ENTRY A0413 20240911 A118A0413000 1 SUBENT A0413001 20240911 A118A0413001 1 BIB 6 12 A0413001 2 TITLE Low-energy cross sections for B-11(p,3alpha)* A0413001 3 AUTHOR (H.W.Becker, C.Rolfs, H.P.Trautvetter) A0413001 4 REFERENCE (J,ZP/A,327,341,1987) A0413001 5 INSTITUTE (2GERMST) A0413001 6 FACILITY (CCW,2GERMST) Proton beam. A0413001 7 (DYNAM,2GERMST) B-11 beam. A0413001 8 HISTORY (19890601C) A0413001 9 (20040921A) Correction according to new rules. Angular A0413001 10 distributions and elastic scattering were added. A0413001 11 (20050120U) Last checking has been done. A0413001 12 (20240911A) SD: Corrections in all Subents. Several A0413001 13 Subents were merged. Subent 011 added. A0413001 14 ENDBIB 12 0 A0413001 15 NOCOMMON 0 0 A0413001 16 ENDSUBENT 15 0 A041300199999 SUBENT A0413002 20240911 A118A0413002 1 BIB 8 28 A0413002 2 REACTION (5-B-11(P,A)4-BE-8,PAR,SIG,,SFC) A0413002 3 SAMPLE All targets were fabricated by evaporation of natural A0413002 4 B-11 (81.5% B-11) onto 0.1 mm Ta backings. The targets A0413002 5 ranged in thickness from 2 to 100 ug/cm2. A0413002 6 DETECTOR (SIBAR) Silicon surface-barrier detectors (with an A0413002 7 active area of 300 mm2) were positioned at 90. degr. A0413002 8 and 135. degr. to the beam direction in close geometry.A0413002 9 The alpha-particles were observed with Si detectors A0413002 10 positioned at 40., 60., 90., 120., 140., and 160. degr.A0413002 11 (placed at a distance of 6 to 16 cm from the target A0413002 12 and collimated by 2 to 3 mm diameter apertures in A0413002 13 front of the detectors). A0413002 14 MISC-COL (MISC) Cross sections data were calculated by A0413002 15 compiler using formulae at page 342. A0413002 16 ERR-ANALYS (ERR-1) The errors includes all experimental A0413002 17 uncertainties excluding error due to normalization. A0413002 18 (ERR-2)Error due to the cross section normaliation. A0413002 19 COMMENT -By authors. Due to the thick targets used, data A0413002 20 obtained near 150-keV resonance do not represent cross A0413002 21 section values and have therefore been omitted. A0413002 22 STATUS (TABLE,,H.W.Becker+,J,ZP/A,327,341,1987) Tbl.2 A0413002 23 (COREL,A0413004) Data measured via 1H(11B,alpha)8Be A0413002 24 with a gas target A0413002 25 HISTORY (20240911A) SD: ERR-T -> ERR-1. ERR-ANALYS, STATUS A0413002 26 updated. Data from Subent 003 were added. Data from A0413002 27 REACTION (S) code were moved in col. MISC (data were A0413002 28 not experimental). E-LVL -> LVL-NUMB (no information A0413002 29 in the text about energy level). A0413002 30 ENDBIB 28 0 A0413002 31 COMMON 1 3 A0413002 32 ERR-2 A0413002 33 PER-CENT A0413002 34 6. A0413002 35 ENDCOMMON 3 0 A0413002 36 DATA 6 63 A0413002 37 LVL-NUMB EN-CM DATA ERR-1 MISC MISC-ERR A0413002 38 NO-DIM KEV B*MEV B*MEV B B A0413002 39 0. 51.3 2.9 0.3 4.35E-08 4.50E-09A0413002 40 0. 59.6 2.57 0.15 1.51E-07 9.00E-09A0413002 41 0. 67.8 2.12 0.11 3.69E-07 1.90E-08A0413002 42 0. 72.6 2.8 0.4 8.42E-07 1.20E-07A0413002 43 0. 77.6 2.12 0.14 1.06E-06 7.00E-08A0413002 44 0. 84.3 2.34 0.18 2.16E-06 1.70E-07A0413002 45 0. 93.1 2.4 0.2 4.43E-06 3.70E-07A0413002 46 0. 102.1 2.3 0.2 7.81E-06 6.80E-07A0413002 47 0. 