ENTRY C1132 20171128 C172C113200000001 SUBENT C1132001 20171128 C172C113200100001 BIB 7 13 C113200100002 TITLE Excitation functions and angular distributions for C113200100003 the reaction C12(He3,n)O14 C113200100004 AUTHOR (G.U.Din,H.M.Kuan,T.W.Bonner) C113200100005 REFERENCE (J,NP,50,267,1964) C113200100006 #doi:10.1016/0029-5582(64)90206-8 C113200100007 INSTITUTE (1USARIC) C113200100008 FACILITY (VDG,1USARIC) The Rice University 5.5 MeV Van de C113200100009 Graaff accelerator. C113200100010 CORRECTION A detection efficiency correction, depending on the C113200100011 energy of neutrons, was applied for the neutrons C113200100012 counted at various He3 bombarding energies and angles C113200100013 of detection. C113200100014 HISTORY (20171128C) BP C113200100015 ENDBIB 13 0 C113200100016 NOCOMMON 0 0 C113200100017 ENDSUBENT 16 0 C113200199999 SUBENT C1132002 20171128 C172C113200200001 BIB 8 15 C113200200002 REACTION (6-C-12(HE3,N)8-O-14,,SIG) C113200200003 REL-REF (A,C0482001,Hsin-Min Kuan+,J,NP,51,518,1964) Better C113200200004 experimental uncertainties. C113200200005 SAMPLE The thin carbon target on a 0.025 cm tungsten backing C113200200006 was mounted on a 0.035 cm thick aluminium plate. C113200200007 DETECTOR (SCIN) A cylindrical plastic scintillator 2.2 cm in C113200200008 diameter and 1.8 cm long was used to detect the C113200200009 positrons C113200200010 (NAICR) A 2.54 cmx 2.54 cm NaI(TI) crystal was used forC113200200011 the detection of 2.31 MeV gamma rays. C113200200012 METHOD (ACTIV) C113200200013 DECAY-DATA (8-O-14,72.1SEC,B+,1830.,,DG,2310.) C113200200014 ERR-ANALYS (DATA-ERR,,30.) The error of this neutron cross C113200200015 section determination is estimated less than 30%. C113200200016 STATUS (CURVE) Fig. 1, page 269. C113200200017 ENDBIB 15 0 C113200200018 NOCOMMON 0 0 C113200200019 DATA 2 78 C113200200020 EN DATA C113200200021 MEV MB C113200200022 1.692 1.835 C113200200023 1.898 2.619 C113200200024 2.035 4.625 C113200200025 2.172 7.709 C113200200026 2.301 14.384 C113200200027 2.370 20.055 C113200200028 2.408 23.429 C113200200029 2.439 24.936 C113200200030 2.477 24.432 C113200200031 2.520 23.713 C113200200032 2.541 22.851 C113200200033 2.580 21.580 C113200200034 2.611 21.516 C113200200035 2.644 21.704 C113200200036 2.682 21.450 C113200200037 2.716 22.019 C113200200038 2.784 22.017 C113200200039 2.851 21.318 C113200200040 2.923 20.430 C113200200041 2.990 17.707 C113200200042 3.028 17.390 C113200200043 3.062 16.376 C113200200044 3.092 15.173 C113200200045 3.129 13.337 C113200200046 3.163 10.362 C113200200047 3.200 8.652 C113200200048 3.264 7.068 C113200200049 3.339 6.180 C113200200050 3.407 6.431 C113200200051 3.437 7.126 C113200200052 3.475 7.315 C113200200053 3.505 7.883 C113200200054 3.543 8.199 C113200200055 3.576 8.071 C113200200056 3.610 8.576 C113200200057 3.644 8.702 C113200200058 3.682 8.954 C113200200059 3.712 9.332 C113200200060 3.750 9.648 C113200200061 3.780 10.027 C113200200062 3.852 10.910 C113200200063 3.916 12.554 C113200200064 3.957 13.628 C113200200065 4.025 15.271 C113200200066 4.063 16.156 C113200200067 4.093 17.294 C113200200068 4.127 18.242 C113200200069 4.165 18.937 C113200200070 4.191 20.582 C113200200071 4.233 21.593 C113200200072 4.263 23.301 C113200200073 4.301 24.249 C113200200074 4.331 25.260 C113200200075 4.369 26.398 C113200200076 4.399 27.347 C113200200077 4.467 28.610 C113200200078 4.505 31.710 C113200200079 4.535 32.785 C113200200080 4.569 34.366 C113200200081 4.603 36.263 C113200200082 4.641 37.148 C113200200083 4.675 36.514 