ENTRY C2597 20210223 C201C259700000001 SUBENT C2597001 20210223 C201C259700100001 BIB 9 29 C259700100002 TITLE Test of nuclear level density inputs for C259700100003 Hauser-Feshbach model calculations C259700100004 AUTHOR (A.V.Voinov,S.M.Grimes,C.R.Brune,M.J.Hornish, C259700100005 T.N.Massey, A.Salas) C259700100006 REFERENCE (J,PR/C,76,044602,2007) C259700100007 #doi:10.1103/PhysRevC.76.044602 C259700100008 INSTITUTE (1USAOHO,1USALAS) C259700100009 FACILITY (VDGT,1USAOHO) The tandem accelerator at Ohio C259700100010 University's Edwards Accelerator Laboratory. C259700100011 DETECTOR (SI) C259700100012 METHOD (TOF,EDE) The outgoing charged particles were C259700100013 registered by charged particle spectrometer. The C259700100014 setup has ten 2-m time-of-flight legs ending with Si C259700100015 detectors. Legs are set up at different angles C259700100016 ranging from 22.5 up to 157.5 degrees, however we C259700100017 used nine angles for 3He+58Fe and two backward angles C259700100018 for d+59Co reactions due to some electronics and C259700100019 detector problems. The mass of the charged particles C259700100020 is determined by measuring both the energy deposited C259700100021 in Si detectors and the time of flight. Additionally, C259700100022 a neutron detector was placed at the distance of 140 C259700100023 cm from the target to measure the neutron energy C259700100024 spectrum. The mass resolution was sufficient to C259700100025 resolve protons, deuterons, 3H/3He, and C259700100026 alpha-particles. Additional measurements with a blank C259700100027 target have been performed at each angle to determine C259700100028 background contribution. C259700100029 STATUS (APRVD) Approved by A.Voinov, 3/10/2021. C259700100030 HISTORY (20210223C) BP C259700100031 ENDBIB 29 0 C259700100032 NOCOMMON 0 0 C259700100033 ENDSUBENT 32 0 C259700199999 SUBENT C2597002 20210223 C201C259700200001 BIB 5 15 C259700200002 REACTION (26-FE-58(HE3,X)1-H-1,,DA) C259700200003 SAMPLE (26-FE-58,ENR=0.82) Self-supporting foils of 0.625- C259700200004 mg/cm2 58Fe (82% enriched) have been used as targets. C259700200005 ANALYSIS The absolute cross section has been calculated by C259700200006 taking into account the target thickness, the C259700200007 accumulated charge of incoming deuteron or 3He beam, C259700200008 and the neutron detector efficiency. C259700200009 ERR-ANALYS (DATA-ERR) Experimental errors. C259700200010 (ERR-SYS) The overall systematic error for the C259700200011 absolute cross sections is estimated to be 15%. The C259700200012 errors in ratios of proton and alpha cross sections C259700200013 are only a few percents because they are determined C259700200014 by counting statistics alone. C259700200015 STATUS (TABLE) Data were received from A.Voinov on 3/10/2021. C259700200016 Also shown in Fig. 2, page 044602-4. C259700200017 ENDBIB 15 0 C259700200018 COMMON 2 3 C259700200019 EN ERR-SYS C259700200020 MEV PER-CENT C259700200021 10.0 15.0 C259700200022 ENDCOMMON 3 0 C259700200023 DATA 3 10 C259700200024 ANG DATA DATA-ERR C259700200025 ADEG MB/SR MB/SR C259700200026 22.5 3.15868 0.31587 C259700200027 37.5 3.1486 0.31486 C259700200028 52.5 3.16628 0.31663 C259700200029 67.5 2.73217 0.27322 C259700200030 82.5 2.50367 0.25037 C259700200031 97.5 2.73393 0.27339 C259700200032 112.5 2.36844 0.23684 C259700200033 127.5 2.39904 0.2399 C259700200034 142.5 2.15478 0.21548 C259700200035 157.5 2.42975 0.24298 C259700200036 ENDDATA 12 0 C259700200037 ENDSUBENT 36 0 C259700299999 SUBENT C2597003 20210223 C201C259700300001 BIB 5 15 C259700300002 REACTION (26-FE-58(HE3,X)2-HE-4,,DA) C259700300003 SAMPLE (26-FE-58,ENR=0.82) Self-supporting foils of 0.625- C259700300004 mg/cm2 58Fe (82% enriched) have been used as targets. C259700300005 