C266900600003 DETECTOR (GELI) A 2.5%-efficient Ge(Li) detector was rigidly C266900600004 mounted on the goniometer arm with the face of C266900600005 the detector 12.7 cm from the target. The detector C266900600006 subtended approximately 10 degrees of arc. C266900600007 (SIBAR) The monitor of proton beam C266900600008 SAMPLE A thin strip of iron foil measuring 1 mm by 10 mm C266900600009 was carefully positioned on the axis of rotation of a C266900600010 high angular precision goniometer. C266900600011 CORRECTION Dead-time and amplifier pileup corrections, and C266900600012 run-to-run normalizations. C266900600013 ADD-RES Least-squares fits to the experimental gamma-ray C266900600014 angular distributions using the computer code GADFIT C266900600015 were made; the even order Legendre polynomial C266900600016 equation was used, the fitting parameters and mixing C266900600017 ratio were defined. C266900600018 ANALYSIS Angular distributions of 56Co gamma rays has been C266900600019 normalized to 1 at 90 degrees. C266900600020 ERR-ANALYS (DATA-ERR) The major uncertainties are in the gamma-rayC266900600021 peak areas and the angle-to-angle normalizations. C266900600022 STATUS (CURVE) Fig.11 (p.2396) in Phys.Rev.C,7,2379,1973 was C266900600023 digitized by GSYS2.4.7. C266900600024 ENDBIB 22 0 C266900600025 COMMON 2 3 C266900600026 EN E C266900600027 MEV KEV C266900600028 6.65 576.6 C266900600029 ENDCOMMON 3 0 C266900600030 DATA 3 10 C266900600031 ANG DATA DATA-ERR C266900600032 ADEG ARB-UNITS ARB-UNITS C266900600033 0.009 0.746 0.022 C266900600034 8.497 0.760 0.022 C266900600035 18.341 0.777 0.015 C266900600036 28.704 0.809 0.016 C266900600037 38.901 0.831 0.021 C266900600038 48.727 0.863 0.019 C266900600039 59.089 0.896 0.023 C266900600040 69.064 0.953 0.025 C266900600041 79.427 0.985 0.018 C266900600042 89.444 1.008 0.018 C266900600043 ENDDATA 12 0 C266900600044 ENDSUBENT 43 0 C266900699999 SUBENT C2669007 20220110 C210C266900700001 BIB 8 22 C266900700002 REACTION (26-FE-56(P,N)27-CO-56,PAR,DA,G,REL) C266900700003 DETECTOR (GELI) A 2.5%-efficient Ge(Li) detector was rigidly C266900700004 mounted on the goniometer arm with the face of C266900700005 the detector 12.7 cm from the target. The detector C266900700006 subtended approximately 10 degrees of arc. C266900700007 (SIBAR) The monitor of proton beam C266900700008 SAMPLE A thin strip of iron foil measuring 1 mm by 10 mm C266900700009 was carefully positioned on the axis of rotation of a C266900700010 high angular precision goniometer. C266900700011 CORRECTION Dead-time and amplifier pileup corrections, and C266900700012 run-to-run normalizations. C266900700013 ADD-RES Least-squares fits to the experimental gamma-ray C266900700014 angular distributions using the computer code GADFIT C266900700015 were made; the even order Legendre polynomial C266900700016 equation was used, the fitting parameters and mixing C266900700017 ratio were defined. C266900700018 ANALYSIS Angular distributions of 56Co gamma rays has been C266900700019 normalized to 1 at 90 degrees. C266900700020 ERR-ANALYS (DATA-ERR) The major uncertainties are in the gamma-rayC266900700021 peak areas and the angle-to-angle normalizations. C266900700022 STATUS (CURVE) Fig.11 (p.2396) in Phys.Rev.C,7,2379,1973 was C266900700023 digitized by GSYS2.4.7. C266900700024 ENDBIB 22 0 C266900700025 COMMON 2 3 C266900700026 EN E C266900700027 MEV KEV C266900700028 6.65 671.3 C266900700029 ENDCOMMON 3 0 C266900700030 DATA 3 10 C266900700031 ANG DATA DATA-ERR C266900700032 ADEG ARB-UNITS ARB-UNITS C266900700033 1.097 1.204 0.030 C266900700034 11.258 1.225 0.029 C266900700035 21.244 1.178 0.042 C266900700036 31.048 1.187 0.048 C266900700037 41.386 1.229 0.030 C266900700038 51.556 1.079 0.029 C266900700039 61.719 1.057 0.027 C266900700040 71.521 1.103 0.033 C266900700041 81.865 1.043 0.033 C266900700042 91.853 0.945 0.034 C266900700043 ENDDATA 12 0 C266900700044 ENDSUBENT 43 0 C266900799999 SUBENT C2669008 20220110 C210C266900800001 BIB 8 22 C266900800002 REACTION (26-FE-56(P,N)27-CO-56,PAR,DA,G,REL) C266900800003 DETECTOR (GELI) A 2.5%-efficient Ge(Li) detector was rigidly C266900800004 mounted on the goniometer arm with the face of C266900800005 the detector 12.7 cm from the target. The detector C266900800006 subtended approximately 10 degrees of arc. C266900800007 (SIBAR) The monitor of proton beam C266900800008 SAMPLE A thin strip of iron foil measuring 1 mm by 10 mm C266900800009 was carefully positioned on the axis of rotation of a C266900800010 high angular precision goniometer. C266900800011 CORRECTION Dead-time and amplifier pileup corrections, and C266900800012 run-to-run normalizations. C266900800013 ADD-RES Least-squares fits to the experimental gamma-ray C266900800014 angular distributions using the computer code GADFIT C266900800015 were made; the even order Legendre polynomial C266900800016 equation was used, the fitting parameters and mixing C266900800017 ratio were defined. C266900800018 ANALYSIS Angular distributions of 56Co gamma rays has been C266900800019 normalized to 1 at 90 degrees. C266900800020 ERR-ANALYS (DATA-ERR) The major uncertainties are in the gamma-rayC266900800021 peak areas and the angle-to-angle normalizations. C266900800022 STATUS (CURVE) Fig.11 (p.2396) in Phys.Rev.C,7,2379,1973 was C266900800023 digitized by GSYS2.4.7. C266900800024 ENDBIB 22 0 C266900800025 COMMON 2 3 C266900800026 EN E C266900800027 MEV KEV C266900800028 6.65 811.9 C266900800029 ENDCOMMON 3 0 C266900800030 DATA 3 10 C266900800031 ANG DATA DATA-ERR C266900800032 ADEG ARB-UNITS ARB-UNITS C266900800033 0.070 0.810 0.006 C266900800034 10.035 0.820 0.005 C266900800035 20.266 0.822 0.005 C266900800036 29.784 0.842 0.006 C266900800037 40.377 0.851 0.006 C266900800038 50.345 0.864 0.006 C266900800039 60.494 0.875 0.006 C266900800040 70.464 0.886 0.004 C266900800041 80.304 0.903 0.008 C266900800042 90.595 0.898 0.007 C266900800043 ENDDATA 12 0 C266900800044 ENDSUBENT 43 0 C266900899999 SUBENT C2669009 20220110 C210C266900900001 BIB 8 22 C266900900002 REACTION (26-FE-56(P,N)27-CO-56,PAR,DA,G,REL) C266900900003 DETECTOR (GELI) A 2.5%-efficient Ge(Li) detector was rigidly C266900900004 mounted on the goniometer arm with the face of C266900900005 the detector 12.7 cm from the target. The detector C266900900006 subtended approximately 10 degrees of arc. C266900900007 (SIBAR) The monitor of proton beam C266900900008 SAMPLE A thin strip of iron foil measuring 1 mm by 10 mm C266900900009 was carefully positioned on the axis of rotation of a C266900900010 high angular precision goniometer. C266900900011 CORRECTION Dead-time and amplifier pileup corrections, and C266900900012 run-to-run normalizations. C266900900013 ADD-RES Least-squares fits to the experimental gamma-ray C266900900014 angular distributions using the computer code GADFIT C266900900015 were made; the even order Legendre polynomial C266900900016 equation was used, the fitting parameters and mixing C266900900017 ratio were defined. C266900900018 ANALYSIS Angular distributions of 56Co gamma rays has been C266900900019 normalized to 1 at 90 degrees. C266900900020 