ENTRY F1375 20181207 F071F137500000001 SUBENT F1375001 20181207 F071F137500100001 BIB 7 8 F137500100002 TITLE Investigation of the C12(t,a)B11 reactions. F137500100003 AUTHOR (K.Niedzwiedziuk,V.I.Salatskii,I.V.Sizov) F137500100004 INSTITUTE (4ZZZDUB) F137500100005 REFERENCE (J,ZET,44,1450,1963) F137500100006 (J,JET,17,974,1963) English translation F137500100007 FACILITY (VDG,4ZZZDUB) Electrostatic generator F137500100008 METHOD (PHD) F137500100009 HISTORY (20181207C) F137500100010 ENDBIB 8 0 F137500100011 NOCOMMON 0 0 F137500100012 ENDSUBENT 11 0 F137500199999 SUBENT F1375002 20181207 F071F137500200001 BIB 5 8 F137500200002 REACTION (6-C-12(T,A)5-B-11,PAR,DA) F137500200003 DETECTOR (SIBAR) F137500200004 SAMPLE Solid carbon target was made by evaporating graphite F137500200005 in vacuum on a glass plate. The thickness was 15 to F137500200006 25 mu-g/cm2. F137500200007 ERR-ANALYS (DATA-ERR) Error from the graphic bars. No source of F137500200008 uncertainty is given. F137500200009 STATUS (CURVE) Figure 2 F137500200010 ENDBIB 8 0 F137500200011 COMMON 4 3 F137500200012 E-LVL ANG EN-ERR-DIG ERR-DIG F137500200013 MEV ADEG KEV MB/SR F137500200014 0. 90. 1.66 0.00964 F137500200015 ENDCOMMON 3 0 F137500200016 DATA 3 123 F137500200017 EN DATA DATA-ERR F137500200018 KEV MB/SR MB/SR F137500200019 281.83 0.00802 F137500200020 398.50 0.07277 F137500200021 413.95 0.07001 F137500200022 420.80 0.08683 F137500200023 441.37 0.12050 F137500200024 456.82 0.12054 F137500200025 489.37 0.18506 F137500200026 503.09 0.19630 F137500200027 509.95 0.20192 F137500200028 511.69 0.18512 F137500200029 537.34 0.28043 F137500200030 537.35 0.26922 F137500200031 551.05 0.30287 F137500200032 561.31 0.34772 F137500200033 561.33 0.32811 F137500200034 586.93 0.47384 F137500200035 600.65 0.48228 F137500200036 607.43 0.56633 F137500200037 610.82 0.60836 F137500200038 610.84 0.58875 F137500200039 626.20 0.67843 F137500200040 636.39 0.79050 F137500200041 636.40 0.77930 F137500200042 638.02 0.87734 0.03361 F137500200043 646.54 0.93619 F137500200044 649.91 0.99502 F137500200045 649.94 0.97261 F137500200046 655.04 1.01740 F137500200047 660.17 1.03710 F137500200048 661.88 1.04830 F137500200049 661.90 1.02310 F137500200050 667.06 1.01190 F137500200051 668.84 0.95585 F137500200052 673.95 0.98948 F137500200053 674.00 0.94746 F137500200054 674.02 0.92786 F137500200055 675.85 0.81021 0.03362 F137500200056 677.50 0.87464 F137500200057 679.24 0.86064 F137500200058 689.55 0.84947 F137500200059 689.68 0.72342 F137500200060 696.52 0.74585 0.02521 F137500200061 713.89 0.54701 F137500200062 715.54 0.60864 F137500200063 715.56 0.59184 F137500200064 720.75 0.54983 F137500200065 729.34 0.54986 F137500200066 731.06 0.54146 F137500200067 744.77 0.56951 F137500200068 749.85 0.63955 F137500200069 760.21 0.57515 F137500200070 761.87 0.62838 F137500200071 761.89 0.61717 F137500200072 761.91 0.58916 F137500200073 772.19 0.61160 F137500200074 787.52 0.72648 F137500200075 806.30 0.83578 F137500200076 818.31 0.84141 F137500200077 848.96 1.08520 F137500200078 864.25 1.24490 