C113200200084 4.705 36.893 C113200200085 4.739 35.942 C113200200086 4.773 35.625 C113200200087 4.810 35.750 C113200200088 4.841 37.711 C113200200089 4.874 37.710 C113200200090 4.912 39.418 C113200200091 4.939 41.125 C113200200092 4.980 41.820 C113200200093 5.014 40.237 C113200200094 5.048 40.806 C113200200095 5.082 38.843 C113200200096 5.119 36.564 C113200200097 5.190 29.917 C113200200098 5.258 30.675 C113200200099 5.323 41.114 C113200200100 ENDDATA 80 0 C113200200101 ENDSUBENT 100 0 C113200299999 SUBENT C1132003 20171128 C172C113200300001 BIB 4 15 C113200300002 REACTION (6-C-12(HE3,N)8-O-14,,DA) C113200300003 DETECTOR (BF3) B10 enriched BF3 counter (modified long C113200300004 counter). The counter tube was 2.5 cm in diameter and C113200300005 15 cm in length and was embedded in a paraffin C113200300006 cylinder 15 cm in diameter and 12.2 cm long. C113200300007 SAMPLE The carbon target used for the excitation functions C113200300008 and for the total yield was made by cracking carbon C113200300009 from methyl iodide (CH3I) on a tungsten blank of C113200300010 1.905 cm diameter and 0.025 cm thickness. The C113200300011 thickness of the carbon target was about 60 keV for 3 C113200300012 MeV He3 particles. For the study of the angular C113200300013 distributions, a carbon target was made in the same C113200300014 way as mentioned above on a thick tantalum backing. It C113200300015 was about 300 keV thick for 3 MeV He3 ions. C113200300016 STATUS (CURVE) Fig. 1, page 269. C113200300017 ENDBIB 15 0 C113200300018 COMMON 1 3 C113200300019 ANG C113200300020 ADEG C113200300021 0.0 C113200300022 ENDCOMMON 3 0 C113200300023 DATA 2 75 C113200300024 EN DATA C113200300025 MEV MB/SR C113200300026 1.690 0.147 C113200300027 1.754 0.146 C113200300028 1.825 0.190 C113200300029 1.863 0.234 C113200300030 1.897 0.278 C113200300031 1.965 0.380 C113200300032 2.033 0.571 C113200300033 2.067 0.645 C113200300034 2.100 0.703 C113200300035 2.138 0.777 C113200300036 2.172 0.909 C113200300037 2.202 1.100 C113200300038 2.236 1.233 C113200300039 2.274 1.439 C113200300040 2.304 1.645 C113200300041 2.338 1.836 C113200300042 2.376 2.042 C113200300043 2.410 2.115 C113200300044 2.444 2.056 C113200300045 2.477 1.967 C113200300046 2.511 1.673 C113200300047 2.545 1.334 C113200300048 2.579 1.024 C113200300049 2.616 0.818 C113200300050 2.650 0.759 C113200300051 2.684 0.685 C113200300052 2.714 0.758 C113200300053 2.752 0.773 C113200300054 2.786 0.816 C113200300055 2.823 0.949 C113200300056 2.853 1.007 C113200300057 2.887 1.081 C113200300058 2.921 1.213 C113200300059 2.959 1.345 C113200300060 2.989 1.493 C113200300061 3.027 1.698 C113200300062 3.064 1.698 C113200300063 3.098 1.153 C113200300064 3.098 1.271 C113200300065 3.132 0.814 C113200300066 3.166 0.608 C113200300067 3.200 0.652 C113200300068 3.237 0.799 C113200300069 3.264 0.946 C113200300070 3.301 1.078 C113200300071 3.335 1.210 C113200300072 3.365 1.269 C113200300073 3.407 1.313 C113200300074 3.478 1.357 C113200300075 3.542 1.341 C113200300076 3.614 1.576 C113200300077 3.682 1.782 C113200300078 3.746 2.120 C113200300079 3.806 2.341 C113200300080 3.885 2.620 C113200300081 3.957 3.062 C113200300082 4.025 3.400 C113200300083 4.089 3.797 C113200300084 4.165 4.150 C113200300085 4.233 4.311 C113200300086 4.300 4.591 C113200300087 4.368 4.885 C113200300088 4.436 5.385 C113200300089 4.504 5.591 C113200300090 4.576 5.973 C113200300091 4.644 6.400 C113200300092 4.712 6.488 C113200300093 4.779 6.281 C113200300094 4.847 6.590 C113200300095 4.911 6.943 C113200300096 4.983 