ENTRY A0289 20120110 A075A028900000001 SUBENT A0289001 20120110 A075A028900100001 BIB 12 33 A028900100002 TITLE Cross Section Measurements of Two-Nucleon Pickup A028900100003 Reactions in the 13-C+D System at Deuteron Energies A028900100004 Below 350 keV A028900100005 AUTHOR (A.A.Naqvi, M.M.Nagadi, S.Kidwai, M.A.Al-Ohali, A028900100006 F.Z.Khiari) A028900100007 INSTITUTE (3SARDHA) Center For Applied Physical Sciences and A028900100008 Department of Physics A028900100009 REFERENCE (J,AUJ,51,903,1998) A028900100010 DETECTOR (SIBAR) A028900100011 FACILITY (ACCEL,3SARDHA) 350 K-V Accelerator A028900100012 METHOD (SITA) A028900100013 COMMENT Abstract: the Excitation Functions of 13-C(D,A0)11-B A028900100014 And 13-C(D,A1)11-B Reactions with 5.167 and 3.307 MeV A028900100015 Q-Values, Respectively, Exhibit Smooth Variations of A028900100016 Cross Section with Energy. The Angular Distribution ofA028900100017 13-C(D,A0)11-B Reaction is Asymmetric. With DecreasingA028900100018 Deuteron Energy, the Degree of Asymmetry Increases andA028900100019 Below 220 KeV Deuteron Energy the Angular DistributionA028900100020 Is Backward-Peaked. This Indicates a Dominating A028900100021 Contribution from the Direct Reaction in this Channel A028900100022 Below 220 KeV Deuteron Energy. The Angular A028900100023 Distribution of 13-C(D,A1)11-B Reactions are Highly A028900100024 Symmetric About 90 Degree, Indicating a Dominating A028900100025 Compound Nucleus Contribution Over this Energy Range. A028900100026 - By Compiler: Energy of First Excited Level of B-11 A028900100027 Was Taken from ENSDF by Compiler. A028900100028 SAMPLE 30 Micro-Gramm/Cm**2 Thick Enriched 13-C Foils. A028900100029 HISTORY (20020605C) A028900100030 (20120110A) Correction in sub.002, MeV---to keV, A028900100031 according N.Otsuka remarks. Correction in Err-Analys, A028900100032 according new Exfor rules. A028900100033 PART-DET (A) A028900100034 EN-SEC (E-LVL,5-B-11) A028900100035 ENDBIB 33 0 A028900100036 NOCOMMON 0 0 A028900100037 ENDSUBENT 36 0 A028900199999 SUBENT A0289002 20120110 A075A028900200001 BIB 3 10 A028900200002 REACTION (6-C-13(D,A)5-B-11,PAR,DA) A028900200003 STATUS (CURVE) By CAJAD-Figure 2,4 of J,AUJ,51,903,1998 A028900200004 ERR-ANALYS Statistical uncertainties were 2-10 % for ground state A028900200005 production and 5-6% for first excited level. A028900200006 The systematic uncertainties, which were due to A028900200007 charge integration, target thickness and the finite A028900200008 angular resolution, were estimated to be 4-5%. A028900200009 (EN-ERR-DIG).Digitizing error of energy. A028900200010 (DATA-ERR).The uncertainty is reported by authors on A028900200011 figures. A028900200012 ENDBIB 10 0 A028900200013 COMMON 2 3 A028900200014 ANG EN-ERR-DIG A028900200015 ADEG KEV A028900200016 90. 0.7 A028900200017 ENDCOMMON 3 0 A028900200018 DATA 4 29 A028900200019 EN E-LVL DATA DATA-ERR A028900200020 KEV KEV MU-B/SR MU-B/SR A028900200021 180.3 0. 0.36 0.12 A028900200022 190.1 0. 0.21 0.12 A028900200023 200.3 0. 1.15 0.12 A028900200024 210.2 0. 1.01 0.12 A028900200025 220. 0. 1.45 0.12 A028900200026 230.2 0. 2.14 0.12 A028900200027 240.4 0. 3.83 0.12 A028900200028 249.9 2124. 0.748 0.018 A028900200029 250.5 0. 6.36 0.12 A028900200030 259.7 0. 