ENTRY F0833 20130523 F051F083300000001 SUBENT F0833001 20130523 F051F083300100001 BIB 7 20 F083300100002 TITLE Cross sections of proton induced reactions on 61Ni. F083300100003 AUTHOR (C.I.W.Tingwell,V.Y.Hansper,S.G.Tims,A.F.Scott, F083300100004 D.G.Sargood) F083300100005 INSTITUTE (3AULAML) F083300100006 REFERENCE (J,NP/A,480,162,1988) F083300100007 #doi:10.1016/0375-9474(88)90390-9 F083300100008 FACILITY (VDGT,3AULAML) 5U Pelletron accelerator F083300100009 SAMPLE The target was prepared by vacuum evaporation of F083300100010 elemental Ni, enriched to 88.84% in 61Ni, from a F083300100011 previously outgassed tungsten boat, on to an outgassed F083300100012 tantalum backing. The backing was weighed before and F083300100013 after the evaporation to give a measurement of target F083300100014 thickness. Target thickness was determined also from F083300100015 alpha-particle back-scattering measurements at an angleF083300100016 of 145 degr. The adopted thickness value was F083300100017 (7.3+ -0.4)*10**18 atoms of 61Ni cm**(-2). F083300100018 HISTORY (20070618C) F083300100019 (20130523A)SAMPLE in sub 001 was corrected. FACILITY F083300100020 was corrected. Data in sub 004 were redigitized. Data F083300100021 format in sub 002-004 was changed. F083300100022 ENDBIB 20 0 F083300100023 NOCOMMON 0 0 F083300100024 ENDSUBENT 23 0 F083300199999 SUBENT F0833002 20130617 F051F083300200001 BIB 7 19 F083300200002 REACTION (28-NI-61(P,G)29-CU-62,,SIG) F083300200003 DECAY-DATA (29-CU-62,9.73MIN,DG) F083300200004 INC-SOURCE Beam currents were typically 500 nA and charge per F083300200005 point 300 mu-C, corresponding to a bombardment period F083300200006 of approximately 10 min. F083300200007 DETECTOR (GELI) The 125 cm3 (GELI) detector was located 3 cm F083300200008 from the target in the 0 degr. direction. F083300200009 METHOD (ACTIV) F083300200010 (BCINT) F083300200011 ERR-ANALYS (DATA-ERR)The absolute uncertainty in the cross F083300200012 section scale is 10%, the main contributors being F083300200013 detection efficiency 7%, target thickness 5%, and beam F083300200014 current integration 4%. F083300200015 (ERR-S) Error bars reflect statistical uncertainties F083300200016 only. F083300200017 (EN-ERR-DIG) Energy digitizing error F083300200018 (ERR-DIG) Data digitizing error F083300200019 STATUS (CURVE) Fig.2 F083300200020 (COREL,F0833007) Prompt gamma-ray measurement F083300200021 ENDBIB 19 0 F083300200022 COMMON 3 3 F083300200023 DATA-ERR EN-ERR-DIG ERR-DIG F083300200024 PER-CENT MEV PER-CENT F083300200025 10. 0.002 0.007 F083300200026 ENDCOMMON 3 0 F083300200027 DATA 3 33 F083300200028 EN DATA ERR-S F083300200029 MEV MB MB F083300200030 0.995 5.00E-04 2.40E-04 F083300200031 1.093 3.80E-03 F083300200032 1.172 6.80E-03 F083300200033 1.273 1.80E-02 F083300200034 1.356 2.90E-02 F083300200035 1.435 3.40E-02 F083300200036 1.515 6.32E-02 F083300200037 1.587 1.09E-01 F083300200038 1.659 1.25E-01 F083300200039 1.731 1.62E-01 F083300200040 1.803 1.84E-01 F083300200041 1.875 2.33E-01 F083300200042 1.943 2.92E-01 F083300200043 2.016 3.31E-01 F083300200044 2.073 3.31E-01 F083300200045 2.138 4.01E-01 F083300200046 2.196 4.14E-01 F083300200047 2.257 4.34E-01 F083300200048 2.314 4.63E-01 F083300200049 2.379 5.01E-01 F083300200050 2.441 5.17E-01 F083300200051 2.502 5.42E-01 F083300200052 2.563 5.60E-01 F083300200053 2.624 5.97E-01 F083300200054 2.686 7.58E-01 F083300200055 2.743 7.00E-01 F083300200056 2.794 6.67E-01 F083300200057 2.837 6.67E-01 F083300200058 2.880 6.88E-01 F083300200059 