ERR-ANALYS (DATA-ERR) The major uncertainties are in the gamma-rayC266900900021 peak areas and the angle-to-angle normalizations. C266900900022 STATUS (CURVE) Fig.11 (p.2396) in Phys.Rev.C,7,2379,1973 was C266900900023 digitized by GSYS2.4.7. C266900900024 ENDBIB 22 0 C266900900025 COMMON 2 3 C266900900026 EN E C266900900027 MEV KEV C266900900028 6.65 829.8 C266900900029 ENDCOMMON 3 0 C266900900030 DATA 3 10 C266900900031 ANG DATA DATA-ERR C266900900032 ADEG ARB-UNITS ARB-UNITS C266900900033 0.268 2.562 0.170 C266900900034 10.309 2.321 0.170 C266900900035 20.452 2.400 0.184 C266900900036 30.293 2.251 0.194 C266900900037 40.536 1.908 0.174 C266900900038 50.210 1.708 0.146 C266900900039 60.146 1.160 0.116 C266900900040 70.303 1.178 0.123 C266900900041 80.297 1.131 0.106 C266900900042 90.143 0.962 0.095 C266900900043 ENDDATA 12 0 C266900900044 ENDSUBENT 43 0 C266900999999 SUBENT C2669010 20220110 C210C266901000001 BIB 8 22 C266901000002 REACTION (26-FE-56(P,N)27-CO-56,PAR,DA,G,REL) C266901000003 DETECTOR (GELI) A 2.5%-efficient Ge(Li) detector was rigidly C266901000004 mounted on the goniometer arm with the face of C266901000005 the detector 12.7 cm from the target. The detector C266901000006 subtended approximately 10 degrees of arc. C266901000007 (SIBAR) The monitor of proton beam C266901000008 SAMPLE A thin strip of iron foil measuring 1 mm by 10 mm C266901000009 was carefully positioned on the axis of rotation of a C266901000010 high angular precision goniometer. C266901000011 CORRECTION Dead-time and amplifier pileup corrections, and C266901000012 run-to-run normalizations. C266901000013 ADD-RES Least-squares fits to the experimental gamma-ray C266901000014 angular distributions using the computer code GADFIT C266901000015 were made; the even order Legendre polynomial C266901000016 equation was used, the fitting parameters and mixing C266901000017 ratio were defined. C266901000018 ANALYSIS Angular distributions of 56Co gamma rays has been C266901000019 normalized to 1 at 90 degrees. C266901000020 ERR-ANALYS (DATA-ERR) The major uncertainties are in the gamma-rayC266901000021 peak areas and the angle-to-angle normalizations. C266901000022 STATUS (CURVE) Fig.11 (p.2396) in Phys.Rev.C,7,2379,1973 was C266901000023 digitized by GSYS2.4.7. C266901000024 ENDBIB 22 0 C266901000025 COMMON 2 3 C266901000026 EN E C266901000027 MEV KEV C266901000028 6.65 1009.2 C266901000029 ENDCOMMON 3 0 C266901000030 DATA 3 10 C266901000031 ANG DATA DATA-ERR C266901000032 ADEG ARB-UNITS ARB-UNITS C266901000033 0.599 1.007 0.067 C266901000034 10.200 0.978 0.065 C266901000035 20.077 1.059 0.067 C266901000036 30.224 1.042 0.073 C266901000037 40.418 0.879 0.063 C266901000038 50.269 0.929 0.065 C266901000039 60.699 1.031 0.070 C266901000040 70.662 1.008 0.073 C266901000041 80.643 1.004 0.071 C266901000042 90.385 0.934 0.062 C266901000043 ENDDATA 12 0 C266901000044 ENDSUBENT 43 0 C266901099999 SUBENT C2669011 20220110 C210C266901100001 BIB 8 22 C266901100002 REACTION (26-FE-56(P,N)27-CO-56,PAR,DA,G,REL) C266901100003 DETECTOR (GELI) A 2.5%-efficient Ge(Li) detector was rigidly C266901100004 mounted on the goniometer arm with the face of C266901100005 the detector 12.7 cm from the target. The detector C266901100006 subtended approximately 10 degrees of arc. C266901100007 (SIBAR) The monitor of proton beam C266901100008 SAMPLE A thin strip of iron foil measuring 1 mm by 10 mm C266901100009 was carefully positioned on the axis of rotation of a C266901100010 high angular precision goniometer. C266901100011 CORRECTION Dead-time and amplifier pileup corrections, and C266901100012 run-to-run normalizations. C266901100013 ADD-RES Least-squares fits to the experimental gamma-ray C266901100014 angular distributions using the computer code GADFIT C266901100015 were made; the even order Legendre polynomial C266901100016 equation was used, the fitting parameters and mixing C266901100017 ratio were defined. C266901100018 ANALYSIS Angular distributions of 56Co gamma rays has been C266901100019 normalized to 1 at 90 degrees. C266901100020 ERR-ANALYS (DATA-ERR) The major uncertainties are in the gamma-rayC266901100021 peak areas and the angle-to-angle normalizations. C266901100022 STATUS (CURVE) Fig.11 (p.2396) in Phys.Rev.C,7,2379,1973 was C266901100023 digitized by GSYS2.4.7. C266901100024 ENDBIB 22 0 C266901100025 COMMON 2 3 C266901100026 EN E C266901100027 MEV KEV C266901100028 6.65 1114.6 C266901100029 ENDCOMMON 3 0 C266901100030 DATA 3 10 C266901100031 ANG DATA DATA-ERR C266901100032 ADEG ARB-UNITS ARB-UNITS C266901100033 3.854 0.946 0.016 C266901100034 13.722 0.964 0.014 C266901100035 23.580 0.946 0.020 C266901100036 33.446 0.958 0.014 C266901100037 43.487 0.965 0.015 C266901100038 53.353 0.975 0.015 C266901100039 63.217 0.982 0.018 C266901100040 73.259 0.990 0.016 C266901100041 83.303 1.010 0.015 C266901100042 93.160 0.986 0.015 C266901100043 ENDDATA 12 0 C266901100044 ENDSUBENT 43 0 C266901199999 SUBENT C2669012 20220110 C210C266901200001 BIB 8 22 C266901200002 REACTION (26-FE-56(P,N)27-CO-56,PAR,DA,G,REL) C266901200003 DETECTOR (GELI) A 2.5%-efficient Ge(Li) detector was rigidly C266901200004 mounted on the goniometer arm with the face of C266901200005 the detector 12.7 cm from the target. The detector C266901200006 subtended approximately 10 degrees of arc. C266901200007 (SIBAR) The monitor of proton beam C266901200008 SAMPLE A thin strip of iron foil measuring 1 mm by 10 mm C266901200009 was carefully positioned on the axis of rotation of a C266901200010 high angular precision goniometer. C266901200011 CORRECTION Dead-time and amplifier pileup corrections, and C266901200012 run-to-run normalizations. C266901200013 ADD-RES Least-squares fits to the experimental gamma-ray C266901200014 angular distributions using the computer code GADFIT C266901200015 were made; the even order Legendre polynomial C266901200016 equation was used, the fitting parameters and mixing C266901200017 ratio were defined. C266901200018 ANALYSIS Angular distributions of 56Co gamma rays has been C266901200019 normalized to 1 at 90 degrees. C266901200020 ERR-ANALYS (DATA-ERR) The major uncertainties are in the gamma-rayC266901200021 peak areas and the angle-to-angle normalizations. C266901200022 STATUS (CURVE) Fig.11 (p.2396) in Phys.Rev.C,7,2379,1973 was C266901200023 digitized by GSYS2.4.7. C266901200024 ENDBIB 22 0 C266901200025 COMMON 2 3 C266901200026 EN E C266901200027 MEV KEV C266901200028 7.05 158.4 C266901200029 ENDCOMMON 3 0 C266901200030 DATA 3 10 C266901200031 ANG DATA DATA-ERR C266901200032 ADEG ARB-UNITS ARB-UNITS C266901200033 3.526 1.012 0.016 C266901200034 13.375 0.958 0.013 C266901200035 23.234 0.943 0.020 C266901200036 33.452 0.953 0.013 C266901200037 42.967 0.969 0.026 C266901200038 52.828 0.962 0.023 C266901200039 63.226 0.989 0.017 C266901200040 73.105 1.051 0.016 C266901200041 82.957 1.008 0.017 C266901200042 92.802 0.939 0.015 C266901200043 ENDDATA 12 0 C266901200044 ENDSUBENT 43 0 C266901299999 SUBENT C2669013 20220110 C210C266901300001 BIB 8 22 C266901300002 REACTION (26-FE-56(P,N)27-CO-56,PAR,DA,G,REL) C266901300003 DETECTOR (GELI) A 