F137500200079 864.81 1.22660 F137500200080 869.41 1.23650 F137500200081 869.67 1.20320 F137500200082 876.94 1.21490 F137500200083 877.99 1.23650 F137500200084 896.29 1.41410 F137500200085 925.35 1.60150 F137500200086 930.19 1.62500 F137500200087 937.45 1.68350 F137500200088 956.82 1.80070 F137500200089 973.78 1.88270 F137500200090 990.69 2.17550 F137500200091 1002.80 2.21070 F137500200092 1017.30 2.25760 F137500200093 1019.80 2.31620 F137500200094 1022.20 2.40980 F137500200095 1051.20 2.70270 F137500200096 1058.40 2.83150 F137500200097 1060.90 2.78470 F137500200098 1060.90 2.87840 F137500200099 1065.70 2.96030 F137500200100 1068.10 3.08910 F137500200101 1072.90 3.06570 F137500200102 1073.00 2.92520 F137500200103 1077.80 3.14770 F137500200104 1080.20 3.18290 F137500200105 1085.00 3.24140 F137500200106 1085.00 3.42880 F137500200107 1089.80 3.39370 F137500200108 1094.70 3.41710 F137500200109 1097.10 3.53420 F137500200110 1099.50 3.79180 F137500200111 1104.30 3.74500 F137500200112 1111.50 4.08460 F137500200113 1111.60 3.90890 F137500200114 1116.40 4.21340 F137500200115 1118.80 4.06120 F137500200116 1118.80 4.16650 F137500200117 1126.00 4.24850 F137500200118 1126.00 4.29540 F137500200119 1126.10 4.20170 F137500200120 1130.90 4.44760 F137500200121 1133.30 4.35390 F137500200122 1133.30 4.41250 F137500200123 1135.70 4.69350 F137500200124 1138.10 4.52960 F137500200125 1138.10 4.72860 F137500200126 1140.50 4.49450 F137500200127 1140.60 4.42420 F137500200128 1150.20 4.92770 F137500200129 1152.60 4.78720 F137500200130 1157.40 5.02140 F137500200131 1164.70 5.16200 F137500200132 1169.50 5.31420 F137500200133 1174.20 5.70060 F137500200134 1186.40 5.70070 F137500200135 1193.60 5.89970 F137500200136 1196.00 5.99340 0.17563 F137500200137 1203.30 6.13390 F137500200138 1205.60 6.35640 F137500200139 1227.40 6.55560 F137500200140 1229.90 6.49700 F137500200141 1239.50 6.61420 F137500200142 ENDDATA 125 0 F137500200143 ENDSUBENT 142 0 F137500299999 SUBENT F1375003 20181207 F071F137500300001 BIB 5 8 F137500300002 REACTION (6-C-12(T,A)5-B-11,PAR,DA) F137500300003 DETECTOR (SIBAR) F137500300004 SAMPLE CH4 or CO2 gas target was used. The pressure was F137500300005 60 mm Hg. The exit window was sealed with a mica film F137500300006 with the thickness of 0.13 mg/cm2. F137500300007 ERR-ANALYS (DATA-ERR) Error from the graphic bars. No source of F137500300008 uncertainty is given. F137500300009 STATUS (CURVE) Figure 2 F137500300010 ENDBIB 8 0 F137500300011 COMMON 4 3 F137500300012 E-LVL ANG EN-ERR-DIG ERR-DIG F137500300013 MEV ADEG KEV MB/SR F137500300014 0. 90. 1.56 0.00729 F137500300015 ENDCOMMON 3 0 F137500300016 DATA 3 31 F137500300017 EN DATA DATA-ERR F137500300018 KEV MB/SR MB/SR F137500300019 542.52 0.25523 0.01681 F137500300020 568.19 0.32813 0.01961 F137500300021 581.84 0.41220 0.02241 F137500300022 597.26 0.44025 0.02802 F137500300023 602.32 0.52710 0.02521 F137500300024 621.16 0.56917 0.02801 F137500300025 629.66 0.65603 0.03081 F137500300026 646.66 0.82414 0.03922 F137500300027 655.08 0.98103 0.04481 F137500300028 667.16 0.91943 