2.945 7.82E-01 F083300200060 2.996 7.82E-01 F083300200061 3.042 7.22E-01 F083300200062 3.096 6.77E-01 F083300200063 ENDDATA 35 0 F083300200064 ENDSUBENT 63 0 F083300299999 SUBENT F0833003 20130617 F051F083300300001 BIB 6 23 F083300300002 REACTION (28-NI-61(P,N)29-CU-61,,SIG) F083300300003 DETECTOR (D4PI) F083300300004 (PROPC) The neutron detector consisted of a block of F083300300005 paraffin 32*32*44 cm3 containing six 3He-filled F083300300006 proportional counters running parallel to the incident F083300300007 beam. Two of the proportional counters, of active F083300300008 length 15 cm, were mounted 8 cm from the target in the F083300300009 horizontal plane and the remaining four, of active F083300300010 length 30 cm, were mounted 15 cm from the target in F083300300011 the 45 degr. diagonal planes. F083300300012 METHOD (GSPEC) F083300300013 SAMPLE For the neutron counting measurement, the target was F083300300014 mounted in a stainless steel tubular cross which was F083300300015 located centrally in the neutron detector. F083300300016 ERR-ANALYS (DATA-ERR)The absolute uncertainty in the cross F083300300017 section scale is 11%, the main contributors being 61Cu F083300300018 branching ratios 5%, gamma-ray detection efficiency 5%,F083300300019 neutron detection efficiency 6%, target thickness 5%, F083300300020 and beam current integration 4%. F083300300021 (EN-ERR-DIG) Energy digitizing error F083300300022 (ERR-DIG) Data digitizing error F083300300023 STATUS (CURVE) Fig.3 F083300300024 (COREL,F0833008) Activation measurement F083300300025 ENDBIB 23 0 F083300300026 COMMON 3 3 F083300300027 DATA-ERR EN-ERR-DIG ERR-DIG F083300300028 PER-CENT MEV PER-CENT F083300300029 11. 0.001 0.005 F083300300030 ENDCOMMON 3 0 F083300300031 DATA 2 33 F083300300032 EN DATA F083300300033 MEV MB F083300300034 3.118 7.5624E+00 F083300300035 3.169 1.0421E+01 F083300300036 3.217 1.0420E+01 F083300300037 3.241 1.4617E+01 F083300300038 3.294 1.7157E+01 F083300300039 3.344 1.6704E+01 F083300300040 3.394 1.8587E+01 F083300300041 3.433 1.9959E+01 F083300300042 3.471 1.9781E+01 F083300300043 3.511 1.8918E+01 F083300300044 3.554 1.9429E+01 F083300300045 3.594 2.6773E+01 F083300300046 3.634 2.5834E+01 F083300300047 3.673 4.1052E+01 F083300300048 3.715 3.3445E+01 F083300300049 3.755 3.0867E+01 F083300300050 3.794 4.3298E+01 F083300300051 3.834 3.4962E+01 F083300300052 3.876 4.2152E+01 F083300300053 3.915 4.1405E+01 F083300300054 3.957 3.6224E+01 F083300300055 3.997 3.8898E+01 F083300300056 4.038 4.6068E+01 F083300300057 4.076 5.5049E+01 F083300300058 4.118 6.0174E+01 F083300300059 4.157 5.4071E+01 F083300300060 4.197 5.4551E+01 F083300300061 4.237 5.1251E+01 F083300300062 4.278 5.6524E+01 F083300300063 4.318 5.8571E+01 F083300300064 4.358 6.1783E+01 F083300300065 4.396 6.6936E+01 F083300300066 4.437 7.1876E+01 F083300300067 ENDDATA 35 0 F083300300068 ENDSUBENT 67 0 F083300399999 SUBENT F0833004 20130523 F051F083300400001 BIB 5 16 F083300400002 REACTION (28-NI-61(P,INL)28-NI-61,PAR,SIG) F083300400003 DETECTOR (GELI) Gamma rays were detected by means of a 125cm3 F083300400004 Ge(Li) detector placed 3 cm from the target in the 55 F083300400005 degr. direction for proton energies below the neutron F083300400006 threshold, and a 60 cm3 Ge(Li) detector similarly F083300400007 placed for energies above the neutron threshold. F083300400008 METHOD (GSPEC) F083300400009 ERR-ANALYS (DATA-ERR)The absolute uncertainty in the cross F083300400010 section scale is 10%, the main contributors being F083300400011 detection efficiency 7%, target thickness 5%, and beam F083300400012 current integration 4%. F083300400013 (ERR-S) Error bars reflect statistical uncertainties F083300400014 only. F083300400015 (EN-ERR-DIG) Energy digitizing error F083300400016 (ERR-DIG) Data digitizing error F083300400017 STATUS (CURVE) Fig. 4 F083300400018 ENDBIB 16 0 F083300400019 COMMON 3 3 F083300400020 DATA-ERR EN-ERR-DIG ERR-DIG F083300400021 PER-CENT MEV PER-CENT F083300400022 10. 