7.443 C113200300097 5.047 7.855 C113200300098 5.122 7.442 C113200300099 5.190 7.795 C113200300100 5.258 7.530 C113200300101 ENDDATA 77 0 C113200300102 ENDSUBENT 101 0 C113200399999 SUBENT C1132004 20171128 C172C113200400001 BIB 4 15 C113200400002 REACTION (6-C-12(HE3,N)8-O-14,,DA) C113200400003 DETECTOR (BF3) B10 enriched BF3 counter (modified long C113200400004 counter). The counter tube was 2.5 cm in diameter and C113200400005 15 cm in length and was embedded in a paraffin C113200400006 cylinder 15 cm in diameter and 12.2 cm long. C113200400007 SAMPLE The carbon target used for the excitation functions C113200400008 and for the total yield was made by cracking carbon C113200400009 from methyl iodide (CH3I) on a tungsten blank of C113200400010 1.905 cm diameter and 0.025 cm thickness. The C113200400011 thickness of the carbon target was about 60 keV for 3 C113200400012 MeV He3 particles. For the study of the angular C113200400013 distributions, a carbon target was made in the same C113200400014 way as mentioned above on a thick tantalum backing. It C113200400015 was about 300 keV thick for 3 MeV He3 ions. C113200400016 STATUS (CURVE) Fig. 1, page 269. C113200400017 ENDBIB 15 0 C113200400018 COMMON 1 3 C113200400019 ANG C113200400020 ADEG C113200400021 90.0 C113200400022 ENDCOMMON 3 0 C113200400023 DATA 2 99 C113200400024 EN DATA C113200400025 MEV MB/SR C113200400026 1.686 0.058 C113200400027 1.754 0.073 C113200400028 1.822 0.116 C113200400029 1.863 0.116 C113200400030 1.893 0.131 C113200400031 1.965 0.189 C113200400032 2.029 0.233 C113200400033 2.066 0.247 C113200400034 2.104 0.291 C113200400035 2.138 0.335 C113200400036 2.172 0.379 C113200400037 2.206 0.438 C113200400038 2.236 0.496 C113200400039 2.274 0.570 C113200400040 2.304 0.702 C113200400041 2.338 0.849 C113200400042 2.375 1.040 C113200400043 2.406 1.158 C113200400044 2.443 1.379 C113200400045 2.477 1.437 C113200400046 2.515 1.496 C113200400047 2.545 1.510 C113200400048 2.575 1.466 C113200400049 2.616 1.451 C113200400050 2.650 1.421 C113200400051 2.680 1.480 C113200400052 2.718 1.494 C113200400053 2.752 1.509 C113200400054 2.790 1.479 C113200400055 2.816 1.435 C113200400056 2.854 1.390 C113200400057 2.887 1.316 C113200400058 2.925 1.213 C113200400059 2.959 1.183 C113200400060 3.000 1.154 C113200400061 3.027 1.139 C113200400062 3.060 1.168 C113200400063 3.098 1.124 C113200400064 3.124 0.814 C113200400065 3.124 1.020 C113200400066 3.169 0.770 C113200400067 3.199 0.637 C113200400068 3.230 0.489 C113200400069 3.263 0.445 C113200400070 3.301 0.356 C113200400071 3.339 0.327 C113200400072 3.369 0.326 C113200400073 3.406 0.282 C113200400074 3.440 0.296 C113200400075 3.470 0.296 C113200400076 3.512 0.311 C113200400077 3.542 0.340 C113200400078 3.576 0.384 C113200400079 3.610 0.384 C113200400080 3.644 0.428 C113200400081 3.681 0.413 C113200400082 3.719 0.412 C113200400083 3.749 0.456 C113200400084 3.779 0.485 C113200400085 3.817 0.485 C113200400086 3.854 0.514 C113200400087 3.884 0.544 C113200400088 3.918 0.573 C113200400089 3.956 0.587 C113200400090 3.990 0.617 C113200400091 4.028 0.616 C113200400092 4.054 0.631 C113200400093 4.092 0.675 C113200400094 4.125 0.733 C113200400095 4.163 0.763 C113200400096 4.193 0.762 C113200400097 4.231 0.792 C113200400098 4.261 0.850 C113200400099 4.299 0.894 C113200400100 4.333 0.953 C113200400101 4.366 0.982 C113200400102 4.397 1.056 C113200400103 4.434 1.099 C113200400104 4.472 1.129 C113200400105 4.506 1.217 C113200400106 4.540 1.305 C113200400107 4.574 1.408 C113200400108 4.604 1.466 C113200400109 