0.04482 F137500300029 684.44 0.80464 0.03641 F137500300030 696.61 0.65621 0.03361 F137500300031 703.56 0.57219 F137500300032 705.25 0.60021 F137500300033 706.94 0.62543 F137500300034 717.35 0.51901 0.02521 F137500300035 722.42 0.60026 0.03081 F137500300036 755.04 0.59194 0.02240 F137500300037 825.08 0.93107 0.04482 F137500300038 825.98 0.90902 F137500300039 837.07 0.96191 0.04482 F137500300040 838.09 0.94424 F137500300041 842.08 1.09640 0.04762 F137500300042 842.90 1.07310 F137500300043 876.77 1.29580 F137500300044 954.21 1.75290 F137500300045 963.90 1.78810 F137500300046 968.71 1.89360 F137500300047 1012.20 2.30370 0.09367 F137500300048 1087.10 3.15890 0.12879 F137500300049 1099.00 3.95520 0.12879 F137500300050 ENDDATA 33 0 F137500300051 ENDSUBENT 50 0 F137500399999 SUBENT F1375004 20181207 F071F137500400001 BIB 5 8 F137500400002 REACTION (6-C-12(T,A)5-B-11,PAR,DA) F137500400003 DETECTOR (SIBAR) F137500400004 SAMPLE Solid carbon target was made by evaporating graphite F137500400005 in vacuum on a glass plate. The thickness was 15 to F137500400006 25 mu-g/cm2. F137500400007 ERR-ANALYS (DATA-ERR) Error from the graphic bars. No source of F137500400008 uncertainty is given. F137500400009 STATUS (CURVE) Figure 3 F137500400010 ENDBIB 8 0 F137500400011 COMMON 4 3 F137500400012 E-LVL ANG EN-ERR-DIG ERR-DIG F137500400013 MEV ADEG KEV MB/SR F137500400014 2.13 90. 1.35 0.00353 F137500400015 ENDCOMMON 3 0 F137500400016 DATA 3 86 F137500400017 EN DATA DATA-ERR F137500400018 KEV MB/SR MB/SR F137500400019 419.38 0.02570 F137500400020 502.68 0.07009 F137500400021 536.73 0.07417 F137500400022 538.58 0.06048 F137500400023 551.87 0.08307 F137500400024 587.86 0.10990 F137500400025 610.65 0.15057 F137500400026 627.76 0.19131 F137500400027 642.86 0.17745 F137500400028 654.39 0.25470 F137500400029 663.88 0.27278 F137500400030 671.41 0.25902 F137500400031 675.25 0.28174 F137500400032 678.97 0.25436 F137500400033 694.08 0.24960 F137500400034 714.86 0.24021 F137500400035 735.65 0.23537 F137500400036 735.70 0.25813 F137500400037 750.75 0.22605 F137500400038 752.70 0.24879 F137500400039 763.99 0.22587 F137500400040 764.06 0.25774 F137500400041 765.91 0.23950 F137500400042 779.17 0.24843 F137500400043 792.44 0.26191 F137500400044 807.56 0.26170 F137500400045 809.48 0.27533 F137500400046 820.83 0.27518 F137500400047 835.93 0.26586 F137500400048 851.14 0.29753 F137500400049 866.20 0.27000 F137500400050 870.04 0.29727 F137500400051 900.26 0.28319 F137500400052 926.73 0.28283 F137500400053 932.45 0.30096 0.02732 F137500400054 940.08 0.32818 F137500400055 958.94 0.30971 F137500400056 993.16 0.38665 F137500400057 1006.50 0.43200 F137500400058 1019.90 0.50012 F137500400059 1021.90 0.52742 F137500400060 1025.80 0.59112 0.03643 F137500400061 1054.50 0.72733 F137500400062 1058.70 0.93219 F137500400063 1060.90 1.03230 F137500400064 1062.10 0.75455 F137500400065 1067.00 1.21440 F137500400066 1071.00 1.31000 0.05009 F137500400067 1073.10 1.39190 F137500400068 1074.00 0.96841 F137500400069 1079.10 1.53750 F137500400070 1081.10 1.59670 F137500400071 