0.002 0.009 F083300400023 ENDCOMMON 3 0 F083300400024 DATA 4 302 F083300400025 E-LVL EN DATA ERR-S F083300400026 KEV MEV MB MB F083300400027 282.95 1.016 3.066E-04 6.700E-05 F083300400028 282.95 1.114 4.409E-04 8.156E-05 F083300400029 282.95 1.190 1.177E-03 F083300400030 282.95 1.288 1.378E-03 F083300400031 282.95 1.372 1.753E-03 3.152E-04 F083300400032 282.95 1.457 2.629E-03 F083300400033 282.95 1.528 3.489E-03 F083300400034 282.95 1.601 6.984E-03 F083300400035 282.95 1.669 6.403E-03 F083300400036 282.95 1.745 1.574E-02 F083300400037 282.95 1.801 1.926E-02 F083300400038 282.95 1.883 1.915E-02 F083300400039 282.95 1.946 5.330E-02 F083300400040 282.95 2.031 7.673E-02 F083300400041 282.95 2.076 1.417E-01 F083300400042 282.95 2.146 1.596E-01 F083300400043 282.95 2.202 1.952E-01 F083300400044 282.95 2.258 2.112E-01 F083300400045 282.95 2.319 4.786E-01 F083300400046 282.95 2.383 2.909E-01 F083300400047 282.95 2.452 2.895E-01 F083300400048 282.95 2.510 4.175E-01 F083300400049 282.95 2.551 4.520E-01 F083300400050 282.95 2.621 5.302E-01 F083300400051 282.95 2.680 9.013E-01 F083300400052 282.95 2.737 1.197E+00 F083300400053 282.95 2.790 9.711E-01 F083300400054 282.95 2.848 1.400E+00 F083300400055 282.95 2.891 2.022E+00 F083300400056 282.95 2.944 1.574E+00 F083300400057 282.95 2.989 2.570E+00 F083300400058 282.95 3.042 2.084E+00 F083300400059 282.95 3.083 1.837E+00 F083300400060 282.95 3.138 1.907E+00 F083300400061 282.95 3.192 1.900E+00 F083300400062 282.95 3.232 1.675E+00 F083300400063 282.95 3.288 1.739E+00 F083300400064 282.95 3.345 2.507E+00 F083300400065 282.95 3.400 2.602E+00 F083300400066 282.95 3.441 2.491E+00 F083300400067 282.95 3.481 2.287E+00 F083300400068 282.95 3.500 4.234E+00 F083300400069 282.95 3.551 2.796E+00 F083300400070 282.95 3.593 3.027E+00 F083300400071 282.95 3.623 4.028E+00 F083300400072 282.95 3.678 4.182E+00 F083300400073 282.95 3.703 3.261E+00 F083300400074 282.95 3.720 4.527E+00 F083300400075 282.95 3.760 4.158E+00 F083300400076 282.95 3.789 5.311E+00 F083300400077 282.95 3.829 4.681E+00 F083300400078 282.95 3.871 5.280E+00 F083300400079 282.95 3.898 4.659E+00 F083300400080 656.01 1.664 1.540E-03 9.300E-04 F083300400081 656.01 1.739 3.230E-03 1.130E-03 F083300400082 656.01 1.803 4.490E-03 1.260E-03 F083300400083 656.01 1.883 6.360E-03 1.140E-03 F083300400084 656.01 1.947 1.204E-02 F083300400085 656.01 2.017 1.362E-02 F083300400086 656.01 2.081 1.893E-02 F083300400087 656.01 2.145 2.798E-02 F083300400088 656.01 2.204 3.508E-02 F083300400089 656.01 2.263 4.051E-02 F083300400090 656.01 2.321 7.205E-02 F083300400091 656.01 2.391 7.206E-02 F083300400092 656.01 2.450 1.043E-01 F083300400093 656.01 2.514 1.002E-01 F083300400094 656.01 2.572 1.781E-01 F083300400095 656.01 2.642 1.781E-01 F083300400096 656.01 2.690 2.918E-01 F083300400097 656.01 2.760 3.104E-01 F083300400098 656.01 2.808 3.891E-01 F083300400099 656.01 2.856 6.921E-01 F083300400100 656.01 2.957 5.085E-01 F083300400101 656.01 3.006 6.246E-01 F083300400102 656.01 3.059 8.160E-01 F083300400103 656.01 3.107 