8.3 0.12 A028900200031 259.8 2124. 1.03 0.04 A028900200032 269.5 0. 10.16 0.12 A028900200033 270. 2124. 1.19 0.06 A028900200034 280. 2124. 1.45 0.12 A028900200035 280.1 0. 11.6 0.12 A028900200036 289.6 2124. 1.99 0.12 A028900200037 289.7 0. 14.5 0.4 A028900200038 299.7 2124. 3.08 0.2 A028900200039 300.2 0. 19.3 0.4 A028900200040 309.2 2124. 3.92 0.22 A028900200041 310.1 0. 25.5 0.6 A028900200042 326.2 2124. 6.35 0.18 A028900200043 327.6 0. 36.4 0.8 A028900200044 334.4 2124. 7.13 0.2 A028900200045 334.7 0. 42.8 1.1 A028900200046 339.2 2124. 7.43 0.22 A028900200047 339.3 0. 50.5 0.9 A028900200048 349.7 2124. 7.74 0.26 A028900200049 350.2 0. 56.4 1.1 A028900200050 ENDDATA 31 0 A028900200051 ENDSUBENT 50 0 A028900299999 SUBENT A0289003 20120110 A075A028900300001 BIB 3 10 A028900300002 REACTION (6-C-13(D,A)5-B-11,PAR,DA) A028900300003 STATUS (CURVE) By CAJAD-Figure 3,5 of J,AUJ,51,903,1998 A028900300004 ERR-ANALYS (ANG-ERR-D).Digitizing error of angle A028900300005 (DATA-ERR).The uncertainty is reported by authors on A028900300006 figures. A028900300007 Statistical uncertainties were 2-24 % for ground state A028900300008 production and 2-8% for first excited level. A028900300009 The systematic uncertainties, which were due to A028900300010 charge integration, target thickness and the finite A028900300011 angular resolution, were estimated to be 4-5%. A028900300012 ENDBIB 10 0 A028900300013 COMMON 1 3 A028900300014 ANG-ERR-D A028900300015 ADEG A028900300016 0.6 A028900300017 ENDCOMMON 3 0 A028900300018 DATA 5 190 A028900300019 EN ANG E-LVL DATA DATA-ERR A028900300020 KEV ADEG KEV MU-B/SR MU-B/SR A028900300021 180. 29.8 0. 0.382 0.013 A028900300022 180. 48. 0. 0.368 0.025 A028900300023 180. 66.2 0. 0.29 0.04 A028900300024 180. 79.7 0. 0.228 0.011 A028900300025 180. 90.1 0. 0.4 0.04 A028900300026 180. 109.5 0. 0.56 0.04 A028900300027 180. 119.7 0. 0.6 0.04 A028900300028 180. 128. 0. 0.74 0.05 A028900300029 180. 137.8 0. 0.77 0.06 A028900300030 180. 145.6 0. 0.92 0.07 A028900300031 180. 154.8 0. 1.17 0.1 A028900300032 180. 164.6 0. 1.17 0.1 A028900300033 200. 29.8 0. 1.1 0.06 A028900300034 200. 57.7 0. 1.01 0.05 A028900300035 200. 65.6 0. 0.81 0.04 A028900300036 200. 79.7 0. 0.91 0.05 A028900300037 200. 89.7 0. 1.11 0.07 A028900300038 200. 110.2 0. 1.21 0.07 A028900300039 200. 119. 0. 1.8 0.11 A028900300040 200. 128.4 0. 2.19 0.14 A028900300041 200. 137.2 0. 2.44 0.15 A028900300042 200. 145.5 0. 3. 0.16 A028900300043 200. 153.8 0. 2.82 0.18 A028900300044 200. 165.8 0. 3.21 0.2 A028900300045 220. 30.5 0. 1.67 0.06 A028900300046 220. 48. 0. 1.45 0.05 A028900300047 220. 66. 0. 1.18 0.03 A028900300048 220. 79.7 0. 1.28 0.04 A028900300049 220. 90.1 0. 1.43 0.04 A028900300050 220. 109.8 0. 1.9 0.06 A028900300051 220. 119.5 0. 2.59 0.09 A028900300052 220. 127.7 0. 2.7 0.09 A028900300053 220. 138. 0. 2.78 0.09 A028900300054 220. 145.8 0. 3.24 0.12 A028900300055 220. 154.7 0. 3.6 0.12 A028900300056 220. 165.1 0. 4.11 0.14 A028900300057 250. 30.5 0. 7.86 0.05 A028900300058 250. 31.1 2124. 3.95 A028900300059 250. 58.4 0. 6.78 0.05 A028900300060 250. 58.4 2124. 2.41 A028900300061 250. 66.4 2124. 1.45 A028900300062 250. 66.5 0. 5.83 0.05 A028900300063 250. 79.9 2124. 0.99 A028900300064 250. 80.2 0. 5.87 0.05 A028900300065 250. 89.6 0. 