1087.50 1.88350 F137500400072 1088.20 2.21140 F137500400073 1093.40 2.01090 F137500400074 1093.50 2.03370 F137500400075 1098.20 2.40250 0.09560 F137500400076 1101.90 2.38420 F137500400077 1102.00 2.41610 F137500400078 1107.00 2.13370 F137500400079 1112.40 2.03340 F137500400080 1114.50 2.13810 F137500400081 1119.10 1.65080 F137500400082 1119.50 1.81930 F137500400083 1125.90 1.34560 0.03643 F137500400084 1126.30 1.50960 F137500400085 1127.00 1.02690 F137500400086 1127.70 1.28640 0.08652 F137500400087 1133.20 1.21350 F137500400088 1134.60 1.01770 F137500400089 1137.00 1.22710 F137500400090 1137.90 0.82181 0.04553 F137500400091 1138.60 1.12230 F137500400092 1140.00 0.89464 F137500400093 1140.50 1.14050 F137500400094 1141.80 0.86729 F137500400095 1151.50 0.97189 F137500400096 1153.50 1.00830 F137500400097 1160.50 0.79418 0.03188 F137500400098 1171.70 0.72116 0.04553 F137500400099 1194.50 0.78460 F137500400100 1198.40 0.82553 0.05464 F137500400101 1207.90 0.82085 0.04553 F137500400102 1229.10 0.98904 F137500400103 1232.70 0.91613 F137500400104 1244.10 0.95241 0.05464 F137500400105 ENDDATA 88 0 F137500400106 ENDSUBENT 105 0 F137500499999 SUBENT F1375005 20181207 F071F137500500001 BIB 5 8 F137500500002 REACTION (6-C-12(T,A)5-B-11,PAR,DA) F137500500003 DETECTOR (SIBAR) F137500500004 SAMPLE CH4 or CO2 gas target was used. The pressure was F137500500005 60 mm Hg. The exit window was sealed with a mica film F137500500006 with the thickness of 0.13 mg/cm2. F137500500007 ERR-ANALYS (DATA-ERR) Error from the graphic bars. No source of F137500500008 uncertainty is given. F137500500009 STATUS (CURVE) Figure 3 F137500500010 ENDBIB 8 0 F137500500011 COMMON 4 3 F137500500012 E-LVL ANG EN-ERR-DIG ERR-DIG F137500500013 MEV ADEG KEV MB/SR F137500500014 2.13 90. 1.35 0.00353 F137500500015 ENDCOMMON 3 0 F137500500016 DATA 3 28 F137500500017 EN DATA DATA-ERR F137500500018 KEV MB/SR MB/SR F137500500019 544.31 0.08317 F137500500020 568.99 0.12382 F137500500021 582.28 0.14640 F137500500022 595.45 0.11890 F137500500023 603.04 0.13246 F137500500024 621.96 0.13675 F137500500025 633.41 0.18213 F137500500026 650.56 0.23654 F137500500027 661.95 0.25460 F137500500028 669.45 0.22717 F137500500029 677.11 0.26805 F137500500030 686.55 0.26336 0.03188 F137500500031 699.85 0.29050 F137500500032 705.49 0.27677 F137500500033 709.21 0.24939 F137500500034 718.67 0.25382 F137500500035 726.25 0.25826 0.02279 F137500500036 758.36 0.24416 F137500500037 826.53 0.28876 0.02732 F137500500038 839.79 0.29769 F137500500039 843.60 0.31129 F137500500040 881.40 0.30167 F137500500041 957.24 0.38714 0.03188 F137500500042 968.59 0.39154 F137500500043 970.54 0.41428 F137500500044 1016.20 0.51384 0.03190 F137500500045 1089.00 1.72870 0.08652 F137500500046 1101.50 2.22940 0.10928 F137500500047 ENDDATA 30 0 F137500500048 ENDSUBENT 47 0 F137500599999 SUBENT F1375006 20181207 F071F137500600001 BIB 5 12 F137500600002 REACTION (6-C-12(T,A)5-B-11,PAR,DA) F137500600003 DETECTOR (SIBAR) A chamber with two semiconductor detectors F137500600004 was used for the measurements. One, mounted