5.873E-01 F083300400104 656.01 3.155 7.673E-01 F083300400105 656.01 3.209 7.518E-01 F083300400106 656.01 3.257 6.925E-01 F083300400107 656.01 3.305 7.675E-01 F083300400108 656.01 3.353 1.337E+00 F083300400109 656.01 3.412 1.283E+00 F083300400110 656.01 3.449 1.365E+00 F083300400111 656.01 3.476 1.452E+00 F083300400112 656.01 3.519 1.482E+00 F083300400113 656.01 3.562 1.677E+00 F083300400114 656.01 3.604 1.784E+00 F083300400115 656.01 3.647 2.060E+00 F083300400116 656.01 3.690 1.784E+00 F083300400117 656.01 3.727 1.366E+00 F083300400118 656.01 3.770 1.207E+00 F083300400119 656.01 3.808 2.583E+00 F083300400120 656.01 3.850 1.610E+00 F083300400121 656.01 3.888 3.375E+00 F083300400122 656.01 3.931 2.748E+00 F083300400123 908.62 2.014 6.200E-04 5.200E-04 F083300400124 908.62 2.073 2.290E-03 9.500E-04 F083300400125 908.62 2.137 4.780E-03 9.700E-04 F083300400126 908.62 2.196 6.500E-03 1.000E-03 F083300400127 908.62 2.255 7.350E-03 1.490E-03 F083300400128 908.62 2.318 2.310E-02 F083300400129 908.62 2.382 2.358E-02 F083300400130 908.62 2.441 3.014E-02 F083300400131 908.62 2.505 5.235E-02 F083300400132 908.62 2.564 6.165E-02 F083300400133 908.62 2.628 7.411E-02 F083300400134 908.62 2.687 1.369E-01 F083300400135 908.62 2.750 1.899E-01 F083300400136 908.62 2.796 1.579E-01 F083300400137 908.62 2.846 2.528E-01 F083300400138 908.62 2.900 2.688E-01 F083300400139 908.62 2.950 2.688E-01 F083300400140 908.62 2.996 4.964E-01 F083300400141 908.62 3.050 4.669E-01 F083300400142 908.62 3.100 5.066E-01 F083300400143 908.62 3.150 7.173E-01 F083300400144 908.62 3.200 9.358E-01 F083300400145 908.62 3.255 1.080E+00 F083300400146 908.62 3.305 1.380E+00 F083300400147 908.62 3.350 9.948E-01 F083300400148 908.62 3.405 1.298E+00 F083300400149 908.62 3.446 1.659E+00 F083300400150 908.62 3.482 1.875E+00 F083300400151 908.62 3.523 1.693E+00 F083300400152 908.62 3.564 2.035E+00 F083300400153 908.62 3.605 2.766E+00 F083300400154 908.62 3.646 2.710E+00 F083300400155 908.62 3.682 3.836E+00 F083300400156 908.62 3.728 2.348E+00 F083300400157 908.62 3.764 2.497E+00 F083300400158 908.62 3.805 3.393E+00 F083300400159 908.62 3.846 3.126E+00 F083300400160 908.62 3.882 4.337E+00 F083300400161 908.62 3.928 3.534E+00 F083300400162 1015.2 2.077 3.600E-03 1.810E-03 F083300400163 1015.2 2.134 5.000E-03 2.060E-03 F083300400164 1015.2 2.195 1.440E-03 2.170E-03 F083300400165 1015.2 2.260 6.660E-03 2.210E-03 F083300400166 1015.2 2.316 1.111E-02 3.390E-03 F083300400167 1015.2 2.382 1.231E-02 4.130E-03 F083300400168 1015.2 2.438 2.139E-02 2.790E-03 F083300400169 1015.2 2.499 2.096E-02 3.730E-03 F083300400170 1015.2 2.560 2.680E-02 4.770E-03 F083300400171 1015.2 2.621 3.643E-02 4.760E-03 F083300400172 1015.2 2.681 7.928E-02 F083300400173 1015.2 2.742 7.458E-02 F083300400174 1015.2 2.794 7.613E-02 F083300400175 1015.2 2.845 1.219E-01 F083300400176 1015.2 2.892 1.657E-01 F083300400177 1015.2 2.948 2.118E-01 F083300400178 1015.2 3.000 2.395E-01 F083300400179 1015.2 3.051 2.347E-01 F083300400180 1015.2 3.098 3.463E-01 F083300400181 1015.2 3.150 5.108E-01 F083300400182 1015.2 3.201 6.944E-01 F083300400183 1015.2 3.253 6.804E-01 F083300400184 1015.2 3.304 8.350E-01 F083300400185 1015.2 3.356 8.016E-01 F083300400186 1015.2 3.407 1.135E+00 F083300400187 1015.2 3.440 1.159E+00 F083300400188 1015.2 3.482 1.207E+00 F083300400189 1015.2 3.525 1.258E+00 F083300400190 1015.2 3.562 1.394E+00 F083300400191 1015.2 3.604 1.710E+00 F083300400192 1015.2 3.642 2.099E+00 F083300400193 1015.2 3.674 2.523E+00 F083300400194 1015.2 3.721 