111.2 2.62 0.13 1.52E-05 8.00E-07A0413002 48 0. 120.3 2.82 0.14 2.62E-05 1.30E-06A0413002 49 0. 129.3 3.67 0.18 5.15E-05 2.50E-06A0413002 50 0. 135.9 5. 0.2 9.26E-05 3.70E-06A0413002 51 0. 162.9 5.2 0.3 2.45E-04 1.40E-05A0413002 52 0. 171.9 3.2 0.2 1.96E-04 1.20E-05A0413002 53 0. 181. 2.54 0.13 1.97E-04 1.00E-05A0413002 54 0. 190. 2.16 0.11 2.09E-04 1.10E-05A0413002 55 0. 199. 2.08 0.1 2.47E-04 1.20E-05A0413002 56 0. 208. 1.87 0.09 2.68E-04 1.30E-05A0413002 57 0. 221. 1.91 0.16 3.51E-04 2.90E-05A0413002 58 0. 235. 2.1 0.11 4.93E-04 2.60E-05A0413002 59 0. 244. 1.98 0.1 5.38E-04 2.70E-05A0413002 60 0. 253. 1.98 0.1 6.16E-04 3.10E-05A0413002 61 0. 266. 1.9 0.2 7.11E-04 7.50E-05A0413002 62 0. 284. 1.77 0.13 8.34E-04 6.10E-05A0413002 63 0. 302. 1.79 0.09 1.04E-03 5.00E-05A0413002 64 0. 316. 1.79 0.09 1.21E-03 6.00E-05A0413002 65 0. 325. 1.77 0.09 1.30E-03 7.00E-05A0413002 66 1. 21.8 380. 90. 1.82E-10 4.30E-11A0413002 67 1. 26.1 230. 16. 1.47E-09 1.00E-10A0413002 68 1. 30.3 213. 14. 9.74E-09 6.40E-10A0413002 69 1. 34.6 210. 11. 4.85E-08 2.50E-09A0413002 70 1. 38.8 237. 12. 2.03E-07 1.00E-08A0413002 71 1. 43. 207. 11. 5.35E-07 2.80E-08A0413002 72 1. 45.4 192. 14. 8.68E-07 6.30E-08A0413002 73 1. 51.3 213. 11. 3.20E-06 1.70E-07A0413002 74 1. 54.5 187. 10. 4.94E-06 2.60E-07A0413002 75 1. 59.6 209. 11. 1.23E-05 6.00E-07A0413002 76 1. 63.6 202. 11. 2.07E-05 1.10E-06A0413002 77 1. 67.8 205. 10. 3.57E-05 1.70E-06A0413002 78 1. 72.6 201. 11. 6.05E-05 3.30E-06A0413002 79 1. 77.6 218. 11. 1.09E-04 6.00E-06A0413002 80 1. 84.3 213. 11. 1.96E-04 1.00E-05A0413002 81 1. 93.1 235. 14. 4.34E-04 2.60E-05A0413002 82 1. 102.1 234. 17. 7.95E-04 5.80E-05A0413002 83 1. 111.2 266. 20. 1.54E-03 1.20E-04A0413002 84 1. 120.3 255. 13. 2.37E-03 1.20E-04A0413002 85 1. 129.3 290. 30. 4.08E-03 4.20E-04A0413002 86 1. 135.9 328. 16. 6.07E-03 3.00E-04A0413002 87 1. 162.9 392. 20. 1.85E-02 9.00E-04A0413002 88 1. 171.9 304. 15. 1.86E-02 9.00E-04A0413002 89 1. 181. 284. 14. 2.21E-02 1.10E-03A0413002 90 1. 190. 262. 13. 2.54E-02 1.30E-03A0413002 91 1. 199. 265. 13. 3.13E-02 1.50E-03A0413002 92 1. 208. 241. 12. 3.45E-02 1.70E-03A0413002 93 1. 221. 266. 13. 4.89E-02 2.40E-03A0413002 94 1. 235. 270. 13. 6.34E-02 3.10E-03A0413002 95 1. 244. 269. 13. 7.30E-02 3.50E-03A0413002 96 1. 253. 273. 13. 8.49E-02 4.00E-03A0413002 97 1. 266. 271. 13. 1.01E-01 4.79E-03A0413002 98 1. 284. 282. 15. 1.32E-01 6.91E-03A0413002 99 1. 302. 280. 14. 1.61E-01 8.03E-03A0413002 100 1. 316. 290. 15. 1.95E-01 1.00E-02A0413002 101 1. 325. 315. 16. 2.32E-01 1.20E-02A0413002 102 ENDDATA 65 0 A0413002 103 ENDSUBENT 102 0 A041300299999 NOSUBENT A0413003 20240911 A118A0413003 1 SUBENT A0413004 20240911 A118A0413004 1 BIB 10 32 A0413004 2 REACTION ((1-H-1(5-B-11,A)4-BE-8,PAR,SIG,,SFC)= A0413004 3 (5-B-11(P,A)4-BE-8,PAR,SIG,,SFC)) A0413004 4 SAMPLE The B-11 heavy ion beam was bombarded onto a hydrogen A0413004 5 gas target of the quasi-point supersonic jet system A0413004 6 type. A0413004 7 ANALYSIS The absolute cross section was determined at low A0413004 8 energies relative to the 11B+p elastic scattering crossA0413004 9 section A0413004 10 REL-REF (I,,H.W.Becker+,J,NIM,198,277,1982) - technical