at 90 F137500600005 degr. to the tritium-ion beam, was used as a monitor. F137500600006 The other was rotated around the target in the angle F137500600007 range 0-155 degr. F137500600008 SAMPLE Solid carbon target was made by evaporating graphite F137500600009 in vacuum on a glass plate. The thickness was 15 to F137500600010 25 mu-g/cm2. F137500600011 ERR-ANALYS (DATA-ERR) Error from the graphic bars. No source of F137500600012 uncertainty is given. F137500600013 STATUS (CURVE) Figure 4a F137500600014 ENDBIB 12 0 F137500600015 COMMON 3 3 F137500600016 E-LVL ANG-ERR-D ERR-DIG F137500600017 MEV ADEG MB/SR F137500600018 0. 0.42 0.00130 F137500600019 ENDCOMMON 3 0 F137500600020 DATA 4 99 F137500600021 EN ANG-CM DATA-CM DATA-ERR F137500600022 KEV ADEG MB/SR MB/SR F137500600023 425. 26.93 0.01325 F137500600024 425. 32.13 0.01059 F137500600025 425. 42.52 0.01062 F137500600026 425. 53.66 0.02408 F137500600027 425. 63.68 0.02949 F137500600028 425. 74.07 0.04564 F137500600029 425. 84.46 0.07521 F137500600030 425. 94.48 0.09135 F137500600031 425. 104.50 0.09676 F137500600032 425. 114.15 0.12633 F137500600033 425. 123.80 0.14247 F137500600034 425. 133.45 0.14519 F137500600035 425. 142.72 0.16670 F137500600036 425. 152.00 0.18553 F137500600037 425. 156.46 0.18823 F137500600038 561. 38.06 0.14487 F137500600039 561. 43.26 0.14757 F137500600040 561. 54.02 0.14492 F137500600041 561. 64.41 0.16375 F137500600042 561. 74.80 0.19601 F137500600043 561. 85.19 0.25244 F137500600044 561. 94.46 0.33840 F137500600045 561. 105.59 0.39751 0.01880 F137500600046 561. 115.24 0.42439 0.02148 F137500600047 561. 124.52 0.49424 0.01880 F137500600048 561. 133.79 0.57752 F137500600049 561. 144.55 0.61783 0.02148 F137500600050 561. 152.71 0.68230 0.02148 F137500600051 561. 157.17 0.68769 0.02685 F137500600052 610. 38.05 0.31941 0.01611 F137500600053 610. 43.62 0.31406 0.02148 F137500600054 610. 54.75 0.34095 0.01611 F137500600055 610. 65.14 0.38395 0.01611 F137500600056 610. 75.16 0.44574 0.02148 F137500600057 610. 85.17 0.49411 0.01880 F137500600058 610. 95.56 0.56128 0.03760 F137500600059 610. 105.58 0.63918 0.02417 F137500600060 610. 115.60 0.69561 0.02685 F137500600061 610. 124.86 0.85407 0.03222 F137500600062 610. 134.14 0.98836 0.02417 F137500600063 610. 143.04 1.08510 0.03222 F137500600064 610. 152.31 1.23820 0.03759 F137500600065 610. 157.12 1.32950 0.04565 F137500600066 636. 22.10 0.14482 0.01880 F137500600067 636. 39.16 0.30599 F137500600068 636. 54.37 0.43493 0.01880 F137500600069 636. 64.76 0.54775 0.02148 F137500600070 636. 75.15 0.60149 0.02148 F137500600071 636. 85.53 0.69282 0.02148 F137500600072 636. 95.92 0.74119 0.02954 F137500600073 636. 105.19 0.88354 0.02954 F137500600074 636. 114.84 0.95339 0.02954 F137500600075 636. 124.49 0.95611 0.02954 F137500600076 636. 134.13 1.05010 0.03759 F137500600077 636. 143.41 1.08510 0.03222 F137500600078 636. 152.31 1.16030 0.03759 F137500600079 636. 157.13 1.22740 0.03222 F137500600080 662. 32.85 0.33282 0.02954 F137500600081 662. 43.61 0.47517 0.02685 F137500600082 662. 