ANALYSIS The absolute cross section has been calculated by C259700300006 taking into account the target thickness, the C259700300007 accumulated charge of incoming deuteron or 3He beam, C259700300008 and the neutron detector efficiency. C259700300009 ERR-ANALYS (DATA-ERR) Experimental errors. C259700300010 (ERR-SYS) The overall systematic error for the C259700300011 absolute cross sections is estimated to be 15%. The C259700300012 errors in ratios of proton and alpha cross sections C259700300013 are only a few percents because they are determined C259700300014 by counting statistics alone. C259700300015 STATUS (TABLE) Data were received from A.Voinov on 3/10/2021. C259700300016 Also shown in Fig. 2, page 044602-4. C259700300017 ENDBIB 15 0 C259700300018 COMMON 2 3 C259700300019 EN ERR-SYS C259700300020 MEV PER-CENT C259700300021 10.0 15.0 C259700300022 ENDCOMMON 3 0 C259700300023 DATA 3 10 C259700300024 ANG DATA DATA-ERR C259700300025 ADEG MB/SR MB/SR C259700300026 22.5 26.433 2.6433 C259700300027 37.5 1.13209 0.11321 C259700300028 52.5 0.854 0.0854 C259700300029 67.5 0.73547 0.07355 C259700300030 82.5 0.58945 0.05895 C259700300031 97.5 0.51947 0.05195 C259700300032 112.5 0.45345 0.04535 C259700300033 127.5 0.42557 0.04256 C259700300034 142.5 0.401 0.0401 C259700300035 157.5 0.44018 0.04402 C259700300036 ENDDATA 12 0 C259700300037 ENDSUBENT 36 0 C259700399999 SUBENT C2597004 20210223 C201C259700400001 BIB 5 23 C259700400002 REACTION (26-FE-58(HE3,X)0-NN-1,,IPA/DE) C259700400003 SAMPLE (26-FE-58,ENR=0.82) Self-supporting foils of 0.625- C259700400004 mg/cm2 58Fe (82% enriched) have been used as targets. C259700400005 ANALYSIS The absolute cross section has been calculated by C259700400006 taking into account the target thickness, the C259700400007 accumulated charge of incoming deuteron or 3He beam, C259700400008 and the neutron detector efficiency. In order to C259700400009 eliminate contributions from the direct reaction C259700400010 mechanism, energy spectra of neutron, protons, and C259700400011 a-particles measured at backward angles (from 112 to C259700400012 157) have been used for analysis. However, units for C259700400013 cross sections are mb/MeV in Fig.3. This is because C259700400014 cross sections were determined for each angle in the C259700400015 units of mb/MeV/Sr and then multiplied by 4pi to be C259700400016 able to compare them with Empire calculations. C259700400017 ERR-ANALYS (DATA-ERR) Experimental errors. C259700400018 (ERR-SYS) The overall systematic error for the C259700400019 absolute cross sections is estimated to be 15%. The C259700400020 errors in ratios of proton and alpha cross sections C259700400021 are only a few percents because they are determined C259700400022 by counting statistics alone. C259700400023 STATUS (TABLE) Data were received from A.Voinov on 3/10/2021. C259700400024 Also shown in Fig. 3, page 044602-5. C259700400025 ENDBIB 23 0 C259700400026 COMMON 4 3 C259700400027 EN ANG-MIN ANG-MAX ERR-SYS C259700400028 MEV ADEG ADEG PER-CENT C259700400029 10.0 112.0 157.0 15.0 C259700400030 ENDCOMMON 3 0 C259700400031 DATA 3 51 C259700400032 E DATA DATA-ERR C259700400033 MEV MB/MEV MB/MEV C259700400034 0.15 0. 0. C259700400035 0.4500001 0. 0. C259700400036 0.7500002 0. 