detailsA0413004 11 and properties of the experim. system A0413004 12 (M,,A.Redder+,J,ZP/A,305,325,1982) Details of gas A0413004 13 target. A0413004 14 MISC-COL (MISC) Cross sections data were calculated by A0413004 15 compiler using formulae at page 342. A0413004 16 FLAG (1.) Analysis of the data near the 150-keV resonance isA0413004 17 not certain. (Comment by authors). A0413004 18 ERR-ANALYS (ERR-1) The errors includes all experimental A0413004 19 uncertainties excluding error due to normalization. A0413004 20 (ERR-2)Error due to the cross section normalization. A0413004 21 COMMENT -By authors. Due to the thick targets used, data A0413004 22 obtained near 150-keV resonance do not represent cross A0413004 23 section values and have therefore been omitted. A0413004 24 STATUS (TABLE,,H.W.Becker+,J,ZP/A,327,341,1987) Tbl.2 A0413004 25 (DEP,A0413011) These values have been used as the A0413004 26 standards for Tbl.2 A0413004 27 (COREL,A0413002) Data measured via 11B(p,alpha)8Be A0413004 28 with a solid target A0413004 29 HISTORY (20240911A) SD: ERR-T -> ERR-1. ERR-ANALYS, STATUS A0413004 30 updated. Data from Subent 003 were added. Data from A0413004 31 REACTION (S) code were moved in col. MISC (data were A0413004 32 not experimental.). E-LVL -> LVL-NUMB (no information A0413004 33 in the text about energy level). A0413004 34 ENDBIB 32 0 A0413004 35 COMMON 1 3 A0413004 36 ERR-2 A0413004 37 PER-CENT A0413004 38 6. A0413004 39 ENDCOMMON 3 0 A0413004 40 DATA 7 60 A0413004 41 LVL-NUMB EN-CM DATA ERR-1 MISC MISC-ERR A0413004 42 FLAG A0413004 43 NO-DIM KEV B*EV B*EV B B A0413004 44 NO-DIM A0413004 45 0. 140. 11.9 0.6 2.59E-04 1.30E-05A0413004 46 A0413004 47 0. 143. 23. 1.1 5.60E-04 2.70E-05A0413004 48 A0413004 49 0. 145. 42. 2. 1.10E-03 5.00E-05A0413004 50 A0413004 51 0. 146.5 64. 3. 1.77E-03 8.00E-05A0413004 52 A0413004 53 0. 148. 98. 5. 2.85E-03 1.50E-04A0413004 54 A0413004 55 0. 150. 76. 4. 2.37E-03 1.20E-04A0413004 56 A0413004 57 0. 155. 16.7 0.8 6.16E-04 3.00E-05A0413004 58 A0413004 59 0. 160. 6.4 0.3 2.76E-04 1.30E-05A0413004 60 A0413004 61 0. 170. 4.3 0.2 2.49E-04 1.20E-05A0413004 62 A0413004 63 0. 200. 1.95 0.1 2.36E-04 1.20E-05A0413004 64 A0413004 65 0. 230. 1.96 0.14 4.23E-04 3.00E-05A0413004 66 A0413004 67 0. 260. 1.83 0.11 6.30E-04 3.80E-05A0413004 68 A0413004 69 0. 292. 1.91 0.1 9.90E-04 5.20E-05A0413004 70 A0413004 71 0. 300. 1.82 0.09 1.03E-03 5.00E-05A0413004 72 A0413004 73 0. 350. 1.78 0.09 1.65E-03 8.00E-05A0413004 74 A0413004 75 0. 400. 1.64 0.09 2.23E-03 1.20E-04A0413004 76 A0413004 77 0. 450. 1.56 0.08 2.90E-03 1.50E-04A0413004 78 A0413004 79 0. 500. 1.38 0.08 3.32E-03 1.90E-04A0413004 80 A0413004 81 0. 550. 1.11 0.12 3.32E-03 3.60E-04A0413004 82 A0413004 83 0. 600. 1.35 0.08 4.87E-03 2.90E-04A0413004 84 A0413004 85 0. 642. 1.14 0.06 4.71E-03 2.50E-04A0413004 86 A0413004 87 0. 700. 1.12 0.06 5.46E-03 2.90E-04A0413004 88 A0413004 89 0. 750. 1.29 0.08 7.11E-03 4.40E-04A0413004 90 A0413004 91 0. 800. 1. 0.06 6.15E-03 3.70E-04A0413004 92 A0413004 93 0. 850. 0.94 0.05 6.38E-03 3.40E-04A0413004 94 A0413004 95 0. 900. 0.91 0.05 5.48E-03 3.00E-04A0413004 96 A0413004 97 0. 950. 0.74 0.05 5.94E-03 4.00E-04A0413004 98 A0413004 99 0. 