2.5%-efficient Ge(Li) detector was rigidly C266901300004 mounted on the goniometer arm with the face of C266901300005 the detector 12.7 cm from the target. The detector C266901300006 subtended approximately 10 degrees of arc. C266901300007 (SIBAR) The monitor of proton beam C266901300008 SAMPLE A thin strip of iron foil measuring 1 mm by 10 mm C266901300009 was carefully positioned on the axis of rotation of a C266901300010 high angular precision goniometer. C266901300011 CORRECTION Dead-time and amplifier pileup corrections, and C266901300012 run-to-run normalizations. C266901300013 ADD-RES Least-squares fits to the experimental gamma-ray C266901300014 angular distributions using the computer code GADFIT C266901300015 were made; the even order Legendre polynomial C266901300016 equation was used, the fitting parameters and mixing C266901300017 ratio were defined. C266901300018 ANALYSIS Angular distributions of 56Co gamma rays has been C266901300019 normalized to 1 at 90 degrees. C266901300020 ERR-ANALYS (DATA-ERR) The major uncertainties are in the gamma-rayC266901300021 peak areas and the angle-to-angle normalizations. C266901300022 STATUS (CURVE) Fig.11 (p.2396) in Phys.Rev.C,7,2379,1973 was C266901300023 digitized by GSYS2.4.7. C266901300024 ENDBIB 22 0 C266901300025 COMMON 2 3 C266901300026 EN E C266901300027 MEV KEV C266901300028 7.05 285.0 C266901300029 ENDCOMMON 3 0 C266901300030 DATA 3 10 C266901300031 ANG DATA DATA-ERR C266901300032 ADEG ARB-UNITS ARB-UNITS C266901300033 3.608 0.798 0.038 C266901300034 13.665 0.838 0.042 C266901300035 23.348 0.831 0.042 C266901300036 33.391 0.839 0.029 C266901300037 43.804 0.888 0.059 C266901300038 53.526 0.967 0.066 C266901300039 63.182 0.897 0.036 C266901300040 73.265 0.997 0.041 C266901300041 83.316 1.024 0.049 C266901300042 93.161 0.982 0.036 C266901300043 ENDDATA 12 0 C266901300044 ENDSUBENT 43 0 C266901399999 SUBENT C2669014 20220110 C210C266901400001 BIB 8 22 C266901400002 REACTION (26-FE-56(P,N)27-CO-56,PAR,DA,G,REL) C266901400003 DETECTOR (GELI) A 2.5%-efficient Ge(Li) detector was rigidly C266901400004 mounted on the goniometer arm with the face of C266901400005 the detector 12.7 cm from the target. The detector C266901400006 subtended approximately 10 degrees of arc. C266901400007 (SIBAR) The monitor of proton beam C266901400008 SAMPLE A thin strip of iron foil measuring 1 mm by 10 mm C266901400009 was carefully positioned on the axis of rotation of a C266901400010 high angular precision goniometer. C266901400011 CORRECTION Dead-time and amplifier pileup corrections, and C266901400012 run-to-run normalizations. C266901400013 ADD-RES Least-squares fits to the experimental gamma-ray C266901400014 angular distributions using the computer code GADFIT C266901400015 were made; the even order Legendre polynomial C266901400016 equation was used, the fitting parameters and mixing C266901400017 ratio were defined. C266901400018 ANALYSIS Angular distributions of 56Co gamma rays has been C266901400019 normalized to 1 at 90 degrees. C266901400020 ERR-ANALYS (DATA-ERR) The major uncertainties are in the gamma-rayC266901400021 peak areas and the angle-to-angle normalizations. C266901400022 STATUS (CURVE) Fig.11 (p.2396) in Phys.Rev.C,7,2379,1973 was C266901400023 digitized by GSYS2.4.7. C266901400024 ENDBIB 22 0 C266901400025 COMMON 2 3 C266901400026 EN E C266901400027 MEV KEV C266901400028 7.05 480.5 C266901400029 ENDCOMMON 3 0 C266901400030 DATA 3 10 C266901400031 ANG DATA DATA-ERR C266901400032 ADEG ARB-UNITS ARB-UNITS C266901400033 3.244 1.003 0.018 C266901400034 13.092 0.973 0.024 C266901400035 23.135 0.981 0.033 C266901400036 33.023 1.032 0.029 C266901400037 42.858 0.975 0.033 C266901400038 52.915 1.011 0.032 C266901400039 62.959 1.020 0.026 C266901400040 72.804 0.985 0.026 C266901400041 82.669 0.989 0.032 C266901400042 92.362 1.001 0.021 C266901400043 ENDDATA 12 0 C266901400044 ENDSUBENT 43 0 C266901499999 SUBENT C2669015 20220110 C210C266901500001 BIB 8 22 C266901500002 REACTION (26-FE-56(P,N)27-CO-56,PAR,DA,G,REL) C266901500003 DETECTOR (GELI) A 2.5%-efficient Ge(Li) detector was rigidly C266901500004 mounted on the goniometer arm with the face of C266901500005 the detector 12.7 cm from the target. The detector C266901500006 subtended approximately 10 degrees of arc. C266901500007 (SIBAR) The monitor of proton beam C266901500008 SAMPLE A thin strip of iron foil measuring 1 mm by 10 mm C266901500009 was carefully positioned on the axis of rotation of a C266901500010 high angular precision goniometer. C266901500011 CORRECTION Dead-time and amplifier pileup corrections, and C266901500012 run-to-run normalizations. C266901500013 ADD-RES Least-squares fits to the experimental gamma-ray C266901500014 angular distributions using the computer code GADFIT C266901500015 were made; the even order Legendre polynomial C266901500016 equation was used, the fitting parameters and mixing C266901500017 ratio were defined. C266901500018 ANALYSIS Angular distributions of 56Co gamma rays has been C266901500019 normalized to 1 at 90 degrees. C266901500020 ERR-ANALYS (DATA-ERR) The major uncertainties are in the gamma-rayC266901500021 peak areas and the angle-to-angle normalizations. C266901500022 STATUS (CURVE) Fig.11 (p.2396) in Phys.Rev.C,7,2379,1973 was C266901500023 digitized by GSYS2.4.7. C266901500024 ENDBIB 22 0 C266901500025 COMMON 2 3 C266901500026 EN E C266901500027 MEV KEV C266901500028 7.05 576.6 C266901500029 ENDCOMMON 3 0 C266901500030 DATA 3 10 C266901500031 ANG DATA DATA-ERR C266901500032 ADEG ARB-UNITS ARB-UNITS C266901500033 1.409 0.771 0.018 C266901500034 11.448 0.816 0.023 C266901500035 21.311 0.815 0.027 C266901500036 31.174 0.813 0.019 C266901500037 41.389 0.842 0.033 C266901500038 51.252 0.901 0.027 C266901500039 61.115 0.944 0.019 C266901500040 71.330 0.976 0.026 C266901500041 81.017 0.984 0.026 C266901500042 91.056 0.983 0.020 C266901500043 ENDDATA 12 0 C266901500044 ENDSUBENT 43 0 C266901599999 SUBENT C2669016 20220110 C210C266901600001 BIB 8 22 C266901600002 REACTION (26-FE-56(P,N)27-CO-56,PAR,DA,G,REL) C266901600003 DETECTOR (GELI) A 2.5%-efficient Ge(Li) detector was rigidly C266901600004 mounted on the goniometer arm with the face of C266901600005 the detector 12.7 cm from the target. The detector C266901600006 subtended approximately 10 degrees of arc. C266901600007 (SIBAR) The monitor of proton beam C266901600008 SAMPLE A thin strip of iron foil measuring 1 mm by 10 mm C266901600009 was carefully positioned on the axis of rotation of a C266901600010 high angular precision goniometer. C266901600011 CORRECTION Dead-time and amplifier pileup corrections, and C266901600012 run-to-run normalizations. C266901600013 ADD-RES Least-squares fits to the experimental gamma-ray C266901600014 angular distributions using the computer code GADFIT C266901600015 were made; the even order Legendre polynomial C266901600016 equation was used, the fitting parameters and mixing C266901600017 ratio were defined. C266901600018 ANALYSIS Angular distributions of 56Co gamma rays has been C266901600019 normalized to 1 at 90 degrees. C266901600020 ERR-ANALYS (DATA-ERR) The