0. C259700400037 1.05 117.515488 2.689479 C259700400038 1.35 153.124222 3.662468 C259700400039 1.65 140.123459 3.474778 C259700400040 1.950001 116.877396 3.134465 C259700400041 2.25 106.031464 3.148027 C259700400042 2.550001 86.145836 2.811692 C259700400043 2.850001 68.490219 2.467148 C259700400044 3.150001 56.614552 2.257063 C259700400045 3.450001 50.156883 2.144435 C259700400046 3.750001 39.68615 1.826735 C259700400047 4.050001 33.384232 1.736184 C259700400048 4.350001 28.397598 1.602236 C259700400049 4.650001 23.566803 1.410077 C259700400050 4.950001 18.684797 1.278307 C259700400051 5.250001 15.80604 1.222847 C259700400052 5.550001 13.411947 1.115531 C259700400053 5.850001 11.093067 1.012475 C259700400054 6.150002 9.052382 0.9369332 C259700400055 6.450002 8.434997 0.9666272 C259700400056 6.750001 6.106469 0.8436646 C259700400057 7.050002 4.743482 0.7289046 C259700400058 7.350002 4.170984 0.7333307 C259700400059 7.650002 3.622208 0.619063 C259700400060 7.950002 3.586514 0.5512128 C259700400061 8.250002 3.299389 0.5281762 C259700400062 8.550002 2.306469 0.4360668 C259700400063 8.850002 1.562463 0.361787 C259700400064 9.150002 1.461354 0.3769994 C259700400065 9.450003 1.33451 0.3559858 C259700400066 9.750002 1.23466 0.3585824 C259700400067 10.050002 0.7255287 0.2444651 C259700400068 10.350002 0.6793882 0.2440856 C259700400069 10.650002 0.5681934 0.2259024 C259700400070 10.950003 0.4276573 0.1961099 C259700400071 11.250003 0.3002842 0.1696971 C259700400072 11.550003 0.3774766 0.1988557 C259700400073 11.850003 0.3997791 0.1960095 C259700400074 12.150002 0.1207435 0.1604534 C259700400075 12.450003 0.298549 0.1714204 C259700400076 12.750003 0.0161602 0.1219469 C259700400077 13.050003 0.1598815 0.1185431 C259700400078 13.350003 0.3984251 0.2378337 C259700400079 13.650003 0.0399134 0.1446144 C259700400080 13.950004 0.1529546 0.1816176 C259700400081 14.250004 0.0388022 0.1792709 C259700400082 14.550003 0.37303 0.5035647 C259700400083 14.850003 0.1383731 0. C259700400084 15.150003 0.3156563 0. C259700400085 ENDDATA 53 0 C259700400086 ENDSUBENT 85 0 C259700499999 SUBENT C2597005 20210223 C201C259700500001 BIB 5 23 C259700500002 REACTION (26-FE-58(HE3,X)1-H-1,,IPA/DE) C259700500003 SAMPLE (26-FE-58,ENR=0.82) Self-supporting foils of 0.625- C259700500004 mg/cm2 58Fe (82% enriched) have been used as targets. C259700500005 ANALYSIS The absolute cross section has been calculated by C259700500006 taking into account the target thickness, the C259700500007 accumulated charge of incoming deuteron or 3He beam, C259700500008 and the neutron detector efficiency. In order to C259700500009 eliminate contributions from the direct reaction C259700500010 mechanism, energy spectra of neutron, protons, and C259700500011 a-particles measured at backward angles (from 112 to C259700500012 157) have been used for analysis. However, units for C259700500013 cross sections are mb/MeV in Fig.3. This is because C259700500014 cross sections were determined for each angle in the C259700500015 units of mb/MeV/Sr and then multiplied by 4pi to be C259700500016 able to compare them with Empire calculations. C259700500017 ERR-ANALYS (DATA-ERR) Experimental errors. C259700500018 (ERR-SYS) The overall systematic error for the C259700500019 absolute cross sections is estimated to be 15%. The C259700500020 errors in ratios of proton and alpha cross sections C259700500021 are only a few percents because they are determined C259700500022 by counting statistics alone. C259700500023 STATUS (TABLE) Data were received from A.Voinov on 3/10/2021. C259700500024 Also shown in Fig. 3, page 044602-5. C259700500025 ENDBIB 23 0 C259700500026 COMMON 4 3 C259700500027 EN ANG-MIN ANG-MAX ERR-SYS C259700500028 MEV ADEG ADEG PER-CENT C259700500029 10.0 112.0 157.0 15.0 C259700500030 ENDCOMMON 3 0 C259700500031 DATA 3 55 C259700500032 E DATA DATA-ERR C259700500033 MEV MB/MEV MB/MEV C259700500034 2.21 18.453953 0.8966888 C259700500035 2.47 19.970215 0.9708382 C259700500036 2.73 22.948668 0.9121273 C259700500037 2.99 23.206722 0.7350221 C259700500038 3.25 33.13546 0.9513955 C259700500039 3.51 29.211325 0.8145032 C259700500040 3.77 33.607723 0.9375511 C259700500041 4.03 33.635719 0.9029433 C259700500042 4.29 36.929573 0.9736239 C259700500043 4.55 