54.36 0.60410 0.02685 F137500600083 662. 65.12 0.74377 0.03222 F137500600084 662. 75.13 0.87270 0.03759 F137500600085 662. 79.95 0.93179 0.02417 F137500600086 662. 85.52 0.96940 0.03491 F137500600087 662. 90.34 0.99627 0.02417 F137500600088 662. 95.53 1.03930 0.04296 F137500600089 662. 105.92 1.08490 0.04296 F137500600090 662. 115.20 1.11450 0.04296 F137500600091 662. 124.84 1.17630 0.02148 F137500600092 662. 134.12 1.21930 0.04565 F137500600093 662. 143.40 1.24620 0.04565 F137500600094 662. 152.30 1.31600 0.04834 F137500600095 662. 157.49 1.39930 0.03759 F137500600096 688. 42.88 0.28720 F137500600097 688. 53.64 0.30067 F137500600098 688. 64.77 0.40274 0.01880 F137500600099 688. 74.78 0.56926 0.02685 F137500600100 688. 85.53 0.67671 0.01611 F137500600101 688. 95.92 0.75999 0.02148 F137500600102 688. 105.57 0.79493 0.02148 F137500600103 688. 114.85 0.78690 0.01611 F137500600104 688. 124.87 0.79768 0.02148 F137500600105 688. 134.15 0.72789 0.01880 F137500600106 688. 143.06 0.70912 0.02417 F137500600107 688. 152.71 0.63934 0.02148 F137500600108 688. 157.17 0.63398 0.02148 F137500600109 715. 43.99 0.27915 0.02417 F137500600110 715. 54.76 0.17446 F137500600111 715. 65.15 0.19867 0.01880 F137500600112 715. 75.54 0.32491 0.03222 F137500600113 715. 85.55 0.47800 0.02685 F137500600114 715. 95.93 0.58276 0.02417 F137500600115 715. 105.95 0.62039 0.01880 F137500600116 715. 115.60 0.65801 0.03222 F137500600117 715. 124.88 0.62314 0.02954 F137500600118 715. 134.90 0.60169 0.03222 F137500600119 715. 143.81 0.52653 0.02685 F137500600120 715. 153.10 0.42184 0.01611 F137500600121 715. 157.18 0.43259 0.02954 F137500600122 ENDDATA 101 0 F137500600123 ENDSUBENT 122 0 F137500699999 SUBENT F1375007 20181207 F071F137500700001 BIB 5 12 F137500700002 REACTION (6-C-12(T,A)5-B-11,PAR,DA) F137500700003 DETECTOR (SIBAR) A chamber with two semiconductor detectors F137500700004 was used for the measurements. One, mounted at 90 F137500700005 degr. to the tritium-ion beam, was used as a monitor. F137500700006 The other was rotated around the target in the angle F137500700007 range 0-155 degr. F137500700008 SAMPLE Solid carbon target was made by evaporating graphite F137500700009 in vacuum on a glass plate. The thickness was 15 to F137500700010 25 mu-g/cm2. F137500700011 ERR-ANALYS (DATA-ERR) Error from the graphic bars. No source of F137500700012 uncertainty is given. F137500700013 STATUS (CURVE) Figure 4b F137500700014 ENDBIB 12 0 F137500700015 COMMON 3 3 F137500700016 E-LVL ANG-ERR-D ERR-DIG F137500700017 MEV ADEG MB/SR F137500700018 0. 0.51 0.0207 F137500700019 ENDCOMMON 3 0 F137500700020 DATA 4 58 F137500700021 EN ANG-CM DATA-CM DATA-ERR F137500700022 KEV ADEG MB/SR MB/SR F137500700023 1012. 44.42 4.1856 0.1707 F137500700024 1012. 49.55 3.2247 0.1281 F137500700025 1012. 55.06 2.3917 0.1708 F137500700026 1012. 60.57 1.7935 F137500700027 1012. 65.72 1.4302 F137500700028 1012. 76.77 1.2583 F137500700029 1012. 86.36 1.6202 F137500700030 1012. 96.33 2.3236 F137500700031 1012. 106.30 2.8349 F137500700032 1012. 116.62 3.0046 F137500700033 1012. 