1.856E+00 F083300400195 1015.2 3.759 2.739E+00 F083300400196 1015.2 3.792 2.796E+00 F083300400197 1015.2 3.834 2.576E+00 F083300400198 1015.2 3.876 2.913E+00 F083300400199 1015.2 3.913 2.684E+00 F083300400200 1099.6 2.263 1.560E-03 1.050E-03 F083300400201 1099.6 2.322 1.130E-03 1.030E-03 F083300400202 1099.6 2.384 4.970E-03 1.500E-03 F083300400203 1099.6 2.443 7.780E-03 1.370E-03 F083300400204 1099.6 2.505 1.057E-02 2.650E-03 F083300400205 1099.6 2.563 2.026E-02 F083300400206 1099.6 2.626 3.045E-02 F083300400207 1099.6 2.689 4.051E-02 F083300400208 1099.6 2.747 5.500E-02 F083300400209 1099.6 2.798 5.504E-02 F083300400210 1099.6 2.849 1.122E-01 F083300400211 1099.6 2.900 1.243E-01 F083300400212 1099.6 2.947 1.322E-01 F083300400213 1099.6 3.001 2.199E-01 F083300400214 1099.6 3.052 2.436E-01 F083300400215 1099.6 3.099 1.949E-01 F083300400216 1099.6 3.150 3.242E-01 F083300400217 1099.6 3.201 3.740E-01 F083300400218 1099.6 3.248 4.875E-01 F083300400219 1099.6 3.303 3.453E-01 F083300400220 1099.6 3.349 7.183E-01 F083300400221 1099.6 3.404 5.748E-01 F083300400222 1099.6 3.439 9.178E-01 F083300400223 1099.6 3.486 8.130E-01 F083300400224 1099.6 3.521 9.570E-01 F083300400225 1099.6 3.565 1.082E+00 F083300400226 1099.6 3.608 1.127E+00 F083300400227 1099.6 3.647 1.199E+00 F083300400228 1099.6 3.686 1.355E+00 F083300400229 1099.6 3.725 1.152E+00 F083300400230 1099.6 3.764 1.502E+00 F083300400231 1099.6 3.807 1.768E+00 F083300400232 1099.6 3.846 2.699E+00 F083300400233 1099.6 3.885 2.083E+00 F083300400234 1099.6 3.929 2.084E+00 F083300400235 1132.3 2.258 3.990E-03 8.600E-04 F083300400236 1132.3 2.318 2.940E-03 1.130E-03 F083300400237 1132.3 2.376 5.210E-03 1.170E-03 F083300400238 1132.3 2.439 9.590E-03 1.470E-03 F083300400239 1132.3 2.498 1.441E-02 1.870E-03 F083300400240 1132.3 2.561 1.804E-02 F083300400241 1132.3 2.620 3.002E-02 F083300400242 1132.3 2.683 4.796E-02 F083300400243 1132.3 2.746 6.252E-02 F083300400244 1132.3 2.797 5.426E-02 F083300400245 1132.3 2.848 1.129E-01 F083300400246 1132.3 2.899 9.999E-02 F083300400247 1132.3 2.946 1.085E-01 F083300400248 1132.3 2.997 1.880E-01 F083300400249 1132.3 3.049 1.445E-01 F083300400250 1132.3 3.100 2.084E-01 F083300400251 1132.3 3.151 2.172E-01 F083300400252 1132.3 3.202 3.199E-01 F083300400253 1132.3 3.249 3.922E-01 F083300400254 1132.3 3.300 6.796E-01 F083300400255 1132.3 3.351 4.813E-01 F083300400256 1132.3 3.403 7.233E-01 F083300400257 1132.3 3.438 9.426E-01 F083300400258 1132.3 3.485 9.625E-01 F083300400259 1132.3 3.521 7.098E-01 F083300400260 1132.3 3.560 1.111E+00 F083300400261 1132.3 3.603 9.639E-01 F083300400262 1132.3 3.643 1.282E+00 F083300400263 1132.3 3.682 1.776E+00 F083300400264 1132.3 3.721 1.364E+00 F083300400265 1132.3 3.765 1.814E+00 F083300400266 1132.3 3.800 2.136E+00 F083300400267 1132.3 3.847 1.970E+00 F083300400268 1132.3 3.883 2.620E+00 F083300400269 1132.3 3.926 2.012E+00 F083300400270 1185.2 2.319 6.800E-04 5.800E-04 F083300400271 1185.2 2.381 8.600E-04 6.500E-04 F083300400272 1185.2 2.439 1.420E-03 6.600E-04 F083300400273 1185.2 2.505 4.180E-03 6.300E-04 F083300400274 1185.2 2.559 9.220E-03 1.220E-03 F083300400275 1185.2 2.625 1.663E-02 F083300400276 1185.2 2.684 3.059E-02 F083300400277 1185.2 2.742 4.067E-02 F083300400278 1185.2 2.796 3.603E-02 F083300400279 1185.2 2.847 5.521E-02 F083300400280 1185.2 2.897 9.556E-02 F083300400281 1185.2 2.944 7.492E-02 F083300400282 1185.2 2.999 1.436E-01 F083300400283 1185.2 3.049 1.436E-01 F083300400284 1185.2 3.100 1.272E-01 F083300400285 1185.2 