major uncertainties are in the gamma-rayC266901600021 peak areas and the angle-to-angle normalizations. C266901600022 STATUS (CURVE) Fig.11 (p.2396) in Phys.Rev.C,7,2379,1973 was C266901600023 digitized by GSYS2.4.7. C266901600024 ENDBIB 22 0 C266901600025 COMMON 2 3 C266901600026 EN E C266901600027 MEV KEV C266901600028 7.05 671.3 C266901600029 ENDCOMMON 3 0 C266901600030 DATA 3 10 C266901600031 ANG DATA DATA-ERR C266901600032 ADEG ARB-UNITS ARB-UNITS C266901600033 2.613 1.215 0.017 C266901600034 12.430 1.162 0.023 C266901600035 22.110 1.186 0.027 C266901600036 31.933 1.144 0.019 C266901600037 41.767 1.126 0.032 C266901600038 51.766 1.086 0.042 C266901600039 61.431 1.080 0.029 C266901600040 71.954 1.033 0.031 C266901600041 81.432 1.006 0.036 C266901600042 91.258 0.971 0.025 C266901600043 ENDDATA 12 0 C266901600044 ENDSUBENT 43 0 C266901699999 SUBENT C2669017 20220110 C210C266901700001 BIB 8 22 C266901700002 REACTION (26-FE-56(P,N)27-CO-56,PAR,DA,G,REL) C266901700003 DETECTOR (GELI) A 2.5%-efficient Ge(Li) detector was rigidly C266901700004 mounted on the goniometer arm with the face of C266901700005 the detector 12.7 cm from the target. The detector C266901700006 subtended approximately 10 degrees of arc. C266901700007 (SIBAR) The monitor of proton beam C266901700008 SAMPLE A thin strip of iron foil measuring 1 mm by 10 mm C266901700009 was carefully positioned on the axis of rotation of a C266901700010 high angular precision goniometer. C266901700011 CORRECTION Dead-time and amplifier pileup corrections, and C266901700012 run-to-run normalizations. C266901700013 ADD-RES Least-squares fits to the experimental gamma-ray C266901700014 angular distributions using the computer code GADFIT C266901700015 were made; the even order Legendre polynomial C266901700016 equation was used, the fitting parameters and mixing C266901700017 ratio were defined. C266901700018 ANALYSIS Angular distributions of 56Co gamma rays has been C266901700019 normalized to 1 at 90 degrees. C266901700020 ERR-ANALYS (DATA-ERR) The major uncertainties are in the gamma-rayC266901700021 peak areas and the angle-to-angle normalizations. C266901700022 STATUS (CURVE) Fig.11 (p.2396) in Phys.Rev.C,7,2379,1973 was C266901700023 digitized by GSYS2.4.7. C266901700024 ENDBIB 22 0 C266901700025 COMMON 2 3 C266901700026 EN E C266901700027 MEV KEV C266901700028 7.05 811.9 C266901700029 ENDCOMMON 3 0 C266901700030 DATA 3 10 C266901700031 ANG DATA DATA-ERR C266901700032 ADEG ARB-UNITS ARB-UNITS C266901700033 0.705 0.917 0.015 C266901700034 10.568 0.878 0.014 C266901700035 20.783 0.889 0.015 C266901700036 30.822 0.928 0.014 C266901700037 40.685 0.920 0.022 C266901700038 50.548 0.973 0.020 C266901700039 60.587 0.962 0.010 C266901700040 70.626 0.978 0.014 C266901700041 80.665 1.009 0.017 C266901700042 90.352 0.985 0.017 C266901700043 ENDDATA 12 0 C266901700044 ENDSUBENT 43 0 C266901799999 SUBENT C2669018 20220110 C210C266901800001 BIB 8 22 C266901800002 REACTION (26-FE-56(P,N)27-CO-56,PAR,DA,G,REL) C266901800003 DETECTOR (GELI) A 2.5%-efficient Ge(Li) detector was rigidly C266901800004 mounted on the goniometer arm with the face of C266901800005 the detector 12.7 cm from the target. The detector C266901800006 subtended approximately 10 degrees of arc. C266901800007 (SIBAR) The monitor of proton beam C266901800008 SAMPLE A thin strip of iron foil measuring 1 mm by 10 mm C266901800009 was carefully positioned on the axis of rotation of a C266901800010 high angular precision goniometer. C266901800011 CORRECTION Dead-time and amplifier pileup corrections, and C266901800012 run-to-run normalizations. C266901800013 ADD-RES Least-squares fits to the experimental gamma-ray C266901800014 angular distributions using the computer code GADFIT C266901800015 were made; the even order Legendre polynomial C266901800016 equation was used, the fitting parameters and mixing C266901800017 ratio were defined. C266901800018 ANALYSIS Angular distributions of 56Co gamma rays has been C266901800019 normalized to 1 at 90 degrees. C266901800020 ERR-ANALYS (DATA-ERR) The major uncertainties are in the gamma-rayC266901800021 peak areas and the angle-to-angle normalizations. C266901800022 STATUS (CURVE) Fig.11 (p.2396) in Phys.Rev.C,7,2379,1973 was C266901800023 digitized by GSYS2.4.7. C266901800024 ENDBIB 22 0 C266901800025 COMMON 2 3 C266901800026 EN E C266901800027 MEV KEV C266901800028 7.05 829.8 C266901800029 ENDCOMMON 3 0 C266901800030 DATA 3 10 C266901800031 ANG DATA DATA-ERR C266901800032 ADEG ARB-UNITS ARB-UNITS C266901800033 0.357 1.960 0.022 C266901800034 10.427 1.879 0.030 C266901800035 20.318 1.824 0.026 C266901800036 30.225 1.656 0.028 C266901800037 40.312 1.463 0.030 C266901800038 50.211 1.346 0.028 C266901800039 59.935 1.222 0.024 C266901800040 70.016 1.074 0.020 C266901800041 79.907 1.013 0.037 C266901800042 89.790 1.005 0.028 C266901800043 ENDDATA 12 0 C266901800044 ENDSUBENT 43 0 C266901899999 SUBENT C2669019 20220110 C210C266901900001 BIB 8 22 C266901900002 REACTION (26-FE-56(P,N)27-CO-56,PAR,DA,G,REL) C266901900003 DETECTOR (GELI) A 2.5%-efficient Ge(Li) detector was rigidly C266901900004 mounted on the goniometer arm with the face of C266901900005 the detector 12.7 cm from the target. The detector C266901900006 subtended approximately 10 degrees of arc. C266901900007 (SIBAR) The monitor of proton beam C266901900008 SAMPLE A thin strip of iron foil measuring 1 mm by 10 mm C266901900009 was carefully positioned on the axis of rotation of a C266901900010 high angular precision goniometer. C266901900011 CORRECTION Dead-time and amplifier pileup corrections, and C266901900012 run-to-run normalizations. C266901900013 ADD-RES Least-squares fits to the experimental gamma-ray C266901900014 angular distributions using the computer code GADFIT C266901900015 were made; the even order Legendre polynomial C266901900016 equation was used, the fitting parameters and mixing C266901900017 ratio were defined. C266901900018 ANALYSIS Angular distributions of 56Co gamma rays has been C266901900019 normalized to 1 at 90 degrees. C266901900020 ERR-ANALYS (DATA-ERR) The major uncertainties are in the gamma-rayC266901900021 peak areas and the angle-to-angle normalizations. C266901900022 STATUS (CURVE) Fig.11 (p.2396) in Phys.Rev.C,7,2379,1973 was C266901900023 digitized by GSYS2.4.7. C266901900024 ENDBIB 22 0 C266901900025 COMMON 2 3 C266901900026 EN E C266901900027 MEV KEV C266901900028 7.05 1009.2 C266901900029 ENDCOMMON 3 0 C266901900030 DATA 3 10 C266901900031 ANG DATA DATA-ERR C266901900032 ADEG ARB-UNITS ARB-UNITS C266901900033 1.953 0.939 0.030 C266901900034 11.893 0.828 0.024 C266901900035 22.012 0.911 0.022 C266901900036 31.953 0.899 0.023 C266901900037 41.893 0.897 0.035 C266901900038 52.012 1.012 0.042 C266901900039 62.130 0.964 0.032 C266901900040 72.071 0.961 0.031 C266901900041 82.012 0.968 0.035 C266901900042 92.130 1.016 0.028 C266901900043 ENDDATA 12 0 C266901900044 ENDSUBENT 43 0 C266901999999 SUBENT C2669020 20220110 C210C266902000001 BIB 8 22 C266902000002 REACTION (26-FE-56(P,N)27-CO-56,PAR,DA,G,REL) C266902000003 DETECTOR (GELI) A 2.5%-efficient Ge(Li) detector was