1000. 0.67 0.06 5.78E-03 3.50E-04A0413004 100 A0413004 101 0. 1050. 0.67 0.04 6.17E-03 3.70E-04A0413004 102 A0413004 103 0. 1100. 0.56 0.03 5.79E-03 3.10E-04A0413004 104 A0413004 105 1. 140. 560. 30. 1.20E-02 6.43E-04A0413004 106 A0413004 107 1. 143. 940. 50. 2.30E-02 1.22E-03A0413004 108 1. A0413004 109 1. 145. 1620. 80. 4.20E-02 2.07E-03A0413004 110 1. A0413004 111 1. 146.5 2390. 120. 6.60E-02 3.31E-03A0413004 112 1. A0413004 113 1. 148. 3290. 160. 9.60E-02 4.67E-03A0413004 114 1. A0413004 115 1. 150. 2600. 130. 8.10E-02 4.05E-03A0413004 116 1. A0413004 117 1. 155. 463. 23. 1.70E-02 8.44E-04A0413004 118 A0413004 119 1. 160. 316. 16. 1.40E-02 7.09E-04A0413004 120 A0413004 121 1. 170. 360. 18. 2.10E-02 1.05E-03A0413004 122 A0413004 123 1. 200. 253. 13. 3.10E-02 1.59E-03A0413004 124 A0413004 125 1. 230. 263. 13. 5.70E-02 2.86E-03A0413004 126 A0413004 127 1. 260. 272. 14. 9.40E-02 4.84E-03A0413004 128 A0413004 129 1. 292. 271. 14. 1.41E-01 7.28E-03A0413004 130 A0413004 131 1. 300. 290. 15. 1.65E-01 8.53E-03A0413004 132 A0413004 133 1. 350. 293. 15. 2.71E-01 1.39E-02A0413004 134 A0413004 135 1. 400. 332. 17. 4.52E-01 2.31E-02A0413004 136 A0413004 137 1. 450. 361. 18. 6.72E-01 3.40E-02A0413004 138 A0413004 139 1. 500. 377. 19. 9.08E-01 4.60E-02A0413004 140 A0413004 141 1. 550. 357. 18. 1.07E+00 5.40E-02A0413004 142 A0413004 143 1. 600. 340. 17. 1.23E+00 6.10E-02A0413004 144 A0413004 145 1. 642. 239. 12. 9.88E-01 4.90E-02A0413004 146 A0413004 147 1. 700. 135. 7. 6.58E-01 3.40E-02A0413004 148 A0413004 149 1. 750. 68. 4. 3.75E-01 2.20E-02A0413004 150 A0413004 151 1. 800. 55. 3. 3.38E-01 1.80E-02A0413004 152 A0413004 153 1. 850. 42. 2. 2.85E-01 1.40E-02A0413004 154 A0413004 155 1. 900. 35. 2. 2.59E-01 1.50E-02A0413004 156 A0413004 157 1. 950. 30. 2. 2.41E-01 1.60E-02A0413004 158 A0413004 159 1. 1000. 26. 1. 2.24E-01 8.62E-03A0413004 160 A0413004 161 1. 1050. 26. 1. 2.40E-01 9.23E-03A0413004 162 A0413004 163 1. 1100. 24. 1. 2.35E-01 9.79E-03A0413004 164 A0413004 165 ENDDATA 124 0 A0413004 166 ENDSUBENT 165 0 A041300499999 NOSUBENT A0413005 20240911 A118A0413005 1 SUBENT A0413006 20240911 A118A0413006 1 BIB 5 10 A0413006 2 REACTION (5-B-11(P,EL)5-B-11,,DA,,RTH) A0413006 3 SAMPLE Hydrogen - argon gas mixture. A0413006 4 COMMENT -By compiler. Data point density is very high about A0413006 5 150-keV region. Therefore some data-points could be A0413006 6 missed. A0413006 7 -By authors. The data have been used in the A0413006 8 normalization of the 11-B(P,3alpha) reaction yields. A0413006 9 Boron-11 beam was used in the experiment. A0413006 10 STATUS (CURVE,,H.W.Becker+,J,ZP/A,327,341,1987)) Fig.9 A0413006 11 HISTORY (20240911U) SD: BIB updated. A0413006 12 ENDBIB 10 0 A0413006 13 COMMON 3 3 A0413006 14 ANG EN-ERR-DIG ERR-DIG A0413006 15 ADEG MEV NO-DIM A0413006 16 37.5 4.E-03 1.E-02 A0413006 17 ENDCOMMON 3 0 A0413006 18 DATA 2 27 A0413006 19 EN-CM DATA A0413006 20 MEV NO-DIM A0413006 21 0.121 0.992 A0413006 22 0.131 1.006 A0413006 23 0.134 0.986 A0413006 24 0.145 1.007 A0413006 25 0.156 1.049 A0413006 26 0.159 0.974 A0413006 27 0.172 1.022 A0413006 28 0.194 1.037 A0413006 29 0.228 0.998 A0413006 30 0.258 0.993 