32.855534 0.9067284 C259700500044 4.81 37.017773 1.05503 C259700500045 5.07 31.15724 0.9160135 C259700500046 5.33 31.299002 0.9819385 C259700500047 5.59 23.922396 0.7961484 C259700500048 5.85 23.943563 0.887102 C259700500049 6.11 19.20332 0.6755987 C259700500050 6.37 17.580574 0.6687387 C259700500051 6.63 14.827006 0.6304092 C259700500052 6.89 14.729783 0.6775083 C259700500053 7.15 12.081 0.5362808 C259700500054 7.41 12.019324 0.5598163 C259700500055 7.67 10.913574 0.5442561 C259700500056 7.93 10.386634 0.6283754 C259700500057 8.19 7.788784 0.5463189 C259700500058 8.45 8.016965 0.6190801 C259700500059 8.71 6.365582 0.5355366 C259700500060 8.969999 5.754635 0.3948781 C259700500061 9.23 4.237252 0.3136481 C259700500062 9.49 3.851019 0.3075298 C259700500063 9.75 3.445246 0.288054 C259700500064 10.009999 4.13245 0.5991354 C259700500065 10.27 3.231521 0.5031934 C259700500066 10.53 2.405132 0.2434275 C259700500067 10.79 2.0136 0.2197736 C259700500068 11.049999 2.314898 0.2404648 C259700500069 11.309999 1.830085 0.2038816 C259700500070 11.57 1.396019 0.1884505 C259700500071 11.83 1.128593 0.1660708 C259700500072 12.089999 1.119463 0.1662568 C259700500073 12.349999 0.7777958 0.1288884 C259700500074 12.61 0.6864255 0.1292215 C259700500075 12.87 0.4136392 0.0985065 C259700500076 13.129999 0.3649153 0.0986428 C259700500077 13.389999 0.371847 0.0929186 C259700500078 13.65 0.3871034 0.0996671 C259700500079 13.91 0.2823246 0.084854 C259700500080 14.169999 0.2439967 0.0802863 C259700500081 14.429999 0.1767882 0.0640451 C259700500082 14.69 0.1601788 0.0662645 C259700500083 14.95 0.1184569 0.0530501 C259700500084 15.209999 0.0439345 0.0292078 C259700500085 15.469999 0.1553459 0.0628242 C259700500086 15.73 0.081402 0.0411481 C259700500087 15.99 0.0246776 0.0217984 C259700500088 16.25 0.0033791 0.0033791 C259700500089 ENDDATA 57 0 C259700500090 ENDSUBENT 89 0 C259700599999 SUBENT C2597006 20210223 C201C259700600001 BIB 5 23 C259700600002 REACTION (26-FE-58(HE3,X)2-HE-4,,IPA/DE) C259700600003 SAMPLE (26-FE-58,ENR=0.82) Self-supporting foils of 0.625- C259700600004 mg/cm2 58Fe (82% enriched) have been used as targets. C259700600005 ANALYSIS The absolute cross section has been calculated by C259700600006 taking into account the target thickness, the C259700600007 accumulated charge of incoming deuteron or 3He beam, C259700600008 and the neutron detector efficiency. In order to C259700600009 eliminate contributions from the direct reaction C259700600010 mechanism, energy spectra of neutron, protons, and C259700600011 a-particles measured at backward angles (from 112 to C259700600012 157) have been used for analysis. However, units for C259700600013 cross sections are mb/MeV in Fig.3. This is because C259700600014 cross sections were determined for each angle in the C259700600015 units of mb/MeV/Sr and then multiplied by 4pi to be C259700600016 able to compare them with Empire calculations. C259700600017 ERR-ANALYS (DATA-ERR) Experimental errors. C259700600018 (ERR-SYS) The overall systematic error for the C259700600019 absolute cross sections is estimated to be 15%. The C259700600020 errors in ratios of proton and alpha cross sections C259700600021 are only a few percents because they are determined C259700600022 by counting statistics alone. C259700600023 STATUS (TABLE) Data were received from A.Voinov on 3/10/2021. C259700600024 Also shown in Fig. 3, page 044602-5. C259700600025 ENDBIB 23 0 C259700600026 COMMON 4 3 C259700600027 EN ANG-MIN ANG-MAX ERR-SYS C259700600028 MEV ADEG ADEG PER-CENT C259700600029 10.0 112.0 157.0 15.0 C259700600030 ENDCOMMON 3 0 C259700600031 DATA 3 55 C259700600032 E DATA DATA-ERR C259700600033 MEV MB/MEV MB/MEV C259700600034 4.03 2.525824 0.2196291 C259700600035 4.55 0.0583775 0. C259700600036 