121.04 2.8975 F137500700034 1012. 125.46 2.8970 F137500700035 1012. 135.03 2.4265 F137500700036 1012. 144.24 2.0628 F137500700037 1012. 153.06 1.4856 F137500700038 1012. 157.48 1.1650 F137500700039 1078. 44.82 5.0821 0.3202 F137500700040 1078. 55.07 2.7119 0.2348 F137500700041 1078. 66.10 1.7716 F137500700042 1078. 76.42 1.7279 F137500700043 1078. 86.75 2.1751 0.1281 F137500700044 1078. 97.09 3.1773 0.1708 F137500700045 1078. 107.07 3.9874 0.1921 F137500700046 1078. 116.67 4.7121 0.1281 F137500700047 1078. 125.90 5.0314 F137500700048 1078. 135.83 4.5608 0.1066 F137500700049 1078. 144.66 4.1117 0.1494 F137500700050 1078. 153.49 3.2998 0.1494 F137500700051 1078. 157.53 2.9365 0.1494 F137500700052 1110. 32.81 10.2480 0.7044 F137500700053 1110. 39.00 7.8147 0.5336 F137500700054 1110. 44.48 6.0853 0.4055 F137500700055 1110. 55.83 3.6936 0.2988 F137500700056 1110. 66.11 2.2199 F137500700057 1110. 76.44 2.4536 F137500700058 1110. 86.76 2.7728 0.1494 F137500700059 1110. 96.75 3.9030 0.1921 F137500700060 1110. 107.10 5.0973 0.2134 F137500700061 1110. 116.70 5.7153 0.1067 F137500700062 1110. 125.91 5.6290 0.1067 F137500700063 1110. 135.12 5.4360 0.1494 F137500700064 1110. 144.68 4.6240 0.1494 F137500700065 1110. 153.50 3.6840 0.1708 F137500700066 1110. 157.54 3.2781 0.2134 F137500700067 1143. 38.34 10.1840 1.2380 F137500700068 1143. 44.16 7.7074 0.5977 F137500700069 1143. 55.49 4.4193 0.4269 F137500700070 1143. 65.74 2.3266 F137500700071 1143. 76.44 2.6671 0.1494 F137500700072 1143. 86.79 3.4985 0.1494 F137500700073 1143. 96.77 4.5220 0.1708 F137500700074 1143. 107.49 5.8016 0.1921 F137500700075 1143. 116.36 6.6972 0.1708 F137500700076 1143. 125.96 7.1231 0.1281 F137500700077 1143. 135.16 6.7807 0.1067 F137500700078 1143. 144.36 6.3956 0.1707 F137500700079 1143. 153.54 5.1140 0.2562 F137500700080 1143. 157.94 4.4306 0.2988 F137500700081 ENDDATA 60 0 F137500700082 ENDSUBENT 81 0 F137500799999 SUBENT F1375008 20181207 F071F137500800001 BIB 5 12 F137500800002 REACTION (6-C-12(T,A)5-B-11,PAR,DA) F137500800003 DETECTOR (SIBAR) A chamber with two semiconductor detectors F137500800004 was used for the measurements. One, mounted at 90 F137500800005 degr. to the tritium-ion beam, was used as a monitor. F137500800006 The other was rotated around the target in the angle F137500800007 range 0-155 degr. F137500800008 SAMPLE Solid carbon target was made by evaporating graphite F137500800009 in vacuum on a glass plate. The thickness was 15 to F137500800010 25 mu-g/cm2. F137500800011 ERR-ANALYS (DATA-ERR) Error from the graphic bars. No source of F137500800012 uncertainty is given. F137500800013 STATUS (CURVE) Figure 4c F137500800014 ENDBIB 12 0 F137500800015 COMMON 3 3 F137500800016 E-LVL ANG-ERR-D ERR-DIG F137500800017 MEV ADEG MB/SR F137500800018 0. 0.39 0.00414 F137500800019 ENDCOMMON 3 0 F137500800020 DATA 4 56 F137500800021 EN ANG-CM DATA-CM DATA-ERR F137500800022 KEV ADEG MB/SR MB/SR F137500800023 771. 44.25 0.56708 F137500800024 771. 49.29 0.41690 F137500800025 771. 55.07 0.30415 F137500800026 771. 65.58 0.20718 F137500800027 771. 