4.638 1.599 C113200400110 4.675 1.569 C113200400111 4.709 1.672 C113200400112 4.739 1.598 C113200400113 4.777 1.598 C113200400114 4.811 1.598 C113200400115 4.845 1.745 C113200400116 4.913 2.009 C113200400117 4.947 2.083 C113200400118 4.950 2.215 C113200400119 4.984 2.289 C113200400120 5.052 2.465 C113200400121 5.116 2.273 C113200400122 5.188 2.420 C113200400123 5.259 2.552 C113200400124 5.324 3.288 C113200400125 ENDDATA 101 0 C113200400126 ENDSUBENT 125 0 C113200499999 SUBENT C1132005 20171128 C172C113200500001 BIB 4 15 C113200500002 REACTION (6-C-12(HE3,N)8-O-14,,DA) C113200500003 DETECTOR (BF3) B10 enriched BF3 counter (modified long C113200500004 counter). The counter tube was 2.5 cm in diameter and C113200500005 15 cm in length and was embedded in a paraffin C113200500006 cylinder 15 cm in diameter and 12.2 cm long. C113200500007 SAMPLE The carbon target used for the excitation functions C113200500008 and for the total yield was made by cracking carbon C113200500009 from methyl iodide (CH3I) on a tungsten blank of C113200500010 1.905 cm diameter and 0.025 cm thickness. The C113200500011 thickness of the carbon target was about 60 keV for 3 C113200500012 MeV He3 particles. For the study of the angular C113200500013 distributions, a carbon target was made in the same C113200500014 way as mentioned above on a thick tantalum backing. It C113200500015 was about 300 keV thick for 3 MeV He3 ions. C113200500016 STATUS (CURVE) Fig. 2, page 270. C113200500017 ENDBIB 15 0 C113200500018 COMMON 1 3 C113200500019 EN C113200500020 MEV C113200500021 1.87 C113200500022 ENDCOMMON 3 0 C113200500023 DATA 2 9 C113200500024 ANG-CM DATA-CM C113200500025 ADEG MB/SR C113200500026 4.221 0.373 C113200500027 24.490 0.401 C113200500028 50.115 0.369 C113200500029 73.958 0.382 C113200500030 96.011 0.380 C113200500031 116.275 0.378 C113200500032 133.560 0.377 C113200500033 150.249 0.376 C113200500034 166.339 0.360 C113200500035 ENDDATA 11 0 C113200500036 ENDSUBENT 35 0 C113200599999 SUBENT C1132006 20171128 C172C113200600001 BIB 4 15 C113200600002 REACTION (6-C-12(HE3,N)8-O-14,,DA) C113200600003 DETECTOR (BF3) B10 enriched BF3 counter (modified long C113200600004 counter). The counter tube was 2.5 cm in diameter and C113200600005 15 cm in length and was embedded in a paraffin C113200600006 cylinder 15 cm in diameter and 12.2 cm long. C113200600007 SAMPLE The carbon target used for the excitation functions C113200600008 and for the total yield was made by cracking carbon C113200600009 from methyl iodide (CH3I) on a tungsten blank of C113200600010 1.905 cm diameter and 0.025 cm thickness. The C113200600011 thickness of the carbon target was about 60 keV for 3 C113200600012 MeV He3 particles. For the study of the angular C113200600013 distributions, a carbon target was made in the same C113200600014 way as mentioned above on a thick tantalum backing. It C113200600015 was about 300 keV thick for 3 MeV He3 ions. C113200600016 STATUS (CURVE) Fig. 2, page 270. C113200600017 ENDBIB 15 0 C113200600018 COMMON 1 3 C113200600019 EN C113200600020 MEV C113200600021 2.33 C113200600022 ENDCOMMON 3 0 C113200600023 DATA 2 9 C113200600024 ANG-CM DATA-CM C113200600025 ADEG MB/SR C113200600026 3.939 1.373 C113200600027 23.560 1.190 C113200600028 47.897 0.813 C113200600029 68.750 0.780 C113200600030 97.452 1.133 C113200600031 111.306 1.683 C113200600032 129.344 2.277 C113200600033 146.711 2.587 C113200600034 165.815 2.704 C113200600035 ENDDATA 11 0 C113200600036 ENDSUBENT 35 0 C113200699999 SUBENT C1132007 20171128 