6.26 0.05 A028900300066 250. 90. 2124. 0.64 A028900300067 250. 109.3 0. 7.23 0.05 A028900300068 250. 109.3 2124. 1.17 A028900300069 250. 119.4 2124. 1.67 A028900300070 250. 119.9 0. 8.67 0.11 A028900300071 250. 127. 2124. 2.17 A028900300072 250. 127.8 0. 10.12 0.14 A028900300073 250. 136.7 2124. 2.67 A028900300074 250. 137.7 0. 10.81 0.14 A028900300075 250. 144.7 2124. 3.3 A028900300076 250. 146. 0. 12.1 0.16 A028900300077 250. 154.1 0. 12.61 0.21 A028900300078 250. 154.3 2124. 4.29 A028900300079 250. 163.6 2124. 4.42 A028900300080 250. 164.5 0. 13.53 0.25 A028900300081 270. 30.1 0. 13.8 0.4 A028900300082 270. 30.6 2124. 7.72 A028900300083 270. 48.3 2124. 4.83 A028900300084 270. 48.5 0. 12. 0.3 A028900300085 270. 57.6 0. 11.5 0.3 A028900300086 270. 58.4 2124. 4.48 A028900300087 270. 65.3 0. 10.63 0.27 A028900300088 270. 66.4 2124. 2.67 A028900300089 270. 79.7 0. 10.04 0.27 A028900300090 270. 79.9 2124. 1.72 A028900300091 270. 89.2 2124. 1.13 A028900300092 270. 89.9 0. 10.2 0.27 A028900300093 270. 109.4 0. 12.04 0.29 A028900300094 270. 109.8 2124. 2.02 A028900300095 270. 119.4 0. 14.7 0.4 A028900300096 270. 119.4 2124. 3.25 A028900300097 270. 126.6 2124. 4.36 A028900300098 270. 128.1 0. 15.7 0.5 A028900300099 270. 137. 0. 16. 0.5 A028900300100 270. 137.1 2124. 5.11 A028900300101 270. 144.6 2124. 6.46 A028900300102 270. 145.1 0. 18.1 0.5 A028900300103 270. 153.9 2124. 7.81 A028900300104 270. 154. 0. 18.5 0.5 A028900300105 270. 164.4 2124. 8.2 A028900300106 270. 165. 0. 19.8 0.6 A028900300107 290. 30.2 0. 21.6 A028900300108 290. 31. 2124. 12.7 0.4 A028900300109 290. 48.7 2124. 8.48 0.17 A028900300110 290. 48.9 0. 17.5 A028900300111 290. 57.7 0. 16.9 A028900300112 290. 58.8 2124. 6.92 0.17 A028900300113 290. 65.1 0. 14.7 A028900300114 290. 66. 2124. 4.13 0.18 A028900300115 290. 79.2 0. 14.3 A028900300116 290. 79.9 2124. 2.94 0.17 A028900300117 290. 89.2 0. 13.2 A028900300118 290. 90. 2124. 2.1 0.17 A028900300119 290. 109.1 0. 15.9 A028900300120 290. 109.7 2124. 3.23 0.17 A028900300121 290. 119.3 0. 19.7 A028900300122 290. 119.4 2124. 5.56 0.17 A028900300123 290. 126.9 0. 21.4 A028900300124 290. 127.4 2124. 6.31 0.17 A028900300125 290. 136.6 2124. 7.66 0.17 A028900300126 290. 137. 0. 22.4 A028900300127 290. 144.6 2124. 9.86 0.17 A028900300128 290. 145.9 0. 24.7 A028900300129 290. 153.8 2124. 10.61 0.17 A028900300130 290. 154.7 0. 25.1 A028900300131 290. 164.3 2124. 13.06 0.25 A028900300132 290. 164.8 0. 26.6 A028900300133 310. 29.6 0. 43.4 0.4 A028900300134 310. 30.9 2124. 22.8 0.6 A028900300135 310. 47.8 2124. 17.6 0.5 A028900300136 310. 48.3 0. 37.2 0.4 A028900300137 310. 57.4 0. 35. 0.4 A028900300138 310. 58.8 2124. 11.54 0.17 A028900300139 310. 66. 0. 27.6 0.4 A028900300140 310. 67.6 2124. 8.15 0.17 A028900300141 310. 79.1 0. 24.8 0.4 A028900300142 310. 79.5 2124. 4.52 0.17 A028900300143 310. 89.2 0. 25. 0.4 A028900300144 310. 90.4 2124. 3.57 0.18 A028900300145 310. 108.7 0. 29.5 0.4 A028900300146 310. 110.1 2124. 5.55 0.17 A028900300147 310. 119.4 0. 36.5 0.4 A028900300148 310. 119.4 2124. 8. 0.17 A028900300149 310. 126.9 2124. 12.3 0.5 A028900300150 310. 127. 0. 39.6 0.4 A028900300151 310. 137. 2124. 13.01 0.3 A028900300152 310. 137.6 0. 42.1 0.5 A028900300153 310. 144.9 2124. 18. 0.6 A028900300154 310. 145.7 0. 