3.146 1.726E-01 F083300400286 1185.2 3.201 2.073E-01 F083300400287 1185.2 3.248 2.988E-01 F083300400288 1185.2 3.302 3.309E-01 F083300400289 1185.2 3.353 3.590E-01 F083300400290 1185.2 3.403 3.976E-01 F083300400291 1185.2 3.442 5.074E-01 F083300400292 1185.2 3.485 5.734E-01 F083300400293 1185.2 3.528 7.469E-01 F083300400294 1185.2 3.563 5.738E-01 F083300400295 1185.2 3.606 6.101E-01 F083300400296 1185.2 3.644 8.618E-01 F083300400297 1185.2 3.683 1.827E+00 F083300400298 1185.2 3.726 8.115E-01 F083300400299 1185.2 3.765 1.146E+00 F083300400300 1185.2 3.804 1.219E+00 F083300400301 1185.2 3.843 1.244E+00 F083300400302 1185.2 3.886 1.794E+00 F083300400303 1185.2 3.925 1.495E+00 F083300400304 1454.6 2.843 6.420E-03 1.450E-03 F083300400305 1454.6 2.893 1.135E-02 2.980E-03 F083300400306 1454.6 2.940 2.779E-02 2.970E-03 F083300400307 1454.6 2.995 1.574E-02 3.160E-03 F083300400308 1454.6 3.045 1.817E-02 2.780E-03 F083300400309 1454.6 3.095 4.631E-02 6.950E-03 F083300400310 1454.6 3.144 7.549E-02 F083300400311 1454.6 3.197 9.072E-02 F083300400312 1454.6 3.244 1.068E-01 F083300400313 1454.6 3.294 1.450E-01 F083300400314 1454.6 3.352 1.674E-01 F083300400315 1454.6 3.402 1.893E-01 F083300400316 1454.6 3.443 3.556E-01 F083300400317 1454.6 3.482 3.487E-01 F083300400318 1454.6 3.521 3.350E-01 F083300400319 1454.6 3.562 3.154E-01 F083300400320 1454.6 3.601 4.369E-01 F083300400321 1454.6 3.642 4.554E-01 F083300400322 1454.6 3.684 7.575E-01 F083300400323 1454.6 3.723 5.048E-01 F083300400324 1454.6 3.764 7.137E-01 F083300400325 1454.6 3.806 7.906E-01 F083300400326 1454.6 3.842 6.588E-01 F083300400327 1454.6 3.880 8.414E-01 F083300400328 1454.6 3.919 8.592E-01 F083300400329 ENDDATA 304 0 F083300400330 ENDSUBENT 329 0 F083300499999 SUBENT F0833005 20070618 F028F083300500001 BIB 4 11 F083300500002 REACTION (28-NI-61(P,G)29-CU-62,,SGV,,,CALC) F083300500003 COMMENT Thermonuclear reaction rates were calculated from the F083300500004 experimental cross section data by means of the F083300500005 expression of Fowler et al. (Ann. Rev. Astr. and F083300500006 Astrophys. 5, 525, 1967). When cross sections were F083300500007 required for energies outside the experimental range, F083300500008 these were calculated by means of HAUSER*4 using the F083300500009 Sevior parameters and reduced by factors of 1.19 for F083300500010 the (p,g) reaction. F083300500011 ERR-ANALYS (DATA-ERR) Combined errors of the reaction rates. F083300500012 STATUS (TABLE) Tbl.1 F083300500013 ENDBIB 11 0 F083300500014 COMMON 1 3 F083300500015 DATA-ERR F083300500016 PER-CENT F083300500017 10. F083300500018 ENDCOMMON 3 0 F083300500019 DATA 2 21 F083300500020 KT DATA F083300500021 K9 CM3/S/MOL F083300500022 0.5 2.06E-05 F083300500023 0.6 3.29E-04 F083300500024 0.8 1.74E-02 F083300500025 1.0 2.66E-01 F083300500026 1.2 1.95 F083300500027 1.4 8.99 F083300500028 1.5 17.0 F083300500029 1.6 30.2 F083300500030 1.8 81.4 F083300500031 2.0 1.85E+02 F083300500032 2.5 8.74E+02 F083300500033 3.0 2.59E+03 F083300500034 3.5 5.76E+03 F083300500035 4.0 1.05E+04 F083300500036 4.5 1.69E+04 F083300500037 5.0 2.44E+04 F083300500038 6.0 4.13E+04 F083300500039 7.0 5.70E+04 F083300500040 8.0 6.87E+04 F083300500041 9.0 7.45E+04 F083300500042 10.0 7.50E+04 F083300500043 ENDDATA 23 0 F083300500044 ENDSUBENT 43 0 F083300599999 SUBENT F0833006 20070618 F028F083300600001 BIB 4 11 F083300600002 REACTION (28-NI-61(P,N)29-CU-61,,SGV,,,CALC) F083300600003 COMMENT Thermonuclear reaction rates were calculated from the F083300600004 experimental cross section data by means of the F083300600005 expression of Fowler et al. (Ann. Rev. Astr. and F083300600006 Astrophys. 