rigidly C266902000004 mounted on the goniometer arm with the face of C266902000005 the detector 12.7 cm from the target. The detector C266902000006 subtended approximately 10 degrees of arc. C266902000007 (SIBAR) The monitor of proton beam C266902000008 SAMPLE A thin strip of iron foil measuring 1 mm by 10 mm C266902000009 was carefully positioned on the axis of rotation of a C266902000010 high angular precision goniometer. C266902000011 CORRECTION Dead-time and amplifier pileup corrections, and C266902000012 run-to-run normalizations. C266902000013 ADD-RES Least-squares fits to the experimental gamma-ray C266902000014 angular distributions using the computer code GADFIT C266902000015 were made; the even order Legendre polynomial C266902000016 equation was used, the fitting parameters and mixing C266902000017 ratio were defined. C266902000018 ANALYSIS Angular distributions of 56Co gamma rays has been C266902000019 normalized to 1 at 90 degrees. C266902000020 ERR-ANALYS (DATA-ERR) The major uncertainties are in the gamma-rayC266902000021 peak areas and the angle-to-angle normalizations. C266902000022 STATUS (CURVE) Fig.11 (p.2396) in Phys.Rev.C,7,2379,1973 was C266902000023 digitized by GSYS2.4.7. C266902000024 ENDBIB 22 0 C266902000025 COMMON 2 3 C266902000026 EN E C266902000027 MEV KEV C266902000028 7.05 1114.6 C266902000029 ENDCOMMON 3 0 C266902000030 DATA 3 10 C266902000031 ANG DATA DATA-ERR C266902000032 ADEG ARB-UNITS ARB-UNITS C266902000033 2.972 1.008 0.023 C266902000034 13.069 0.959 0.020 C266902000035 23.188 0.959 0.017 C266902000036 33.141 0.987 0.017 C266902000037 43.434 0.980 0.028 C266902000038 53.383 0.999 0.030 C266902000039 63.490 0.974 0.020 C266902000040 73.439 0.993 0.021 C266902000041 83.553 0.982 0.028 C266902000042 93.327 1.006 0.024 C266902000043 ENDDATA 12 0 C266902000044 ENDSUBENT 43 0 C266902099999 SUBENT C2669021 20220110 C210C266902100001 BIB 8 22 C266902100002 REACTION (26-FE-56(P,N)27-CO-56,PAR,DA,G,REL) C266902100003 DETECTOR (GELI) A 2.5%-efficient Ge(Li) detector was rigidly C266902100004 mounted on the goniometer arm with the face of C266902100005 the detector 12.7 cm from the target. The detector C266902100006 subtended approximately 10 degrees of arc. C266902100007 (SIBAR) The monitor of proton beam C266902100008 SAMPLE A thin strip of iron foil measuring 1 mm by 10 mm C266902100009 was carefully positioned on the axis of rotation of a C266902100010 high angular precision goniometer. C266902100011 CORRECTION Dead-time and amplifier pileup corrections, and C266902100012 run-to-run normalizations. C266902100013 ADD-RES Least-squares fits to the experimental gamma-ray C266902100014 angular distributions using the computer code GADFIT C266902100015 were made; the even order Legendre polynomial C266902100016 equation was used, the fitting parameters and mixing C266902100017 ratio were defined. C266902100018 ANALYSIS Angular distributions of 56Co gamma rays has been C266902100019 normalized to 1 at 90 degrees. C266902100020 ERR-ANALYS (DATA-ERR) The major uncertainties are in the gamma-rayC266902100021 peak areas and the angle-to-angle normalizations. C266902100022 STATUS (CURVE) Fig.11 (p.2396) in Phys.Rev.C,7,2379,1973 was C266902100023 digitized by GSYS2.4.7. C266902100024 ENDBIB 22 0 C266902100025 COMMON 2 3 C266902100026 EN E C266902100027 MEV KEV C266902100028 7.30 158.4 C266902100029 ENDCOMMON 3 0 C266902100030 DATA 3 10 C266902100031 ANG DATA DATA-ERR C266902100032 ADEG ARB-UNITS ARB-UNITS C266902100033 0.293 0.980 0.023 C266902100034 9.999 0.987 0.031 C266902100035 19.939 0.989 0.017 C266902100036 29.896 0.961 0.017 C266902100037 39.649 0.980 0.033 C266902100038 49.943 0.982 0.029 C266902100039 59.875 0.998 0.020 C266902100040 70.308 1.067 0.043 C266902100041 79.928 1.008 0.028 C266902100042 90.072 0.964 0.024 C266902100043 ENDDATA 12 0 C266902100044 ENDSUBENT 43 0 C266902199999 SUBENT C2669022 20220110 C210C266902200001 BIB 8 22 C266902200002 REACTION (26-FE-56(P,N)27-CO-56,PAR,DA,G,REL) C266902200003 DETECTOR (GELI) A 2.5%-efficient Ge(Li) detector was rigidly C266902200004 mounted on the goniometer arm with the face of C266902200005 the detector 12.7 cm from the target. The detector C266902200006 subtended approximately 10 degrees of arc. C266902200007 (SIBAR) The monitor of proton beam C266902200008 SAMPLE A thin strip of iron foil measuring 1 mm by 10 mm C266902200009 was carefully positioned on the axis of rotation of a C266902200010 high angular precision goniometer. C266902200011 CORRECTION Dead-time and amplifier pileup corrections, and C266902200012 run-to-run normalizations. C266902200013 ADD-RES Least-squares fits to the experimental gamma-ray C266902200014 angular distributions using the computer code GADFIT C266902200015 were made; the even order Legendre polynomial C266902200016 equation was used, the fitting parameters and mixing C266902200017 ratio were defined. C266902200018 ANALYSIS Angular distributions of 56Co gamma rays has been C266902200019 normalized to 1 at 90 degrees. C266902200020 ERR-ANALYS (DATA-ERR) The major uncertainties are in the gamma-rayC266902200021 peak areas and the angle-to-angle normalizations. C266902200022 STATUS (CURVE) Fig.11 (p.2396) in Phys.Rev.C,7,2379,1973 was C266902200023 digitized by GSYS2.4.7. C266902200024 ENDBIB 22 0 C266902200025 COMMON 2 3 C266902200026 EN E C266902200027 MEV KEV C266902200028 7.30 269.5 C266902200029 ENDCOMMON 3 0 C266902200030 DATA 3 10 C266902200031 ANG DATA DATA-ERR C266902200032 ADEG ARB-UNITS ARB-UNITS C266902200033 0.048 0.638 0.018 C266902200034 10.023 0.646 0.018 C266902200035 19.814 0.668 0.016 C266902200036 29.968 0.677 0.009 C266902200037 40.080 0.766 0.020 C266902200038 50.017 0.849 0.022 C266902200039 60.333 0.889 0.015 C266902200040 70.646 0.934 0.026 C266902200041 80.413 1.001 0.018 C266902200042 90.580 0.985 0.015 C266902200043 ENDDATA 12 0 C266902200044 ENDSUBENT 43 0 C266902299999 SUBENT C2669023 20220110 C210C266902300001 BIB 8 22 C266902300002 REACTION (26-FE-56(P,N)27-CO-56,PAR,DA,G,REL) C266902300003 DETECTOR (GELI) A 2.5%-efficient Ge(Li) detector was rigidly C266902300004 mounted on the goniometer arm with the face of C266902300005 the detector 12.7 cm from the target. The detector C266902300006 subtended approximately 10 degrees of arc. C266902300007 (SIBAR) The monitor of proton beam C266902300008 SAMPLE A thin strip of iron foil measuring 1 mm by 10 mm C266902300009 was carefully positioned on the axis of rotation of a C266902300010 high angular precision goniometer. C266902300011 CORRECTION Dead-time and amplifier pileup corrections, and C266902300012 run-to-run normalizations. C266902300013 ADD-RES Least-squares fits to the experimental gamma-ray C266902300014 angular distributions using the computer code GADFIT C266902300015 were made; the even order Legendre polynomial C266902300016 equation was used, the fitting parameters and mixing C266902300017 ratio were defined. C266902300018 ANALYSIS Angular distributions of 56Co gamma rays has been C266902300019 normalized to 1 at 90 degrees. C266902300020 ERR-ANALYS (DATA-ERR) The major uncertainties are in the