45.9 0.7 A028900300155 310. 154.6 0. 49. 0.8 A028900300156 310. 155. 2124. 21.2 0.6 A028900300157 310. 164.2 2124. 23.8 0.7 A028900300158 310. 164.8 0. 51.2 0.6 A028900300159 335. 30.1 0. 74.9 1.2 A028900300160 335. 31.1 2124. 43.8 1.5 A028900300161 335. 48. 0. 57.9 1.1 A028900300162 335. 48.1 2124. 27.5 0.8 A028900300163 335. 58.4 0. 51. 1. A028900300164 335. 58.7 2124. 22. 0.7 A028900300165 335. 65.6 0. 42.5 0.8 A028900300166 335. 66.8 2124. 12.9 0.3 A028900300167 335. 79. 0. 37.2 0.4 A028900300168 335. 80.3 2124. 8.29 0.17 A028900300169 335. 89.8 0. 42.8 0.5 A028900300170 335. 89.9 2124. 7.21 0.17 A028900300171 335. 108.8 0. 47.6 0.6 A028900300172 335. 109.3 2124. 9.56 0.17 A028900300173 335. 119.3 0. 58.8 1. A028900300174 335. 119.3 2124. 15.5 0.6 A028900300175 335. 127. 0. 67.4 1. A028900300176 335. 127.7 2124. 22.7 0.7 A028900300177 335. 136.9 2124. 26. 0.9 A028900300178 335. 137.2 0. 70.4 1.2 A028900300179 335. 145.2 2124. 32. 1. A028900300180 335. 145.3 0. 76.4 1.5 A028900300181 335. 154.5 2124. 34. 1.2 A028900300182 335. 154.9 0. 86.8 1.6 A028900300183 335. 164.5 2124. 44.3 1.6 A028900300184 335. 164.7 0. 91.9 1.6 A028900300185 350. 30.4 0. 97.2 1.7 A028900300186 350. 31.4 2124. 59.9 2.1 A028900300187 350. 47.1 0. 82.9 1.5 A028900300188 350. 48.8 2124. 42.1 1.5 A028900300189 350. 57.5 0. 77.8 1.5 A028900300190 350. 57.8 2124. 29.5 0.9 A028900300191 350. 65.8 0. 63.8 1. A028900300192 350. 65.8 2124. 20.9 0.9 A028900300193 350. 79.4 2124. 12.06 0.17 A028900300194 350. 79.6 0. 54.7 0.9 A028900300195 350. 88.9 0. 57. 0.7 A028900300196 350. 90.4 2124. 7.7 0.17 A028900300197 350. 109.1 0. 69.7 1.5 A028900300198 350. 109.7 2124. 12.72 0.17 A028900300199 350. 118.8 0. 83.2 1.5 A028900300200 350. 119.7 2124. 19.4 0.6 A028900300201 350. 127. 0. 93.9 1.6 A028900300202 350. 127.6 2124. 26.3 0.7 A028900300203 350. 136.8 2124. 32.8 1. A028900300204 350. 137.2 0. 97.2 1.7 A028900300205 350. 145.5 0. 108.4 1.9 A028900300206 350. 145.6 2124. 41. 1.4 A028900300207 350. 154.3 0. 122.2 1.9 A028900300208 350. 154.3 2124. 48. 1.7 A028900300209 350. 164.9 0. 125.5 2.3 A028900300210 350. 165.2 2124. 61.6 2.1 A028900300211 ENDDATA 192 0 A028900300212 ENDSUBENT 211 0 A028900399999 SUBENT A0289004 20120110 A075A028900400001 BIB 4 6 A028900400002 REACTION (6-C-13(D,A)5-B-11,PAR,SIG) A028900400003 ANALYSIS (INTAD) A028900400004 STATUS (TABLE).Table of J,AUJ,51,903,1998 A028900400005 (DEP,A0289003) A028900400006 ERR-ANALYS (DATA-ERR).The Uncertainties were Calculated from the A028900400007 Uncertainties of the Legendre Polynomial Fits. A028900400008 ENDBIB 6 0 A028900400009 NOCOMMON 0 0 A028900400010 DATA 4 15 A028900400011 EN E-LVL DATA DATA-ERR A028900400012 KEV KEV MICRO-B MICRO-B A028900400013 180. 0. 6. 2.5 A028900400014 200. 0. 18. 4. A028900400015 220. 0. 24. 4. A028900400016 250. 0. 99. 11. A028900400017 250. 2125. 27. 6. A028900400018 270. 0. 162. 14. A028900400019 270. 2125. 49. 7. A028900400020 290. 0. 240. 17. A028900400021 290. 2125. 79. 9. A028900400022 310. 0. 441. 23. A028900400023 310. 2125. 143. 12. A028900400024 335. 0. 722. 29. A028900400025 335. 2125. 259. 16. A028900400026 350. 0. 1009. 34. A028900400027 350. 2125. 353. 20. A028900400028 ENDDATA 17 0 A028900400029 ENDSUBENT 28 0 A028900499999 ENDENTRY 4 0 A028999999999