C172C113200700001 BIB 4 15 C113200700002 REACTION (6-C-12(HE3,N)8-O-14,,DA) C113200700003 DETECTOR (BF3) B10 enriched BF3 counter (modified long C113200700004 counter). The counter tube was 2.5 cm in diameter and C113200700005 15 cm in length and was embedded in a paraffin C113200700006 cylinder 15 cm in diameter and 12.2 cm long. C113200700007 SAMPLE The carbon target used for the excitation functions C113200700008 and for the total yield was made by cracking carbon C113200700009 from methyl iodide (CH3I) on a tungsten blank of C113200700010 1.905 cm diameter and 0.025 cm thickness. The C113200700011 thickness of the carbon target was about 60 keV for 3 C113200700012 MeV He3 particles. For the study of the angular C113200700013 distributions, a carbon target was made in the same C113200700014 way as mentioned above on a thick tantalum backing. It C113200700015 was about 300 keV thick for 3 MeV He3 ions. C113200700016 STATUS (CURVE) Fig. 2, page 270. C113200700017 ENDBIB 15 0 C113200700018 COMMON 1 3 C113200700019 EN C113200700020 MEV C113200700021 2.66 C113200700022 ENDCOMMON 3 0 C113200700023 DATA 2 9 C113200700024 ANG-CM DATA-CM C113200700025 ADEG MB/SR C113200700026 4.737 0.787 C113200700027 23.684 0.668 C113200700028 46.776 0.653 C113200700029 69.868 0.950 C113200700030 90.592 1.604 C113200700031 110.132 2.198 C113200700032 129.079 3.000 C113200700033 146.842 3.460 C113200700034 163.421 3.653 C113200700035 ENDDATA 11 0 C113200700036 ENDSUBENT 35 0 C113200799999 SUBENT C1132008 20171128 C172C113200800001 BIB 4 15 C113200800002 REACTION (6-C-12(HE3,N)8-O-14,,DA) C113200800003 DETECTOR (BF3) B10 enriched BF3 counter (modified long C113200800004 counter). The counter tube was 2.5 cm in diameter and C113200800005 15 cm in length and was embedded in a paraffin C113200800006 cylinder 15 cm in diameter and 12.2 cm long. C113200800007 SAMPLE The carbon target used for the excitation functions C113200800008 and for the total yield was made by cracking carbon C113200800009 from methyl iodide (CH3I) on a tungsten blank of C113200800010 1.905 cm diameter and 0.025 cm thickness. The C113200800011 thickness of the carbon target was about 60 keV for 3 C113200800012 MeV He3 particles. For the study of the angular C113200800013 distributions, a carbon target was made in the same C113200800014 way as mentioned above on a thick tantalum backing. It C113200800015 was about 300 keV thick for 3 MeV He3 ions. C113200800016 STATUS (CURVE) Fig. 2, page 270. C113200800017 ENDBIB 15 0 C113200800018 COMMON 1 3 C113200800019 EN C113200800020 MEV C113200800021 2.87 C113200800022 ENDCOMMON 3 0 C113200800023 DATA 2 9 C113200800024 ANG-CM DATA-CM C113200800025 ADEG MB/SR C113200800026 4.452 1.232 C113200800027 23.865 0.991 C113200800028 46.830 0.794 C113200800029 69.348 1.147 C113200800030 90.709 1.589 C113200800031 110.840 1.838 C113200800032 129.805 2.147 C113200800033 146.391 2.382 C113200800034 163.563 2.602 C113200800035 ENDDATA 11 0 C113200800036 ENDSUBENT 35 0 C113200899999 SUBENT C1132009 20171128 C172C113200900001 BIB 4 15 C113200900002 REACTION (6-C-12(HE3,N)8-O-14,,DA) C113200900003 DETECTOR (BF3) B10 enriched BF3 counter (modified long C113200900004 counter). The counter tube was 2.5 cm in diameter and C113200900005 15 cm in length and was embedded in a paraffin C113200900006 cylinder 15 cm in diameter and 12.2 cm long. C113200900007 SAMPLE The carbon target used for the excitation functions C113200900008 and for the total yield was made by cracking carbon C113200900009 from methyl iodide (CH3I) on