gamma-rayC266902300021 peak areas and the angle-to-angle normalizations. C266902300022 STATUS (CURVE) Fig.11 (p.2396) in Phys.Rev.C,7,2379,1973 was C266902300023 digitized by GSYS2.4.7. C266902300024 ENDBIB 22 0 C266902300025 COMMON 2 3 C266902300026 EN E C266902300027 MEV KEV C266902300028 7.30 285.0 C266902300029 ENDCOMMON 3 0 C266902300030 DATA 3 10 C266902300031 ANG DATA DATA-ERR C266902300032 ADEG ARB-UNITS ARB-UNITS C266902300033 1.722 0.799 0.030 C266902300034 11.890 0.819 0.039 C266902300035 21.871 0.821 0.030 C266902300036 32.040 0.844 0.038 C266902300037 41.705 0.939 0.037 C266902300038 52.213 0.924 0.037 C266902300039 62.206 0.951 0.024 C266902300040 72.396 1.022 0.041 C266902300041 82.180 0.981 0.018 C266902300042 92.168 1.000 0.018 C266902300043 ENDDATA 12 0 C266902300044 ENDSUBENT 43 0 C266902399999 SUBENT C2669024 20220110 C210C266902400001 BIB 8 22 C266902400002 REACTION (26-FE-56(P,N)27-CO-56,PAR,DA,G,REL) C266902400003 DETECTOR (GELI) A 2.5%-efficient Ge(Li) detector was rigidly C266902400004 mounted on the goniometer arm with the face of C266902400005 the detector 12.7 cm from the target. The detector C266902400006 subtended approximately 10 degrees of arc. C266902400007 (SIBAR) The monitor of proton beam C266902400008 SAMPLE A thin strip of iron foil measuring 1 mm by 10 mm C266902400009 was carefully positioned on the axis of rotation of a C266902400010 high angular precision goniometer. C266902400011 CORRECTION Dead-time and amplifier pileup corrections, and C266902400012 run-to-run normalizations. C266902400013 ADD-RES Least-squares fits to the experimental gamma-ray C266902400014 angular distributions using the computer code GADFIT C266902400015 were made; the even order Legendre polynomial C266902400016 equation was used, the fitting parameters and mixing C266902400017 ratio were defined. C266902400018 ANALYSIS Angular distributions of 56Co gamma rays has been C266902400019 normalized to 1 at 90 degrees. C266902400020 ERR-ANALYS (DATA-ERR) The major uncertainties are in the gamma-rayC266902400021 peak areas and the angle-to-angle normalizations. C266902400022 STATUS (CURVE) Fig.11 (p.2396) in Phys.Rev.C,7,2379,1973 was C266902400023 digitized by GSYS2.4.7. C266902400024 ENDBIB 22 0 C266902400025 COMMON 2 3 C266902400026 EN E C266902400027 MEV KEV C266902400028 7.30 576.6 C266902400029 ENDCOMMON 3 0 C266902400030 DATA 3 10 C266902400031 ANG DATA DATA-ERR C266902400032 ADEG ARB-UNITS ARB-UNITS C266902400033 0.872 0.759 0.016 C266902400034 8.937 0.754 0.022 C266902400035 18.828 0.821 0.022 C266902400036 28.959 0.842 0.020 C266902400037 38.924 0.853 0.027 C266902400038 49.017 0.903 0.027 C266902400039 58.917 0.963 0.024 C266902400040 68.916 0.949 0.023 C266902400041 79.178 1.005 0.018 C266902400042 88.971 1.013 0.015 C266902400043 ENDDATA 12 0 C266902400044 ENDSUBENT 43 0 C266902499999 SUBENT C2669025 20220110 C210C266902500001 BIB 8 22 C266902500002 REACTION (26-FE-56(P,N)27-CO-56,PAR,DA,G,REL) C266902500003 DETECTOR (GELI) A 2.5%-efficient Ge(Li) detector was rigidly C266902500004 mounted on the goniometer arm with the face of C266902500005 the detector 12.7 cm from the target. The detector C266902500006 subtended approximately 10 degrees of arc. C266902500007 (SIBAR) The monitor of proton beam C266902500008 SAMPLE A thin strip of iron foil measuring 1 mm by 10 mm C266902500009 was carefully positioned on the axis of rotation of a C266902500010 high angular precision goniometer. C266902500011 CORRECTION Dead-time and amplifier pileup corrections, and C266902500012 run-to-run normalizations. C266902500013 ADD-RES Least-squares fits to the experimental gamma-ray C266902500014 angular distributions using the computer code GADFIT C266902500015 were made; the even order Legendre polynomial C266902500016 equation was used, the fitting parameters and mixing C266902500017 ratio were defined. C266902500018 ANALYSIS Angular distributions of 56Co gamma rays has been C266902500019 normalized to 1 at 90 degrees. C266902500020 ERR-ANALYS (DATA-ERR) The major uncertainties are in the gamma-rayC266902500021 peak areas and the angle-to-angle normalizations. C266902500022 STATUS (CURVE) Fig.11 (p.2396) in Phys.Rev.C,7,2379,1973 was C266902500023 digitized by GSYS2.4.7. C266902500024 ENDBIB 22 0 C266902500025 COMMON 2 3 C266902500026 EN E C266902500027 MEV KEV C266902500028 7.30 671.3 C266902500029 ENDCOMMON 3 0 C266902500030 DATA 3 10 C266902500031 ANG DATA DATA-ERR C266902500032 ADEG ARB-UNITS ARB-UNITS C266902500033 0.049 1.147 0.016 C266902500034 9.954 1.097 0.030 C266902500035 19.760 1.087 0.022 C266902500036 30.099 1.083 0.020 C266902500037 40.083 1.073 0.027 C266902500038 50.067 1.065 0.035 C266902500039 60.424 1.019 0.039 C266902500040 70.250 0.966 0.032 C266902500041 80.045 0.982 0.026 C266902500042 90.182 1.028 0.026 C266902500043 ENDDATA 12 0 C266902500044 ENDSUBENT 43 0 C266902599999 SUBENT C2669026 20220110 C210C266902600001 BIB 8 22 C266902600002 REACTION (26-FE-56(P,N)27-CO-56,PAR,DA,G,REL) C266902600003 DETECTOR (GELI) A 2.5%-efficient Ge(Li) detector was rigidly C266902600004 mounted on the goniometer arm with the face of C266902600005 the detector 12.7 cm from the target. The detector C266902600006 subtended approximately 10 degrees of arc. C266902600007 (SIBAR) The monitor of proton beam C266902600008 SAMPLE A thin strip of iron foil measuring 1 mm by 10 mm C266902600009 was carefully positioned on the axis of rotation of a C266902600010 high angular precision goniometer. C266902600011 CORRECTION Dead-time and amplifier pileup corrections, and C266902600012 run-to-run normalizations. C266902600013 ADD-RES Least-squares fits to the experimental gamma-ray C266902600014 angular distributions using the computer code GADFIT C266902600015 were made; the even order Legendre polynomial C266902600016 equation was used, the fitting parameters and mixing C266902600017 ratio were defined. C266902600018 ANALYSIS Angular distributions of 56Co gamma rays has been C266902600019 normalized to 1 at 90 degrees. C266902600020 ERR-ANALYS (DATA-ERR) The major uncertainties are in the gamma-rayC266902600021 peak areas and the angle-to-angle normalizations. C266902600022 STATUS (CURVE) Fig.11 (p.2396) in Phys.Rev.C,7,2379,1973 was C266902600023 digitized by GSYS2.4.7. C266902600024 ENDBIB 22 0 C266902600025 COMMON 2 3 C266902600026 EN E C266902600027 MEV KEV C266902600028 7.30 750.1 C266902600029 ENDCOMMON 3 0 C266902600030 DATA 3 10 C266902600031 ANG DATA DATA-ERR C266902600032 ADEG ARB-UNITS ARB-UNITS C266902600033 0.254 0.920 0.023 C266902600034 9.888 0.980 0.030 C266902600035 19.879 0.939 0.022 C266902600036 30.038 0.938 0.021 C266902600037 40.018 0.938 0.027 C266902600038 50.178 0.931 0.036 C266902600039 60.155 0.945 0.026 C266902600040 70.130 0.965 0.029 C266902600041 80.462 0.984 0.026 C266902600042 90.256 1.013 0.023 C266902600043 ENDDATA 12 0 C266902600044 ENDSUBENT 43 0 C266902699999 SUBENT C2669027 20220110 C210C266902700001 BIB 8 22 C266902700002 REACTION (26-FE-56(P,N)27-CO-56,PAR,DA,G,REL) C266902700003 DETECTOR (GELI) A 2.5%-efficient Ge(Li) detector was rigidly C266902700004 mounted on the