5.07 0.6729056 0.0915914 C259700600037 5.33 0.5318254 0.1054881 C259700600038 5.59 0.6244931 0.1074971 C259700600039 5.85 0.8457088 0.1349331 C259700600040 6.11 1.582704 0.1745267 C259700600041 6.37 1.963166 0.2075349 C259700600042 6.63 2.039046 0.2023 C259700600043 6.89 2.977702 0.2592382 C259700600044 7.15 3.33506 0.2651489 C259700600045 7.41 3.812804 0.29202 C259700600046 7.67 3.945025 0.2878908 C259700600047 7.93 4.422353 0.3116974 C259700600048 8.19 3.740613 0.2699349 C259700600049 8.45 3.891169 0.2894223 C259700600050 8.71 3.973962 0.2873103 C259700600051 8.969999 4.596994 0.3237986 C259700600052 9.23 3.55262 0.2671106 C259700600053 9.49 2.986223 0.2469354 C259700600054 9.75 2.604727 0.22644 C259700600055 10.009999 2.689375 0.2483118 C259700600056 10.27 2.216258 0.2157936 C259700600057 10.53 2.125093 0.2156657 C259700600058 10.79 1.721303 0.1822289 C259700600059 11.049999 1.400397 0.1658232 C259700600060 11.309999 1.221173 0.1562369 C259700600061 11.57 1.20828 0.1657868 C259700600062 11.83 1.108511 0.1543584 C259700600063 12.089999 1.068061 0.1558809 C259700600064 12.349999 0.7308353 0.1249149 C259700600065 12.61 0.5567896 0.1113695 C259700600066 12.87 0.6193483 0.1099422 C259700600067 13.129999 0.68681 0.1170884 C259700600068 13.389999 0.5252429 0.0971435 C259700600069 13.65 0.4792295 0.0908058 C259700600070 13.91 0.6177962 0.1091642 C259700600071 14.169999 0.2756953 0.0725563 C259700600072 14.429999 0.1693214 0.0550313 C259700600073 14.69 0.1569108 0.0537977 C259700600074 14.95 0.0771672 0.0272501 C259700600075 15.209999 0.1272122 0.0564772 C259700600076 15.469999 0.1548534 0.0611258 C259700600077 15.73 0.0694205 0.0324865 C259700600078 15.99 0.0742609 0.0379993 C259700600079 16.25 0.1664479 0.0633801 C259700600080 16.51 0.2105773 0.0671936 C259700600081 16.769999 0.1545418 0.0490404 C259700600082 17.029999 0.0419049 0.0314286 C259700600083 17.289999 0.0785103 0.0394973 C259700600084 17.549999 0.127337 0.0471069 C259700600085 17.809999 0.0425751 0.0275974 C259700600086 18.07 0.0416791 0.0171557 C259700600087 18.33 0.1109705 0.04921 C259700600088 18.59 0.1075444 0.0384087 C259700600089 ENDDATA 57 0 C259700600090 ENDSUBENT 89 0 C259700699999 SUBENT C2597007 20210223 C201C259700700001 BIB 5 23 C259700700002 REACTION (27-CO-59(D,X)0-NN-1,,IPA/DE) C259700700003 SAMPLE Self-supporting 0.89-mg/cm2 59Co (100% natural C259700700004 abundance) have been used as targets. C259700700005 ANALYSIS The absolute cross section has been calculated by C259700700006 taking into account the target thickness, the C259700700007 accumulated charge of incoming deuteron or 3He beam, C259700700008 and the neutron detector efficiency. In order to C259700700009 eliminate contributions from the direct reaction C259700700010 mechanism, energy spectra of neutron, protons, and C259700700011 a-particles measured at backward angles (from 112 to C259700700012 157) have been used for analysis. However, units for C259700700013 cross sections are mb/MeV in Fig.3. This is because C259700700014 cross sections were determined for each angle in the C259700700015 units of mb/MeV/Sr and then multiplied by 4pi to be C259700700016 able to compare them with Empire calculations. C259700700017 ERR-ANALYS (DATA-ERR) Experimental errors. C259700700018 (ERR-SYS) The overall systematic error for the C259700700019 absolute cross sections is estimated to be 15%. The C259700700020 errors in ratios of proton and alpha cross sections C259700700021 are only a few percents because they are determined C259700700022 by counting statistics alone. C259700700023 STATUS (TABLE) Data were received from A.Voinov on 3/10/2021. C259700700024 Also shown in Fig. 3, page 044602-5. C259700700025 ENDBIB 23 0 C259700700026 COMMON 4 3 C259700700027 EN ANG-MIN