5, 525, 1967). When cross sections were F083300600007 required for energies outside the experimental range, F083300600008 these were calculated by means of HAUSER*4 using the F083300600009 Sevior parameters and reduced by factors of 1.14 for F083300600010 the (p,n) reaction. F083300600011 ERR-ANALYS (DATA-ERR) Combined errors of the reaction rates. F083300600012 STATUS (TABLE) Tbl.1 F083300600013 ENDBIB 11 0 F083300600014 COMMON 1 3 F083300600015 DATA-ERR F083300600016 PER-CENT F083300600017 10. F083300600018 ENDCOMMON 3 0 F083300600019 DATA 2 21 F083300600020 KT DATA F083300600021 K9 CM3/S/MOL F083300600022 0.5 3.65E-23 F083300600023 0.6 4.57E-18 F083300600024 0.8 9.98E-12 F083300600025 1.0 6.32E-08 F083300600026 1.2 2.16E-05 F083300600027 1.4 1.41E-03 F083300600028 1.5 7.49E-03 F083300600029 1.6 3.23E-02 F083300600030 1.8 3.73E-01 F083300600031 2.0 2.64 F083300600032 2.5 91.4 F083300600033 3.0 9.96E+02 F083300600034 3.5 5.62E+03 F083300600035 4.0 2.09E+04 F083300600036 4.5 5.92E+04 F083300600037 5.0 1.37E+05 F083300600038 6.0 4.96E+05 F083300600039 7.0 1.26E+06 F083300600040 8.0 2.54E+06 F083300600041 9.0 4.32E+06 F083300600042 10.0 6.40E+06 F083300600043 ENDDATA 23 0 F083300600044 ENDSUBENT 43 0 F083300699999 SUBENT F0833007 20130617 F051F083300700001 BIB 6 18 F083300700002 REACTION (28-NI-61(P,G)29-CU-62,,SIG) F083300700003 INC-SOURCE Beam currents were typically 200 nA and charge per F083300700004 point 200 mu-C. F083300700005 DETECTOR (GELI) Gamma rays were detected by means of a 125cm3 F083300700006 Ge(Li) detector placed 3 cm from the target in the 55 F083300700007 degr. direction for proton energies below the neutron F083300700008 threshold, and a 60 cm3 Ge(Li) detector similarly F083300700009 placed for energies above the neutron threshold. F083300700010 METHOD (GSPEC) F083300700011 (BCINT) F083300700012 ERR-ANALYS (DATA-ERR)The absolute uncertainty in the cross F083300700013 section scale is 10%, the main contributors being F083300700014 detection efficiency 7%, target thickness 5%, and beam F083300700015 current integration 4%. F083300700016 (EN-ERR-DIG) Energy digitizing error F083300700017 (ERR-DIG) Data digitizing error F083300700018 STATUS (CURVE) Fig.2 F083300700019 (COREL,F0833002) Activation measurement F083300700020 ENDBIB 18 0 F083300700021 COMMON 3 3 F083300700022 DATA-ERR EN-ERR-DIG ERR-DIG F083300700023 PER-CENT MEV PER-CENT F083300700024 10. 0.002 0.007 F083300700025 ENDCOMMON 3 0 F083300700026 DATA 2 51 F083300700027 EN DATA F083300700028 MEV MB F083300700029 0.995 1.40E-03 F083300700030 1.089 4.20E-03 F083300700031 1.187 6.60E-03 F083300700032 1.273 1.66E-02 F083300700033 1.360 2.72E-02 F083300700034 1.432 3.51E-02 F083300700035 1.518 6.22E-02 F083300700036 1.594 1.04E-01 F083300700037 1.662 1.22E-01 F083300700038 1.734 1.49E-01 F083300700039 1.806 1.62E-01 F083300700040 1.875 2.12E-01 F083300700041 1.943 2.92E-01 F083300700042 2.019 2.92E-01 F083300700043 2.077 3.11E-01 F083300700044 2.142 4.01E-01 F083300700045 2.199 4.01E-01 F083300700046 2.261 4.27E-01 F083300700047 2.322 4.20E-01 F083300700048 2.383 4.93E-01 F083300700049 2.444 5.01E-01 F083300700050 2.563 5.60E-01 F083300700051 2.624 5.87E-01 F083300700052 2.686 6.89E-01 F083300700053 2.743 7.00E-01 F083300700054 2.794 6.46E-01 F083300700055 2.895 6.36E-01 F083300700056 2.949 7.57E-01 F083300700057 2.996 7.45E-01 F083300700058 3.046 6.88E-01 F083300700059 