goniometer arm with the face of C266902700005 the detector 12.7 cm from the target. The detector C266902700006 subtended approximately 10 degrees of arc. C266902700007 (SIBAR) The monitor of proton beam C266902700008 SAMPLE A thin strip of iron foil measuring 1 mm by 10 mm C266902700009 was carefully positioned on the axis of rotation of a C266902700010 high angular precision goniometer. C266902700011 CORRECTION Dead-time and amplifier pileup corrections, and C266902700012 run-to-run normalizations. C266902700013 ADD-RES Least-squares fits to the experimental gamma-ray C266902700014 angular distributions using the computer code GADFIT C266902700015 were made; the even order Legendre polynomial C266902700016 equation was used, the fitting parameters and mixing C266902700017 ratio were defined. C266902700018 ANALYSIS Angular distributions of 56Co gamma rays has been C266902700019 normalized to 1 at 90 degrees. C266902700020 ERR-ANALYS (DATA-ERR) The major uncertainties are in the gamma-rayC266902700021 peak areas and the angle-to-angle normalizations. C266902700022 STATUS (CURVE) Fig.11 (p.2396) in Phys.Rev.C,7,2379,1973 was C266902700023 digitized by GSYS2.4.7. C266902700024 ENDBIB 22 0 C266902700025 COMMON 2 3 C266902700026 EN E C266902700027 MEV KEV C266902700028 7.30 811.9 C266902700029 ENDCOMMON 3 0 C266902700030 DATA 3 10 C266902700031 ANG DATA DATA-ERR C266902700032 ADEG ARB-UNITS ARB-UNITS C266902700033 0.651 0.903 0.011 C266902700034 9.625 0.902 0.015 C266902700035 19.528 0.939 0.016 C266902700036 29.814 0.919 0.013 C266902700037 39.714 0.958 0.012 C266902700038 49.804 0.976 0.016 C266902700039 59.728 0.970 0.009 C266902700040 69.640 0.989 0.015 C266902700041 79.733 0.998 0.009 C266902700042 89.653 1.000 0.012 C266902700043 ENDDATA 12 0 C266902700044 ENDSUBENT 43 0 C266902799999 SUBENT C2669028 20220110 C210C266902800001 BIB 8 22 C266902800002 REACTION (26-FE-56(P,N)27-CO-56,PAR,DA,G,REL) C266902800003 DETECTOR (GELI) A 2.5%-efficient Ge(Li) detector was rigidly C266902800004 mounted on the goniometer arm with the face of C266902800005 the detector 12.7 cm from the target. The detector C266902800006 subtended approximately 10 degrees of arc. C266902800007 (SIBAR) The monitor of proton beam C266902800008 SAMPLE A thin strip of iron foil measuring 1 mm by 10 mm C266902800009 was carefully positioned on the axis of rotation of a C266902800010 high angular precision goniometer. C266902800011 CORRECTION Dead-time and amplifier pileup corrections, and C266902800012 run-to-run normalizations. C266902800013 ADD-RES Least-squares fits to the experimental gamma-ray C266902800014 angular distributions using the computer code GADFIT C266902800015 were made; the even order Legendre polynomial C266902800016 equation was used, the fitting parameters and mixing C266902800017 ratio were defined. C266902800018 ANALYSIS Angular distributions of 56Co gamma rays has been C266902800019 normalized to 1 at 90 degrees. C266902800020 ERR-ANALYS (DATA-ERR) The major uncertainties are in the gamma-rayC266902800021 peak areas and the angle-to-angle normalizations. C266902800022 STATUS (CURVE) Fig.11 (p.2396) in Phys.Rev.C,7,2379,1973 was C266902800023 digitized by GSYS2.4.7. C266902800024 ENDBIB 22 0 C266902800025 COMMON 2 3 C266902800026 EN E C266902800027 MEV KEV C266902800028 7.30 829.8 C266902800029 ENDCOMMON 3 0 C266902800030 DATA 3 10 C266902800031 ANG DATA DATA-ERR C266902800032 ADEG ARB-UNITS ARB-UNITS C266902800033 1.417 1.816 0.042 C266902800034 11.338 1.822 0.058 C266902800035 21.260 1.874 0.044 C266902800036 31.358 1.707 0.040 C266902800037 41.279 1.642 0.054 C266902800038 51.555 1.501 0.046 C266902800039 61.476 1.271 0.042 C266902800040 71.397 1.150 0.038 C266902800041 81.673 0.995 0.026 C266902800042 91.771 1.073 0.042 C266902800043 ENDDATA 12 0 C266902800044 ENDSUBENT 43 0 C266902899999 SUBENT C2669029 20220110 C210C266902900001 BIB 8 22 C266902900002 REACTION (26-FE-56(P,N)27-CO-56,PAR,DA,G,REL) C266902900003 DETECTOR (GELI) A 2.5%-efficient Ge(Li) detector was rigidly C266902900004 mounted on the goniometer arm with the face of C266902900005 the detector 12.7 cm from the target. The detector C266902900006 subtended approximately 10 degrees of arc. C266902900007 (SIBAR) The monitor of proton beam C266902900008 SAMPLE A thin strip of iron foil measuring 1 mm by 10 mm C266902900009 was carefully positioned on the axis of rotation of a C266902900010 high angular precision goniometer. C266902900011 CORRECTION Dead-time and amplifier pileup corrections, and C266902900012 run-to-run normalizations. C266902900013 ADD-RES Least-squares fits to the experimental gamma-ray C266902900014 angular distributions using the computer code GADFIT C266902900015 were made; the even order Legendre polynomial C266902900016 equation was used, the fitting parameters and mixing C266902900017 ratio were defined. C266902900018 ANALYSIS Angular distributions of 56Co gamma rays has been C266902900019 normalized to 1 at 90 degrees. C266902900020 ERR-ANALYS (DATA-ERR) The major uncertainties are in the gamma-rayC266902900021 peak areas and the angle-to-angle normalizations. C266902900022 STATUS (CURVE) Fig.11 (p.2396) in Phys.Rev.C,7,2379,1973 was C266902900023 digitized by GSYS2.4.7. C266902900024 ENDBIB 22 0 C266902900025 COMMON 2 3 C266902900026 EN E C266902900027 MEV KEV C266902900028 7.30 1009.2 C266902900029 ENDCOMMON 3 0 C266902900030 DATA 3 10 C266902900031 ANG DATA DATA-ERR C266902900032 ADEG ARB-UNITS ARB-UNITS C266902900033 0.886 0.825 0.044 C266902900034 11.338 0.963 0.062 C266902900035 21.260 0.991 0.047 C266902900036 31.181 0.949 0.044 C266902900037 41.456 0.938 0.055 C266902900038 51.378 0.992 0.062 C266902900039 61.476 0.959 0.042 C266902900040 71.574 0.956 0.053 C266902900041 81.495 1.035 0.036 C266902900042 91.771 0.991 0.036 C266902900043 ENDDATA 12 0 C266902900044 ENDSUBENT 43 0 C266902999999 SUBENT C2669030 20220110 C210C266903000001 BIB 8 22 C266903000002 REACTION (26-FE-56(P,N)27-CO-56,PAR,DA,G,REL) C266903000003 DETECTOR (GELI) A 2.5%-efficient Ge(Li) detector was rigidly C266903000004 mounted on the goniometer arm with the face of C266903000005 the detector 12.7 cm from the target. The detector C266903000006 subtended approximately 10 degrees of arc. C266903000007 (SIBAR) The monitor of proton beam C266903000008 SAMPLE A thin strip of iron foil measuring 1 mm by 10 mm C266903000009 was carefully positioned on the axis of rotation of a C266903000010 high angular precision goniometer. C266903000011 CORRECTION Dead-time and amplifier pileup corrections, and C266903000012 run-to-run normalizations. C266903000013 ADD-RES Least-squares fits to the experimental gamma-ray C266903000014 angular distributions using the computer code GADFIT C266903000015 were made; the even order Legendre polynomial C266903000016 equation was used, the fitting parameters and mixing C266903000017 ratio were defined. C266903000018 ANALYSIS Angular distributions of 56Co gamma rays has been C266903000019 normalized to 1 at 90 degrees. C266903000020 ERR-ANALYS (DATA-ERR) The major uncertainties are in the gamma-rayC266903000021 peak areas and