ANG-MAX ERR-SYS C259700700028 MEV ADEG ADEG PER-CENT C259700700029 7.5 112.0 157.0 15.0 C259700700030 ENDCOMMON 3 0 C259700700031 DATA 3 45 C259700700032 E DATA DATA-ERR C259700700033 MEV MB/MEV MB/MEV C259700700034 1.2 172.748016 7.620176 C259700700035 1.5 183.154526 8.026578 C259700700036 1.8 171.335236 7.690265 C259700700037 2.1 148.645096 6.917583 C259700700038 2.400001 130.349625 6.320518 C259700700039 2.700001 110.699753 5.583383 C259700700040 3.000001 91.239548 4.778923 C259700700041 3.300001 79.188148 4.296862 C259700700042 3.600001 70.963646 3.969284 C259700700043 3.900001 62.179108 3.587873 C259700700044 4.200001 53.762516 3.185788 C259700700045 4.500001 48.301472 2.927994 C259700700046 4.800001 41.332397 2.562057 C259700700047 5.100001 34.99976 2.214763 C259700700048 5.400002 27.581926 1.780814 C259700700049 5.700001 21.498518 1.418186 C259700700050 6.000001 19.457741 1.310355 C259700700051 6.300002 16.585154 1.138457 C259700700052 6.600001 13.796175 0.9703183 C259700700053 6.900002 11.318461 0.8196205 C259700700054 7.200002 9.1474 0.6904847 C259700700055 7.500002 9.13519 0.7161153 C259700700056 7.800002 7.930268 0.6451817 C259700700057 8.100002 5.61691 0.4897822 C259700700058 8.400002 4.909454 0.457276 C259700700059 8.700002 3.959155 0.3942129 C259700700060 9.000002 4.076945 0.4220163 C259700700061 9.300002 3.710324 0.3975401 C259700700062 9.600002 2.644058 0.3034171 C259700700063 9.900002 2.141086 0.2598435 C259700700064 10.200003 1.620463 0.2093874 C259700700065 10.500003 1.647725 0.2248051 C259700700066 10.800003 1.544705 0.2183185 C259700700067 11.100002 0.7835662 0.129291 C259700700068 11.400002 0.4267159 0.0806609 C259700700069 11.700003 0.3224064 0.0733024 C259700700070 12.000003 0.2246609 0.0521247 C259700700071 12.300003 0.1432334 0.0349204 C259700700072 12.600003 0.1432028 0.037613 C259700700073 12.900003 0.1887356 0.0502344 C259700700074 13.200003 0.1480327 0.048007 C259700700075 13.500003 0.1024659 0.0423294 C259700700076 13.800003 0.1008203 0.0567599 C259700700077 14.100003 0.1707183 0.1241981 C259700700078 14.400003 0.0861598 0.1385853 C259700700079 ENDDATA 47 0 C259700700080 ENDSUBENT 79 0 C259700799999 SUBENT C2597008 20210223 C201C259700800001 BIB 5 23 C259700800002 REACTION (27-CO-59(D,X)1-H-1,,IPA/DE) C259700800003 SAMPLE Self-supporting 0.89-mg/cm2 59Co (100% natural C259700800004 abundance) have been used as targets. C259700800005 ANALYSIS The absolute cross section has been calculated by C259700800006 taking into account the target thickness, the C259700800007 accumulated charge of incoming deuteron or 3He beam, C259700800008 and the neutron detector efficiency. In order to C259700800009 eliminate contributions from the direct reaction C259700800010 mechanism, energy spectra of neutron, protons, and C259700800011 a-particles measured at backward angles (from 112 to C259700800012 157) have been used for analysis. However, units for C259700800013 cross sections are mb/MeV in Fig.3. This is because C259700800014 cross sections were determined for each angle in the C259700800015 units of mb/MeV/Sr and then multiplied by 4pi to be C259700800016 able to compare them with Empire calculations. C259700800017 ERR-ANALYS (DATA-ERR) Experimental errors. C259700800018 (ERR-SYS) The overall systematic error for the C259700800019 absolute cross sections is estimated to be 15%. The C259700800020 errors in ratios of proton and alpha cross sections C259700800021 are only a few percents because they are determined C259700800022 by counting statistics alone. C259700800023 STATUS (TABLE) Data were received from A.Voinov on 3/10/2021. C259700800024 Also shown in Fig. 3, page 044602-5. C259700800025 ENDBIB 23 0 C259700800026 COMMON 4 3 C259700800027 EN ANG-MIN ANG-MAX ERR-SYS C259700800028 