A0413006 31 0.299 0.975 A0413006 32 0.348 1.019 A0413006 33 0.400 1.035 A0413006 34 0.452 0.868 A0413006 35 0.499 0.769 A0413006 36 0.548 0.812 A0413006 37 0.596 0.985 A0413006 38 0.640 1.212 A0413006 39 0.704 1.502 A0413006 40 0.751 1.702 A0413006 41 0.800 1.718 A0413006 42 0.849 1.762 A0413006 43 0.900 1.874 A0413006 44 0.951 1.774 A0413006 45 1.000 1.831 A0413006 46 1.049 1.834 A0413006 47 1.105 1.763 A0413006 48 ENDDATA 29 0 A0413006 49 ENDSUBENT 48 0 A041300699999 SUBENT A0413007 20240911 A118A0413007 1 BIB 5 11 A0413007 2 REACTION ((5-B-11(P,A)4-BE-8,PAR,DA,,REL)= A0413007 3 (1-H-1(5-B-11,A)4-BE-8,PAR,DA,,REL)) A0413007 4 COMMENT -By authors. Angular distributions were obtained using A0413007 5 a B-11 heavy ion beam incident on a hydrogen gas targetA0413007 6 as well as a proton beam incident on a solid-backed A0413007 7 11-B target. A0413007 8 ERR-ANALYS (ERR-S) Statistical uncertainty A0413007 9 STATUS (CURVE,,H.W.Becker+,J,ZP/A,327,341,1987)) Figs 10,11 A0413007 10 HISTORY (20240911A) SD: BIB updated. Data from Subent 009 addedA0413007 11 E-LVL -> LVL-NUMB (no information in the text about A0413007 12 energy level). Data were re-digitized. DATA-ERR->ERR-S.A0413007 13 ENDBIB 11 0 A0413007 14 COMMON 2 3 A0413007 15 ANG-ERR-D ERR-DIG A0413007 16 ADEG PER-CENT A0413007 17 0.3 0.6 A0413007 18 ENDCOMMON 3 0 A0413007 19 DATA 5 75 A0413007 20 LVL-NUMB EN-CM ANG-CM DATA-CM ERR-S A0413007 21 NO-DIM KEV ADEG ARB-UNITS PER-CENT A0413007 22 0. 140. 27.5 7.718E+00 1.770E+00 A0413007 23 0. 140. 46.4 1.346E+01 3.350E+00 A0413007 24 0. 140. 64.7 1.263E+01 2.677E+00 A0413007 25 0. 140. 89.9 2.347E+01 5.266E+00 A0413007 26 0. 140. 113.8 2.841E+01 A0413007 27 0. 140. 145.9 3.028E+01 A0413007 28 0. 140. 157.8 3.439E+01 A0413007 29 0. 148. 27.8 2.593E+00 1.701E-01 A0413007 30 0. 148. 47.3 2.396E+00 1.775E-01 A0413007 31 0. 148. 65.5 1.918E+00 1.881E-01 A0413007 32 0. 148. 90.6 1.598E+00 2.022E-01 A0413007 33 0. 148. 113.8 2.303E+00 A0413007 34 0. 148. 145.8 2.946E+00 A0413007 35 0. 148. 157.1 2.743E+00 A0413007 36 0. 160. 27.7 3.783E+01 A0413007 37 0. 160. 46.5 3.911E+01 A0413007 38 0. 160. 65.3 2.942E+01 3.986E+00 A0413007 39 0. 160. 91.1 2.286E+01 3.935E+00 A0413007 40 0. 160. 113.7 1.253E+01 A0413007 41 0. 160. 146.4 5.675E+00 9.767E-01 A0413007 42 0. 160. 157.8 4.201E+00 9.631E-01 A0413007 43 0. 300. 32.2 8.361E+00 A0413007 44 0. 300. 53.0 9.492E+00 1.281E+00 A0413007 45 0. 300. 73.2 8.366E+00 1.280E+00 A0413007 46 0. 300. 99.7 9.498E+00 1.806E+00 A0413007 47 0. 300. 122.4 7.612E+00 A0413007 48 0. 300. 152.7 5.549E+00 7.489E-01 A0413007 49 0. 300. 163.4 6.299E+00 A0413007 50 0. 642. 36.1 2.247E+00 1.458E-01 A0413007 51 0. 642. 60.0 3.517E+00 2.282E-01 A0413007 52 0. 642. 82.0 4.280E+00 2.777E-01 A0413007 53 0. 642. 111.5 4.741E+00 3.876E-01 A0413007 54 0. 642. 135.4 3.865E+00 2.833E-01 A0413007 55 0. 642. 168.8 2.735E+00 2.942E-01 A0413007 56 0. 1100. 40.7 1.776E+00 1.302E-01 A0413007 57 0. 1100. 66.3 3.690E+00 2.395E-01 A0413007 58 0. 1100. 91.3 6.105E+00 3.961E-01 A0413007 59 0. 1100. 124.6 6.660E+00 6.938E-01 A0413007 60 0. 1100. 148.4 4.462E+00 4.029E-01 A0413007 61 0. 1100. 173.6 2.019E+00 5.976E-01 A0413007 62 1. 140. 