the angle-to-angle normalizations. C266903000022 STATUS (CURVE) Fig.11 (p.2396) in Phys.Rev.C,7,2379,1973 was C266903000023 digitized by GSYS2.4.7. C266903000024 ENDBIB 22 0 C266903000025 COMMON 2 3 C266903000026 EN E C266903000027 MEV KEV C266903000028 7.30 1114.5 C266903000029 ENDCOMMON 3 0 C266903000030 DATA 3 10 C266903000031 ANG DATA DATA-ERR C266903000032 ADEG ARB-UNITS ARB-UNITS C266903000033 1.063 0.975 0.014 C266903000034 10.984 0.945 0.018 C266903000035 21.083 0.952 0.011 C266903000036 30.827 0.964 0.015 C266903000037 41.102 0.993 0.018 C266903000038 51.023 0.992 0.020 C266903000039 61.299 0.962 0.005 C266903000040 71.220 0.993 0.016 C266903000041 81.318 0.986 0.008 C266903000042 91.239 1.004 0.016 C266903000043 ENDDATA 12 0 C266903000044 ENDSUBENT 43 0 C266903099999 SUBENT C2669031 20220110 C210C266903100001 BIB 8 22 C266903100002 REACTION (26-FE-56(P,N)27-CO-56,PAR,DA,G,REL) C266903100003 DETECTOR (GELI) A 2.5%-efficient Ge(Li) detector was rigidly C266903100004 mounted on the goniometer arm with the face of C266903100005 the detector 12.7 cm from the target. The detector C266903100006 subtended approximately 10 degrees of arc. C266903100007 (SIBAR) The monitor of proton beam C266903100008 SAMPLE A thin strip of iron foil measuring 1 mm by 10 mm C266903100009 was carefully positioned on the axis of rotation of a C266903100010 high angular precision goniometer. C266903100011 CORRECTION Dead-time and amplifier pileup corrections, and C266903100012 run-to-run normalizations. C266903100013 ADD-RES Least-squares fits to the experimental gamma-ray C266903100014 angular distributions using the computer code GADFIT C266903100015 were made; the even order Legendre polynomial C266903100016 equation was used, the fitting parameters and mixing C266903100017 ratio were defined. C266903100018 ANALYSIS Two experimental points were taken at each angle; C266903100019 their weighted average is presented. C266903100020 ERR-ANALYS (DATA-ERR) The major uncertainties are in the gamma-rayC266903100021 peak areas and the angle-to-angle normalizations. C266903100022 STATUS (CURVE) Fig.11 (p.2396) in Phys.Rev.C,7,2379,1973 was C266903100023 digitized by GSYS2.4.7. C266903100024 ENDBIB 22 0 C266903100025 COMMON 1 3 C266903100026 EN C266903100027 MEV C266903100028 7.40 C266903100029 ENDCOMMON 3 0 C266903100030 DATA 4 56 C266903100031 E ANG DATA DATA-ERR C266903100032 KEV ADEG ARB-UNITS ARB-UNITS C266903100033 269.5 0.339 1.008 0.013 C266903100034 269.5 5.310 0.985 0.017 C266903100035 269.5 10.271 0.982 0.016 C266903100036 269.5 15.227 0.994 0.015 C266903100037 269.5 20.532 1.015 0.017 C266903100038 269.5 25.513 0.971 0.019 C266903100039 269.5 30.457 1.008 0.005 C266903100040 269.5 35.605 0.984 0.016 C266903100041 269.5 40.740 0.991 0.012 C266903100042 269.5 45.518 1.002 0.016 C266903100043 269.5 50.661 0.990 0.011 C266903100044 269.5 55.435 1.013 0.015 C266903100045 269.5 60.572 1.013 0.012 C266903100046 269.5 65.723 0.985 0.016 C266903100047 269.5 70.500 0.999 0.015 C266903100048 269.5 75.643 0.988 0.015 C266903100049 269.5 80.425 0.991 0.015 C266903100050 269.5 90.521 0.996 0.019 C266903100051 480.5 0.309 0.950 0.024 C266903100052 480.5 5.120 1.039 0.038 C266903100053 480.5 9.951 0.972 0.031 C266903100054 480.5 14.743 0.960 0.032 C266903100055 480.5 19.865 0.982 0.028 C266903100056 480.5 25.191 0.967 0.028 C266903100057 480.5 29.974 0.967 0.019 C266903100058 480.5 35.093 0.994 0.027 C266903100059 480.5 40.229 0.996 0.027 C266903100060 480.5 45.206 0.973 0.032 C266903100061 480.5 49.833 0.944 0.027 C266903100062 480.5 54.942 0.986 0.030 C266903100063 480.5 60.104 0.951 0.027 C266903100064 480.5 65.022 1.012 0.038 C266903100065 480.5 70.152 1.023 0.038 C266903100066 480.5 75.295 1.015 0.032 C266903100067 480.5 80.281 0.979 0.028 C266903100068 480.5 85.409 0.994 0.031 C266903100069 480.5 90.213 0.964 0.028 C266903100070 750.1 0.600 0.964 0.029 C266903100071 750.1 4.590 1.069 0.033 C266903100072 750.1 9.519 0.946 0.031 C266903100073 750.1 14.643 0.958 0.029 C266903100074 750.1 19.156 1.037 0.028 C266903100075 750.1 24.167 0.994 0.028 C266903100076 750.1 29.629 1.020 0.031 C266903100077 750.1 34.637 0.981 0.027 C266903100078 750.1 39.246 0.978 0.027 C266903100079 750.1 44.578 0.964 0.028 C266903100080 750.1 49.538 0.964 0.027 C266903100081 750.1 54.597 1.031 0.029 C266903100082 750.1 59.435 0.985 0.027 C266903100083 750.1 64.363 1.013 0.032 C266903100084 750.1 69.515 1.001 0.037 C266903100085 750.1 74.520 0.963 0.032 C266903100086 750.1 79.623 0.993 0.028 C266903100087 750.1 84.540 1.030 0.030 C266903100088 750.1 89.551 0.988 0.035 C266903100089 ENDDATA 58 0 C266903100090 ENDSUBENT 89 0 C266903199999 SUBENT C2669032 20220110 C210C266903200001 BIB 7 29 C266903200002 REACTION (26-FE-56(P,N)27-CO-56,PAR,SIG) C266903200003 DETECTOR (GELI) A 2.5%-efficient Ge(Li) detector was positioned C266903200004 with its face 12.7 cm from the center of the target C266903200005 and at 90 degrees to the beam. C266903200006 SAMPLE The 56Fe foil was placed at 55 degrees with respect to C266903200007 the beam direction. The 0.90+/-0.09-mg/cm2 target C266903200008 thickness was determined by measuring the energy loss C266903200009 of 5.48-MeV alpha particles from an 241Am source. The C266903200010 target was placed 15 cm in front of the Faraday cup. C266903200011 CORRECTION Dead-time and amplifier pileup corrections. C266903200012 ANALYSIS The absolute normalization of the counting efficiency C266903200013 curve was determined for the geometry used by counting C266903200014 57Co, 137Cs, 54Mn, and 60Co intensity standards. The C266903200015 precision quoted for the standards was +/-5%. C266903200016 The neutron feeding to each state was determined from C266903200017 the absolute gamma-ray intensities. C266903200018 ERR-ANALYS (DATA-ERR) No information on source of uncertainties C266903200019 presented in the table. C266903200020 (ERR-1) Uncertainty in the target thickness (including C266903200021 nonuniformities). C266903200022 (ERR-2) Uncertainty in the the integrated charge (+5%).C266903200023 (ERR-3) Uncertainty in the absolute normalization for C266903200024 the efficiency curve (including uncertainty in C266903200025 source positioning). C266903200026 (ERR-4,2.,7.) Uncertainty in the gamma-ray peak areas C266903200027 (+/-2 to +/-7%). C266903200028 The total error associated with the measurement is C266903200029 approximately +/-15%. C266903200030 STATUS (TABLE) Tab.VII (p.2400) in Phys.Rev.C,7,2379,1973. C266903200031 ENDBIB 29 0 C266903200032 COMMON 4 3 C266903200033 EN ERR-1 ERR-2 ERR-3 C266903200034 MEV PER-CENT PER-CENT PER-CENT C266903200035 7.30 10. 5. 10. C266903200036 ENDCOMMON 3 0 C266903200037 DATA 4 8 C266903200038 E-EXC E-EXC-ERR DATA DATA-ERR C266903200039 KEV KEV MB MB C266903200040 158.4 0.1 50.7 7.8 C266903200041 576.6 0.1 8.9 1.2 C266903200042 829.7 0.1 18.5 2.6 C266903200043 970.3 0.1 46.9 6.7 C266903200044 1009.2 0.1 6.2 0.9 C266903200045 1114.6 0.1 23.8 3.3 C266903200046 1450.8 0.1 23.9 3.3 C266903200047 1720.3 0.1 14.0 2.0 C266903200048 ENDDATA 10 0 C266903200049 ENDSUBENT 48 0 C266903299999 ENDENTRY 32 0 C266999999999