MEV ADEG ADEG PER-CENT C259700800029 7.5 112.0 157.0 15.0 C259700800030 ENDCOMMON 3 0 C259700800031 DATA 3 41 C259700800032 E DATA DATA-ERR C259700800033 MEV MB/MEV MB/MEV C259700800034 1.95 21.415192 0.5936955 C259700800035 2.21 48.983101 1.094668 C259700800036 2.47 53.471394 1.217829 C259700800037 2.73 56.875423 1.202426 C259700800038 2.99 53.436466 1.111214 C259700800039 3.25 55.488384 1.204643 C259700800040 3.51 45.388878 0.9764884 C259700800041 3.77 54.91806 1.263433 C259700800042 4.0317259 49.0909247 1.432071 C259700800043 4.29 43.299667 1.227671 C259700800044 4.55 49.065754 1.197397 C259700800045 4.81 46.875347 1.08825 C259700800046 5.07 41.624794 0.9511309 C259700800047 5.33 40.480911 0.9541339 C259700800048 5.59 35.09502 0.8443858 C259700800049 5.85 36.927284 0.9254855 C259700800050 6.11 30.45463 0.8040571 C259700800051 6.37 32.833443 0.992488 C259700800052 6.63 28.628397 0.7935055 C259700800053 6.89 26.680254 0.78015 C259700800054 7.15 21.903679 0.9420753 C259700800055 7.41 19.922165 0.8485811 C259700800056 7.67 15.81128 0.591001 C259700800057 7.93 16.09017 0.5932803 C259700800058 8.19 10.572981 0.4869775 C259700800059 8.45 9.431784 0.4551346 C259700800060 8.71 8.484606 0.4320896 C259700800061 8.969999 9.243107 0.4403249 C259700800062 9.23 7.358774 0.4101161 C259700800063 9.49 5.86327 0.3435302 C259700800064 9.75 3.09488 0.2654788 C259700800065 10.009999 4.051551 0.2908975 C259700800066 10.27 4.778851 0.3322496 C259700800067 10.53 4.622792 0.3103417 C259700800068 10.79 2.906978 0.2588292 C259700800069 11.049999 2.817345 0.2431936 C259700800070 11.309999 4.165071 0.3054864 C259700800071 11.57 4.491967 0.3091649 C259700800072 11.83 4.655212 0.3257214 C259700800073 12.089999 3.775267 0.2776548 C259700800074 12.349999 4.382596 0.2548021 C259700800075 ENDDATA 43 0 C259700800076 ENDSUBENT 75 0 C259700899999 SUBENT C2597009 20210223 C201C259700900001 BIB 5 23 C259700900002 REACTION (27-CO-59(D,X)2-HE-4,,IPA/DE) C259700900003 SAMPLE Self-supporting 0.89-mg/cm2 59Co (100% natural C259700900004 abundance) have been used as targets. C259700900005 ANALYSIS The absolute cross section has been calculated by C259700900006 taking into account the target thickness, the C259700900007 accumulated charge of incoming deuteron or 3He beam, C259700900008 and the neutron detector efficiency. In order to C259700900009 eliminate contributions from the direct reaction C259700900010 mechanism, energy spectra of neutron, protons, and C259700900011 a-particles measured at backward angles (from 112 to C259700900012 157) have been used for analysis. However, units for C259700900013 cross sections are mb/MeV in Fig.3. This is because C259700900014 cross sections were determined for each angle in the C259700900015 units of mb/MeV/Sr and then multiplied by 4pi to be C259700900016 able to compare them with Empire calculations. C259700900017 ERR-ANALYS (DATA-ERR) Experimental errors. C259700900018 (ERR-SYS) The overall systematic error for the C259700900019 absolute cross sections is estimated to be 15%. The C259700900020 errors in ratios of proton and alpha cross sections C259700900021 are only a few percents because they are determined C259700900022 by counting statistics alone. C259700900023 STATUS (TABLE) Data were received from A.Voinov on 3/10/2021. C259700900024 Also shown in Fig. 3, page 044602-5. C259700900025 ENDBIB 23 0 C259700900026 COMMON 4 3 C259700900027 EN ANG-MIN ANG-MAX ERR-SYS C259700900028 MEV ADEG ADEG PER-CENT C259700900029 7.5 112.0 157.0 15.0 C259700900030 ENDCOMMON 3 0 C259700900031 DATA 3 43 C259700900032 E DATA DATA-ERR C259700900033 MEV MB/MEV MB/MEV C259700900034 4.03 1.215301 0.1713037 C259700900035 4.29 1.142027 0.1577455 C259700900036 4.55 1.472995 0.1810863 C259700900037 4.81 1.478827 