30.0 1.138E+01 A0413007 63 1. 140. 50.2 7.178E+00 A0413007 64 1. 140. 69.1 1.235E+01 A0413007 65 1. 140. 95.5 1.072E+01 A0413007 66 1. 140. 118.9 9.153E+00 A0413007 67 1. 140. 149.7 8.742E+00 A0413007 68 1. 140. 160.4 1.076E+01 A0413007 69 1. 148. 31.4 7.928E+00 A0413007 70 1. 148. 51.5 1.072E+01 A0413007 71 1. 148. 71.1 8.867E+00 A0413007 72 1. 148. 97.0 9.014E+00 A0413007 73 1. 148. 120.9 5.968E+00 A0413007 74 1. 148. 151.2 4.559E+00 A0413007 75 1. 148. 161.9 4.488E+00 A0413007 76 1. 160. 30.6 1.250E+01 A0413007 77 1. 160. 50.7 1.173E+01 A0413007 78 1. 160. 69.6 1.270E+01 A0413007 79 1. 160. 96.0 1.192E+01 A0413007 80 1. 160. 119.2 8.820E+00 A0413007 81 1. 160. 149.4 5.932E+00 A0413007 82 1. 160. 160.1 6.954E+00 A0413007 83 1. 300. 34.9 1.161E+01 A0413007 84 1. 300. 56.5 1.340E+01 A0413007 85 1. 300. 77.4 1.384E+01 A0413007 86 1. 300. 105.9 1.454E+01 A0413007 87 1. 300. 128.8 1.302E+01 A0413007 88 1. 300. 166.8 1.244E+01 A0413007 89 1. 642. 40.4 7.353E+00 A0413007 90 1. 642. 65.0 8.347E+00 A0413007 91 1. 642. 89.6 7.485E+00 A0413007 92 1. 642. 121.8 8.107E+00 A0413007 93 1. 1100. 44.2 1.805E+01 A0413007 94 1. 1100. 72.5 2.326E+01 A0413007 95 1. 1100. 100.8 1.958E+01 A0413007 96 1. 1100. 141.7 1.147E+01 A0413007 97 ENDDATA 77 0 A0413007 98 ENDSUBENT 97 0 A041300799999 SUBENT A0413008 20240911 A118A0413008 1 BIB 5 11 A0413008 2 REACTION ((5-B-11(P,A)4-BE-8,PAR,DA,,LEG/RS)= A0413008 3 (1-H-1(5-B-11,A)4-BE-8,PAR,DA,,LEG/RS)) A0413008 4 COMMENT -By authors. Angular distributions were obtained using A0413008 5 a B-11 heavy ion beam incident on a hydrogen gas targetA0413008 6 as well as a proton beam incident on a solid-backed A0413008 7 11-B target. A0413008 8 ERR-ANALYS (DATA-ERR) No information about source of uncertainty A0413008 9 STATUS (CURVE,,H.W.Becker+,J,ZP/A,327,341,1987)) Figs 10,11 A0413008 10 HISTORY (20240911A) SD: BIB updated. Data from Subent 010 addedA0413008 11 E-LVL -> LVL-NUMB (no information in the text about A0413008 12 energy level). Data were re-digitized. A0413008 13 ENDBIB 11 0 A0413008 14 COMMON 2 3 A0413008 15 EN-ERR-DIG ERR-DIG A0413008 16 KEV PER-CENT A0413008 17 0.7 0.0065 A0413008 18 ENDCOMMON 3 0 A0413008 19 DATA 5 164 A0413008 20 LVL-NUMB NUMBER EN-CM DATA-CM DATA-ERR A0413008 21 NO-DIM NO-DIM KEV NO-DIM NO-DIM A0413008 22 0. 1. 117.7 -0.8704 A0413008 23 0. 1. 119.1 -0.4867 A0413008 24 0. 1. 126.1 -0.1653 0.1452 A0413008 25 0. 1. 131.7 -0.3831 0.1556 A0413008 26 0. 1. 137.3 -0.6009 0.5600 A0413008 27 0. 1. 142.8 -0.6943 A0413008 28 0. 1. 145.7 -0.2587 A0413008 29 0. 1. 147.0 -0.9639 0.3422 A0413008 30 0. 1. 147.1 -0.1861 A0413008 31 0. 1. 148.5 -0.0617 A0413008 32 0. 1. 152.7 0.1872 A0413008 33 0. 1. 155.6 0.5916 A0413008 34 0. 1. 161.2 0.8819 A0413008 35 0. 1. 171.0 0.9855 A0413008 36 0. 1. 179.3 0.5396 0.4252 A0413008 37 0. 1. 184.9 0.8195 0.0933 A0413008 38 0. 1. 201.7 0.7053 A0413008 39 0. 1. 208.7 0.7883 0.1348 A0413008 40 0. 1. 232.3 0.3007 0.0726 A0413008 41 0. 1. 236.6 0.5392 0.1141 A0413008 42 0. 1. 261.6 0.1865 0.0622 A0413008 43 0. 1. 268.6 0.0827 0.0622 A0413008 44 0. 1. 282.6 0.1863 0.1141 A0413008 45 0. 1. 292.4 -0.0004 A0413008 46 0. 1. 293.7 -0.1663 0.2178 A0413008 47 0. 1. 