a tungsten blank of C113200900010 1.905 cm diameter and 0.025 cm thickness. The C113200900011 thickness of the carbon target was about 60 keV for 3 C113200900012 MeV He3 particles. For the study of the angular C113200900013 distributions, a carbon target was made in the same C113200900014 way as mentioned above on a thick tantalum backing. It C113200900015 was about 300 keV thick for 3 MeV He3 ions. C113200900016 STATUS (CURVE) Fig. 2, page 270. C113200900017 ENDBIB 15 0 C113200900018 COMMON 1 3 C113200900019 EN C113200900020 MEV C113200900021 3.11 C113200900022 ENDCOMMON 3 0 C113200900023 DATA 2 9 C113200900024 ANG-CM DATA-CM C113200900025 ADEG MB/SR C113200900026 4.324 0.7385 C113200900027 22.557 0.62225 C113200900028 45.571 0.5465 C113200900029 68.810 0.6875 C113200900030 90.230 0.78725 C113200900031 109.726 0.7455 C113200900032 128.575 0.65125 C113200900033 146.875 0.59825 C113200900034 162.845 0.58275 C113200900035 ENDDATA 11 0 C113200900036 ENDSUBENT 35 0 C113200999999 SUBENT C1132010 20171128 C172C113201000001 BIB 4 15 C113201000002 REACTION (6-C-12(HE3,N)8-O-14,,DA) C113201000003 DETECTOR (BF3) B10 enriched BF3 counter (modified long C113201000004 counter). The counter tube was 2.5 cm in diameter and C113201000005 15 cm in length and was embedded in a paraffin C113201000006 cylinder 15 cm in diameter and 12.2 cm long. C113201000007 SAMPLE The carbon target used for the excitation functions C113201000008 and for the total yield was made by cracking carbon C113201000009 from methyl iodide (CH3I) on a tungsten blank of C113201000010 1.905 cm diameter and 0.025 cm thickness. The C113201000011 thickness of the carbon target was about 60 keV for 3 C113201000012 MeV He3 particles. For the study of the angular C113201000013 distributions, a carbon target was made in the same C113201000014 way as mentioned above on a thick tantalum backing. It C113201000015 was about 300 keV thick for 3 MeV He3 ions. C113201000016 STATUS (CURVE) Fig. 2, page 270. C113201000017 ENDBIB 15 0 C113201000018 COMMON 1 3 C113201000019 EN C113201000020 MEV C113201000021 3.93 C113201000022 ENDCOMMON 3 0 C113201000023 DATA 2 9 C113201000024 ANG-CM DATA-CM C113201000025 ADEG MB/SR C113201000026 4.507 2.727 C113201000027 23.414 2.425 C113201000028 45.808 1.616 C113201000029 68.837 1.134 C113201000030 90.132 0.979 C113201000031 108.475 0.884 C113201000032 128.614 0.936 C113201000033 145.842 1.376 C113201000034 163.032 1.518 C113201000035 ENDDATA 11 0 C113201000036 ENDSUBENT 35 0 C113201099999 SUBENT C1132011 20171128 C172C113201100001 BIB 4 15 C113201100002 REACTION (6-C-12(HE3,N)8-O-14,,DA) C113201100003 DETECTOR (BF3) B10 enriched BF3 counter (modified long C113201100004 counter). The counter tube was 2.5 cm in diameter and C113201100005 15 cm in length and was embedded in a paraffin C113201100006 cylinder 15 cm in diameter and 12.2 cm long. C113201100007 SAMPLE The carbon target used for the excitation functions C113201100008 and for the total yield was made by cracking carbon C113201100009 from methyl iodide (CH3I) on a tungsten blank of C113201100010 1.905 cm diameter and 0.025 cm thickness. The C113201100011 thickness of the carbon target was about 60 keV for 3 C113201100012 MeV He3 particles. For the study of the angular C113201100013 distributions, a carbon target was made in the same C113201100014 way as mentioned above on a thick tantalum backing. It C113201100015 was about 300 keV thick for 3 MeV He3 ions. C113201100016 STATUS (CURVE) Fig. 2, page 270. C113201100017 ENDBIB 15 0 C113201100018 COMMON 