75.76 0.25476 F137500800028 771. 85.98 0.46830 F137500800029 771. 96.21 0.67112 0.03210 F137500800030 771. 106.03 0.73479 F137500800031 771. 115.83 0.71281 F137500800032 771. 125.26 0.65873 F137500800033 771. 134.32 0.56720 F137500800034 771. 143.37 0.49172 F137500800035 771. 152.42 0.37878 F137500800036 771. 157.13 0.32498 F137500800037 828. 38.27 1.30080 0.10169 F137500800038 828. 43.96 0.87223 0.05890 F137500800039 828. 54.76 0.48617 F137500800040 828. 65.26 0.39456 0.02674 F137500800041 828. 75.45 0.47426 0.03749 F137500800042 828. 86.06 0.74666 0.04818 F137500800043 828. 96.28 0.93878 0.03747 F137500800044 828. 105.74 1.01320 0.03745 F137500800045 828. 115.55 1.01800 0.04280 F137500800046 828. 124.96 0.90499 0.03747 F137500800047 828. 134.36 0.72779 0.03212 F137500800048 828. 144.13 0.59339 0.03212 F137500800049 828. 152.45 0.45908 0.03214 F137500800050 828. 157.15 0.40527 0.03747 F137500800051 888. 33.20 2.72510 0.27838 F137500800052 888. 38.81 1.96460 0.19271 F137500800053 888. 44.12 1.45040 0.10706 F137500800054 888. 55.23 0.90369 0.05890 F137500800055 888. 65.34 0.67827 0.04283 F137500800056 888. 75.90 0.79007 0.04816 F137500800057 888. 86.14 1.04110 0.06959 F137500800058 888. 96.39 1.34030 0.05353 F137500800059 888. 106.22 1.43070 0.05888 F137500800060 888. 116.03 1.46760 0.05886 F137500800061 888. 125.43 1.28500 0.06424 F137500800062 888. 134.80 1.03820 0.04283 F137500800063 888. 143.46 0.80756 0.06422 F137500800064 888. 152.84 0.57147 0.05888 F137500800065 888. 157.16 0.43204 0.05888 F137500800066 948. 44.09 2.69770 0.24089 F137500800067 948. 54.99 1.35870 0.16595 F137500800068 948. 65.40 0.88704 0.03745 F137500800069 948. 75.98 1.06840 0.04818 F137500800070 948. 86.95 1.34620 0.06422 F137500800071 948. 96.50 1.76850 0.06424 F137500800072 948. 106.01 1.99810 0.03747 F137500800073 948. 115.49 2.13140 0.04285 F137500800074 948. 125.26 2.01310 0.05353 F137500800075 948. 136.46 1.78760 0.05353 F137500800076 948. 143.97 1.37500 0.05888 F137500800077 948. 153.30 0.93546 0.06424 F137500800078 948. 157.24 0.74252 0.06422 F137500800079 ENDDATA 58 0 F137500800080 ENDSUBENT 79 0 F137500899999 SUBENT F1375009 20181207 F071F137500900001 BIB 3 3 F137500900002 REACTION (6-C-12(T,A)5-B-11,,SIG) F137500900003 STATUS (TABLE) Table from text. F137500900004 ERR-ANALYS (DATA-ERR) No source of uncertainty is given. F137500900005 ENDBIB 3 0 F137500900006 NOCOMMON 0 0 F137500900007 DATA 4 15 F137500900008 EN EN-ERR DATA DATA-ERR F137500900009 KEV KEV MB MB F137500900010 425. 8. 1.09 0.08 F137500900011 561. 9. 4.4 0.3 F137500900012 610. 10. 7.8 0.3 F137500900013 636. 10. 8.9 0.4 F137500900014 662. 10. 11.6 0.5 F137500900015 688. 10. 7.6 0.3 F137500900016 715. 12. 5.9 0.3 F137500900017 771. 13. 7.3 0.3 F137500900018 828. 14. 11.0 0.6 F137500900019 888. 15. 16.4 0.8 F137500900020 948. 16. 26.3 1.6 F137500900021 1012. 17. 36. 2. F137500900022 1078. 18. 49. 2. F137500900023 1110. 19. 63. 2. F137500900024 1143. 20. 78. 4. F137500900025 ENDDATA 17 0 F137500900026 ENDSUBENT 25 0 F137500999999 ENDENTRY 9 0 F137599999999