302.1 0.1447 0.0519 A0413008 48 0. 1. 316.1 0.0720 0.0726 A0413008 49 0. 1. 352.4 0.0718 0.0519 A0413008 50 0. 1. 401.3 -0.0011 0.0622 A0413008 51 0. 1. 452.9 -0.0429 A0413008 52 0. 1. 503.2 -0.1366 A0413008 53 0. 1. 552.1 -0.1161 0.1141 A0413008 54 0. 1. 601.0 -0.2202 A0413008 55 0. 1. 642.8 -0.2412 A0413008 56 0. 1. 701.5 -0.3556 A0413008 57 0. 1. 750.4 -0.1278 0.1659 A0413008 58 0. 1. 800.6 -0.3251 0.0622 A0413008 59 0. 1. 850.9 -0.5225 A0413008 60 0. 1. 901.2 -0.4917 0.0622 A0413008 61 0. 1. 948.6 -0.5231 0.0726 A0413008 62 0. 1. 1000.3 -0.5442 0.0518 A0413008 63 0. 1. 1049.2 -0.5860 0.0726 A0413008 64 0. 1. 1099.5 -0.4826 A0413008 65 0. 2. 120.3 -0.1629 0.1746 A0413008 66 0. 2. 121.9 0.5149 0.2259 A0413008 67 0. 2. 130.1 -0.0090 A0413008 68 0. 2. 131.4 -0.1528 0.1643 A0413008 69 0. 2. 142.7 -0.0092 A0413008 70 0. 2. 146.8 -0.2660 0.1849 A0413008 71 0. 2. 149.7 0.3091 A0413008 72 0. 2. 159.4 -0.0505 0.1027 A0413008 73 0. 2. 166.5 0.2062 0.1541 A0413008 74 0. 2. 173.4 0.0006 A0413008 75 0. 2. 181.8 -0.0406 A0413008 76 0. 2. 187.4 0.1339 0.1541 A0413008 77 0. 2. 202.7 0.0002 A0413008 78 0. 2. 212.5 -0.0821 0.0719 A0413008 79 0. 2. 230.6 -0.3083 0.1130 A0413008 80 0. 2. 237.6 -0.2160 0.1335 A0413008 81 0. 2. 262.7 -0.4115 0.0719 A0413008 82 0. 2. 265.6 -0.0829 0.1130 A0413008 83 0. 2. 280.9 -0.1345 0.1541 A0413008 84 0. 2. 293.4 -0.3811 0.0924 A0413008 85 0. 2. 293.5 0.0913 0.1232 A0413008 86 0. 2. 301.9 -0.1862 0.0822 A0413008 87 0. 2. 310.2 -0.1452 0.0924 A0413008 88 0. 2. 352.1 -0.1972 0.0616 A0413008 89 0. 2. 402.4 -0.3109 0.0924 A0413008 90 0. 2. 454.1 -0.3220 A0413008 91 0. 2. 502.9 -0.3432 0.0719 A0413008 92 0. 2. 553.2 -0.3029 0.1746 A0413008 93 0. 2. 602.1 -0.3550 0.0513 A0413008 94 0. 2. 644.0 -0.4891 0.0514 A0413008 95 0. 2. 701.3 -0.3976 0.0719 A0413008 96 0. 2. 751.6 -0.2546 0.2054 A0413008 97 0. 2. 801.8 -0.4915 0.0924 A0413008 98 0. 2. 850.7 -0.5333 0.0616 A0413008 99 0. 2. 901.0 -0.4930 0.0822 A0413008 100 0. 2. 951.3 -0.4938 0.1027 A0413008 101 0. 2. 1001.5 -0.6486 0.0924 A0413008 102 0. 2. 1050.4 -0.6698 0.0924 A0413008 103 0. 2. 1099.3 -0.7014 0.0616 A0413008 104 1. 1. 110.1 0.0002 0.0556 A0413008 105 1. 1. 122.7 -0.1596 A0413008 106 1. 1. 131.1 -0.1873 0.1597 A0413008 107 1. 1. 145.1 0.2572 A0413008 108 1. 1. 149.3 0.2988 A0413008 109 1. 1. 152.0 0.4030 A0413008 110 1. 1. 161.8 0.3058 A0413008 111 1. 1. 167.4 0.5002 0.2083 A0413008 112 1. 1. 171.6 0.1461 A0413008 113 1. 1. 180.0 0.2155 0.0833 A0413008 114 1. 1. 194.0 0.2225 0.0833 A0413008 115 1. 1. 202.4 -0.0414 A0413008 116 1. 1. 210.7 0.0628 0.0694 A0413008 117 1. 1. 231.7 -0.0622 A0413008 118 1. 1. 241.5 0.0003 0.0556 A0413008 119 1. 1. 254.1 -0.0483 0.0347 A0413008 120 1. 1. 262.4 -0.0830 A0413008 121 1. 1. 270.8 -0.0482 0.0486 A0413008 122 1. 1. 283.4 0.0004 0.0556 A0413008 123 1. 1. 293.2 -0.0551 A0413008 124 1. 1. 296.0 -0.0829 0.0625 A0413008 125 1. 1. 301.6 -0.0551 A0413008 126 1. 1. 311.3 0.0004 0.0486 A0413008 127 1. 1. 351.9 -0.0967 A0413008 128 1. 1. 403.6 -0.0203 A0413008 129 1. 1. 452.5 -0.0341 A0413008 130 1. 1. 502.8 -0.0549 A0413008 131 1. 1. 553.0 -0.0617 A0413008 132 1. 1. 600.6 -0.0756 A0413008 133 1. 1. 645.3 -0.0338 A0413008 134 1. 