1 3 C113201100019 EN C113201100020 MEV C113201100021 4.49 C113201100022 ENDCOMMON 3 0 C113201100023 DATA 2 9 C113201100024 ANG-CM DATA-CM C113201100025 ADEG MB/SR C113201100026 4.680 5.704 C113201100027 23.427 4.695 C113201100028 46.078 2.478 C113201100029 67.780 1.438 C113201100030 87.886 1.310 C113201100031 108.654 1.535 C113201100032 127.641 1.732 C113201100033 146.029 1.899 C113201100034 163.169 1.744 C113201100035 ENDDATA 11 0 C113201100036 ENDSUBENT 35 0 C113201199999 SUBENT C1132012 20171128 C172C113201200001 BIB 4 15 C113201200002 REACTION (6-C-12(HE3,N)8-O-14,,DA) C113201200003 DETECTOR (BF3) B10 enriched BF3 counter (modified long C113201200004 counter). The counter tube was 2.5 cm in diameter and C113201200005 15 cm in length and was embedded in a paraffin C113201200006 cylinder 15 cm in diameter and 12.2 cm long. C113201200007 SAMPLE The carbon target used for the excitation functions C113201200008 and for the total yield was made by cracking carbon C113201200009 from methyl iodide (CH3I) on a tungsten blank of C113201200010 1.905 cm diameter and 0.025 cm thickness. The C113201200011 thickness of the carbon target was about 60 keV for 3 C113201200012 MeV He3 particles. For the study of the angular C113201200013 distributions, a carbon target was made in the same C113201200014 way as mentioned above on a thick tantalum backing. It C113201200015 was about 300 keV thick for 3 MeV He3 ions. C113201200016 STATUS (CURVE) Fig. 2, page 270. C113201200017 ENDBIB 15 0 C113201200018 COMMON 1 3 C113201200019 EN C113201200020 MEV C113201200021 4.75 C113201200022 ENDCOMMON 3 0 C113201200023 DATA 2 9 C113201200024 ANG-CM DATA-CM C113201200025 ADEG MB/SR C113201200026 4.539 6.231 C113201200027 22.743 4.840 C113201200028 46.193 2.444 C113201200029 67.384 1.613 C113201200030 88.036 1.551 C113201200031 108.111 1.695 C113201200032 128.182 1.781 C113201200033 145.310 1.984 C113201200034 162.419 1.893 C113201200035 ENDDATA 11 0 C113201200036 ENDSUBENT 35 0 C113201299999 SUBENT C1132013 20171128 C172C113201300001 BIB 4 15 C113201300002 REACTION (6-C-12(HE3,N)8-O-14,,DA) C113201300003 DETECTOR (BF3) B10 enriched BF3 counter (modified long C113201300004 counter). The counter tube was 2.5 cm in diameter and C113201300005 15 cm in length and was embedded in a paraffin C113201300006 cylinder 15 cm in diameter and 12.2 cm long. C113201300007 SAMPLE The carbon target used for the excitation functions C113201300008 and for the total yield was made by cracking carbon C113201300009 from methyl iodide (CH3I) on a tungsten blank of C113201300010 1.905 cm diameter and 0.025 cm thickness. The C113201300011 thickness of the carbon target was about 60 keV for 3 C113201300012 MeV He3 particles. For the study of the angular C113201300013 distributions, a carbon target was made in the same C113201300014 way as mentioned above on a thick tantalum backing. It C113201300015 was about 300 keV thick for 3 MeV He3 ions. C113201300016 STATUS (CURVE) Fig. 2, page 270. C113201300017 ENDBIB 15 0 C113201300018 COMMON 1 3 C113201300019 EN C113201300020 MEV C113201300021 5.19 C113201300022 ENDCOMMON 3 0 C113201300023 DATA 2 9 C113201300024 ANG-CM DATA-CM C113201300025 ADEG MB/SR C113201300026 5.524 7.056 C113201300027 22.896 5.378 C113201300028 46.094 3.317 C113201300029 68.309 2.251 C113201300030 88.309 1.919 C113201300031 108.419 2.144 C113201300032 127.332 2.281 C113201300033 145.023 2.214 C113201300034 162.096 2.000 C113201300035 ENDDATA 11 0 C113201300036 ENDSUBENT 35 0 C113201399999 ENDENTRY 13 0 C113299999999