3.096 6.77E-01 F083300700060 3.147 6.66E-01 F083300700061 3.197 6.35E-01 F083300700062 3.248 6.25E-01 F083300700063 3.295 6.99E-01 F083300700064 3.345 6.45E-01 F083300700065 3.399 6.25E-01 F083300700066 3.439 7.10E-01 F083300700067 3.475 6.99E-01 F083300700068 3.518 6.45E-01 F083300700069 3.554 6.05E-01 F083300700070 3.594 6.05E-01 F083300700071 3.637 6.15E-01 F083300700072 3.676 5.16E-01 F083300700073 3.720 4.76E-01 F083300700074 3.759 6.35E-01 F083300700075 3.799 5.77E-01 F083300700076 3.838 5.07E-01 F083300700077 3.882 5.41E-01 F083300700078 3.918 4.84E-01 F083300700079 3.961 5.24E-01 F083300700080 ENDDATA 53 0 F083300700081 ENDSUBENT 80 0 F083300799999 SUBENT F0833008 20130617 F051F083300800001 BIB 7 22 F083300800002 REACTION (28-NI-61(P,N)29-CU-61,,SIG) F083300800003 DECAY-DATA (29-CU-61,3.41HR,DG,656.) F083300800004 INC-SOURCE The bombardment periods of approximately 20 min were F083300800005 followed by counting periods of 20 min. F083300800006 DETECTOR (GELI) The activation measurement was carried out F083300800007 simultaneously with the (p,gamma) gamma-ray yield F083300800008 measurement. Gamma rays were detected by means of F083300800009 a 125cm3 Ge(Li) detector placed 3 cm from the target F083300800010 in the 55 degr. direction for proton energies below F083300800011 the neutron threshold, and a 60 cm3 Ge(Li) detector F083300800012 similarly placed for energies above the neutron F083300800013 threshold. F083300800014 METHOD (ACTIV) F083300800015 ERR-ANALYS (DATA-ERR)The absolute uncertainty in the cross F083300800016 section scale is 11%, the main contributors being 61Cu F083300800017 branching ratios 5%, gamma-ray detection efficiency 5%,F083300800018 neutron detection efficiency 6%, target thickness 5%, F083300800019 and beam current integration 4%. F083300800020 (EN-ERR-DIG) Energy digitizing error F083300800021 (ERR-DIG) Data digitizing error F083300800022 STATUS (CURVE)Fig.3 F083300800023 (COREL,F0833003) Outgoing neutron measurement F083300800024 ENDBIB 22 0 F083300800025 COMMON 3 3 F083300800026 DATA-ERR EN-ERR-DIG ERR-DIG F083300800027 PER-CENT MEV PER-CENT F083300800028 11. 0.001 0.005 F083300800029 ENDCOMMON 3 0 F083300800030 DATA 2 38 F083300800031 EN DATA F083300800032 MEV MB F083300800033 3.118 6.9179E+00 F083300800034 3.169 9.7907E+00 F083300800035 3.217 1.0055E+01 F083300800036 3.241 1.4359E+01 F083300800037 3.292 1.5977E+01 F083300800038 3.342 1.7621E+01 F083300800039 3.433 2.1243E+01 F083300800040 3.473 1.9781E+01 F083300800041 3.513 1.8094E+01 F083300800042 3.554 2.0679E+01 F083300800043 3.592 2.5154E+01 F083300800044 3.634 2.7496E+01 F083300800045 3.673 3.9615E+01 F083300800046 3.713 3.5597E+01 F083300800047 3.753 3.2273E+01 F083300800048 3.794 3.7547E+01 F083300800049 3.834 3.4345E+01 F083300800050 3.874 4.3293E+01 F083300800051 3.915 4.1405E+01 F083300800052 3.959 3.6224E+01 F083300800053 3.997 3.8211E+01 F083300800054 4.038 4.6068E+01 F083300800055 4.038 4.6068E+01 F083300800056 4.076 4.9911E+01 F083300800057 4.118 6.0174E+01 F083300800058 4.159 5.4070E+01 F083300800059 4.197 5.4551E+01 F083300800060 4.239 5.3110E+01 F083300800061 4.278 5.8574E+01 F083300800062 4.318 5.8571E+01 F083300800063 4.358 6.1783E+01 F083300800064 4.396 6.6936E+01 F083300800065 4.439 7.0607E+01 F083300800066 4.477 7.5817E+01 F083300800067 4.517 7.3814E+01 F083300800068 4.558 7.9262E+01 F083300800069 4.598 8.5111E+01 F083300800070 4.638 9.3035E+01 F083300800071 ENDDATA 40 0 F083300800072 ENDSUBENT 71 0 F083300899999 ENDENTRY 8 0 F083399999999