1. 702.5 0.0496 A0413008 135 1. 1. 751.4 0.0635 A0413008 136 1. 1. 798.9 0.0428 A0413008 137 1. 1. 850.6 0.0706 A0413008 138 1. 1. 900.9 0.1263 A0413008 139 1. 1. 949.8 0.0499 A0413008 140 1. 1. 998.7 0.1194 A0413008 141 1. 1. 1047.6 0.0223 A0413008 142 1. 1. 1099.3 0.2099 A0413008 143 1. 2. 117.1 -0.0796 0.0759 A0413008 144 1. 2. 125.4 -0.2728 0.1379 A0413008 145 1. 2. 128.3 0.0720 0.0690 A0413008 146 1. 2. 135.3 -0.0109 0.0828 A0413008 147 1. 2. 143.7 0.0304 A0413008 148 1. 2. 147.8 -0.0248 A0413008 149 1. 2. 149.2 -0.1283 A0413008 150 1. 2. 153.3 -0.2594 A0413008 151 1. 2. 153.3 -0.1835 A0413008 152 1. 2. 158.9 -0.1905 A0413008 153 1. 2. 163.1 -0.1561 A0413008 154 1. 2. 174.3 -0.1010 A0413008 155 1. 2. 184.2 -0.0253 0.0621 A0413008 156 1. 2. 192.5 -0.0599 0.0552 A0413008 157 1. 2. 205.1 -0.1083 A0413008 158 1. 2. 212.1 0.0089 0.0690 A0413008 159 1. 2. 234.4 -0.0811 A0413008 160 1. 2. 237.2 -0.1984 0.0827 A0413008 161 1. 2. 242.9 0.0292 0.0414 A0413008 162 1. 2. 256.8 -0.0607 0.0690 A0413008 163 1. 2. 263.7 -0.1366 A0413008 164 1. 2. 270.8 0.0012 0.0345 A0413008 165 1. 2. 284.8 0.0011 0.0483 A0413008 166 1. 2. 294.5 0.0009 0.0414 A0413008 167 1. 2. 295.9 -0.1232 A0413008 168 1. 2. 302.9 -0.1440 A0413008 169 1. 2. 312.7 -0.0751 0.0621 A0413008 170 1. 2. 354.6 -0.1101 A0413008 171 1. 2. 404.8 -0.1590 A0413008 172 1. 2. 453.7 -0.1941 A0413008 173 1. 2. 504.0 -0.2292 A0413008 174 1. 2. 553.0 -0.0092 A0413008 175 1. 2. 604.7 -0.0925 A0413008 176 1. 2. 646.6 -0.0862 A0413008 177 1. 2. 703.9 -0.0800 A0413008 178 1. 2. 752.8 -0.1013 A0413008 179 1. 2. 803.1 -0.0743 A0413008 180 1. 2. 852.0 -0.0887 A0413008 181 1. 2. 900.8 -0.2135 A0413008 182 1. 2. 952.5 -0.2279 0.0414 A0413008 183 1. 2. 1001.3 -0.3595 A0413008 184 1. 2. 1048.8 -0.4084 A0413008 185 1. 2. 1097.6 -0.5607 A0413008 186 ENDDATA 166 0 A0413008 187 ENDSUBENT 186 0 A041300899999 NOSUBENT A0413009 20240911 A118A0413009 1 NOSUBENT A0413010 20240911 A118A0413010 1 SUBENT A0413011 20240911 A118A0413011 1 BIB 5 15 A0413011 2 REACTION (5-B-11(P,A)4-BE-8,PAR,DA,,4PI) A0413011 3 ANALYSIS The absolute cross section was determined at low A0413011 4 energies relative to the 11B+p elastic scattering A0413011 5 cross section A0413011 6 ERR-ANALYS (ERR-T) Total error A0413011 7 (ERR-1) Uncertainty in angular position A0413011 8 (ERR-2) Uncertainty in counting statistics and A0413011 9 angular distribution A0413011 10 (ERR-3) Uncertainty in contributions of the secondary A0413011 11 alpha-particles to the yield of the alpha1-peak A0413011 12 STATUS (TABLE,,H.W.Becker+,J,ZP/A,327,341,1987) values A0413011 13 on p.353, 354.A0413011 14 (DEP,A0413006) Elastic scattering cross section A0413011 15 relative to Rutherford scattering A0413011 16 HISTORY (20240911C) SD A0413011 17 ENDBIB 15 0 A0413011 18 COMMON 3 3 A0413011 19 EN ANG ERR-1 A0413011 20 KEV ADEG PER-CENT A0413011 21 300. 37.5 2. A0413011 22 ENDCOMMON 3 0 A0413011 23 DATA 5 2 A0413011 24 LVL-NUMB DATA ERR-T ERR-2 ERR-3 A0413011 25 NO-DIM MB MB PER-CENT PER-CENT A0413011 26 0. 1.03 0.06 5.2 A0413011 27 1. 165. 10. 0.5 5.5 A0413011 28 ENDDATA 4 0 A0413011 29 ENDSUBENT 28 0 A041301199999 ENDENTRY 11 0 A041399999999