0.1812399 C259700900038 5.07 1.839703 0.2083851 C259700900039 5.33 2.267314 0.2198955 C259700900040 5.59 2.991394 0.2875302 C259700900041 5.85 3.468245 0.3092102 C259700900042 6.11 3.823309 0.4066671 C259700900043 6.37 3.65627 0.3204261 C259700900044 6.63 4.301674 0.3149392 C259700900045 6.89 4.072086 0.2925822 C259700900046 7.15 5.359664 0.3592423 C259700900047 7.41 5.536062 0.3474805 C259700900048 7.67 6.022611 0.371258 C259700900049 7.93 5.616635 0.3432132 C259700900050 8.19 6.516909 0.3821172 C259700900051 8.45 5.742377 0.3456143 C259700900052 8.71 5.936641 0.3745488 C259700900053 8.969999 5.080589 0.3279859 C259700900054 9.23 5.596714 0.3572423 C259700900055 9.49 5.072848 0.325577 C259700900056 9.75 4.737724 0.3278546 C259700900057 10.009999 4.070632 0.3011928 C259700900058 10.27 3.654176 0.28535 C259700900059 10.53 2.977264 0.2490568 C259700900060 10.79 2.599129 0.2395421 C259700900061 11.049999 1.93731 0.202039 C259700900062 11.309999 1.247323 0.166575 C259700900063 11.57 1.650729 0.1802351 C259700900064 11.83 1.693434 0.1928789 C259700900065 12.089999 1.415727 0.1783023 C259700900066 12.349999 0.8424865 0.1353562 C259700900067 12.61 0.5908619 0.1075662 C259700900068 12.87 0.3865978 0.0869407 C259700900069 13.129999 0.2702089 0.0759526 C259700900070 13.389999 0.3654509 0.0881568 C259700900071 13.65 0.3055563 0.0759764 C259700900072 13.91 0.1838508 0.0627947 C259700900073 14.169999 0.123257 0.0513571 C259700900074 14.429999 0.0685988 0.0394031 C259700900075 14.69 0.188877 0.0619777 C259700900076 14.95 0.0990243 0.0449468 C259700900077 ENDDATA 45 0 C259700900078 ENDSUBENT 77 0 C259700999999 SUBENT C2597010 20210223 C201C259701000001 BIB 5 16 C259701000002 REACTION (26-FE-57(0,0),,LD) C259701000003 EN-SEC (E-EXC,26-FE-57) C259701000004 ANALYSIS (PES) In order to improve level density parameters, C259701000005 the experimental level densities have been fitted C259701000006 with the Fermi-gas function for two different spin C259701000007 cutoff factors sigma1 and sigma2. C259701000008 ERR-ANALYS (DATA-ERR1) Uncertainties of obtained level densities C259701000009 have been estimated to be about 20% which include C259701000010 uncertainties of absolute cross section measurements C259701000011 and uncertainties of particle transmission C259701000012 coefficients (text on page 044602-6) C259701000013 (DATA-ERR2) Errors shown in fig.5 C259701000014 STATUS (DEP,C2597003) C259701000015 (DEP,C2597006) C259701000016 (DEP,C2597009) C259701000017 (CURVE) Fig. 5, page 044602-7. C259701000018 ENDBIB 16 0 C259701000019 COMMON 1 3 C259701000020 DATA-ERR1 C259701000021 PER-CENT C259701000022 20.0 C259701000023 ENDCOMMON 3 0 C259701000024 DATA 3 23 C259701000025 E-EXC DATA DATA-ERR2 C259701000026 MEV 1/MEV 1/MEV C259701000027 4.024 2.593E+01 1.034E+01 C259701000028 4.274 5.416E+01 2.043E+01 C259701000029 4.559 5.909E+01 2.098E+01 C259701000030 4.844 9.652E+01 3.318E+01 C259701000031 5.129 1.191E+02 4.361E+01 C259701000032 5.397 1.751E+02 5.395E+01 C259701000033 5.681 1.944E+02 5.990E+01 C259701000034 5.949 2.618E+02 8.070E+01 C259701000035 6.215 2.440E+02 7.518E+01 C259701000036 6.499 2.234E+02 5.761E+01 C259701000037 6.784 3.008E+02 8.529E+01 C259701000038 7.052 4.501E+02 1.219E+02 C259701000039 7.336 4.826E+02 1.244E+02 C259701000040 7.639 5.648E+02 1.307E+02 C259701000041 7.888 5.847E+02 1.658E+02 C259701000042 8.190 6.964E+02 1.886E+02 C259701000043 8.475 8.898E+02 2.059E+02 C259701000044 8.742 1.137E+03 2.477E+02 C259701000045 9.027 1.241E+03 3.199E+02 C259701000046 9.294 1.557E+03 4.016E+02 C259701000047 9.579 1.584E+03 3.666E+02 C259701000048 9.846 1.920E+03 4.442E+02 C259701000049 10.148 2.497E+03 6.112E+02 C259701000050 ENDDATA 25 0 C259701000051 ENDSUBENT 50 0 C259701099999 ENDENTRY 10 0 C259799999999