ENTRY F1515 20250113 F100F1515000 1 SUBENT F1515001 20250113 F100F1515001 1 BIB 7 11 F1515001 2 TITLE Measurement of 9Be(d,xt) reaction total cross F1515001 3 sections by secondary activation and spectroscopy F1515001 4 methods F1515001 5 AUTHOR (L.N.Generalov,I.A.Karpov) F1515001 6 INSTITUTE (4RUSEPA) F1515001 7 REFERENCE (J,BAS,88,1332,2024) English translation F1515001 8 #doi:10.1134/S1062873824707529 F1515001 9 (J,IZV,88,1316,2024) Russian original F1515001 10 FACILITY (VDGT,4RUSEPA) EGP-10 tandem accelerator F1515001 11 STATUS (APRVD) Entry was approved by Dr. L.N. Generalov. F1515001 12 HISTORY (20250113C) F1515001 13 ENDBIB 11 0 F1515001 14 NOCOMMON 0 0 F1515001 15 ENDSUBENT 14 0 F151500199999 SUBENT F1515002 20250113 F100F1515002 1 BIB 8 22 F1515002 2 REACTION (4-BE-9(D,X)1-H-3,,DA) F1515002 3 REL-REF (M,F0778001,L.N.Generalov+,J,BAS,70,217,2006) English F1515002 4 translation. Experiment description is given. F1515002 5 (M,F0778001,L.N.Generalov+,J,IZV,70,191,2006) Russian F1515002 6 original. F1515002 7 SAMPLE Self-supporting beryllium target with 658+-33 mu-g/cm2 F1515002 8 thick deposited on a thin SiO backing was used. F1515002 9 DETECTOR (SI,TELES) Six telescopes of dE-E detectors were F1515002 10 used. dE detectors thickness was 12-14 mu-m, E F1515002 11 detectors thickness was 1.2 mm. F1515002 12 METHOD (EDE) F1515002 13 PART-DET (T) F1515002 14 ERR-ANALYS (ERR-S) Random error consists of random errors in the F1515002 15 parameters that determine the differential cross F1515002 16 sections, errors in specifying angles and implicit F1515002 17 unevenness in target thickness, about 8%. F1515002 18 (ERR-SYS) Systematic uncertainty includes F1515002 19 (ERR-1) Error in deuteron beam measurement. F1515002 20 (ERR-2) Error in target thickness measurement. F1515002 21 STATUS (TABLE,,L.N.Generalov+,J,BAS,88,1332,2024) Data were F1515002 22 presented by authors. The same on fig. 6 from F1515002 23 Bull.Rus.Ac.Sci.Phys. 88,1332,2024. F1515002 24 ENDBIB 22 0 F1515002 25 COMMON 3 3 F1515002 26 ERR-SYS ERR-1 ERR-2 F1515002 27 PER-CENT PER-CENT PER-CENT F1515002 28 5.3 2. 5. F1515002 29 ENDCOMMON 3 0 F1515002 30 DATA 4 336 F1515002 31 EN ANG-CM DATA-CM ERR-S F1515002 32 MEV ADEG MB/SR MB/SR F1515002 33 2. 10. 48. 4.8 F1515002 34 2. 15. 43. 4.3 F1515002 35 2. 20. 33.9 2.7 F1515002 36 2. 25. 33.8 2.7 F1515002 37 2. 30. 32.5 2.6 F1515002 38 2. 35. 28. 2.2 F1515002 39 2. 40. 23.4 1.9 F1515002 40 2. 45. 20.7 1.7 F1515002 41 2. 50. 16.7 1.3 F1515002 42 2. 55. 16.1 1.3 F1515002 43 2. 60. 16.6 1.3 F1515002 44 2. 70. 13.5 1.1 F1515002 45 2. 80. 13.5 1.1 F1515002 46 2. 85. 13.4 1.2 F1515002 47 2. 90. 12.6 1. F1515002 48 2. 100. 11.8 0.9 F1515002 49 2. 110. 9.2 0.7 F1515002 50 2. 120. 9.8 0.8 F1515002 51 2. 125. 9.9 0.8 F1515002 52 2. 130. 10.6 0.8 F1515002 53 2. 140. 9.8 0.8 F1515002 54 2. 150. 10.6 0.8 F1515002 55 2. 160. 6.1 0.5 F1515002 56 2. 170. 3.3 0.3 F1515002 57 3. 10. 95. 28.5 F1515002 58 3. 15. 83. 24.9 F1515002 59 3. 20. 80. 16. F1515002 60 3. 25. 68. 10.9 F1515002 61 3. 30. 47. 7.5 F1515002 62 3. 35. 38. 6.1 F1515002 63 3. 40. 31. 5. F1515002 64 3. 45. 27. 4.3 F1515002 65 3. 50. 22. 3.5 F1515002 66 3. 55. 20. 3.2 F1515002 67 3. 60. 15.2 2.4 F1515002 68 3. 65. 12.2 2. F1515002 69 3. 70. 11. 1.8 F1515002 70 3. 80. 9.5 1.5 F1515002 71 3. 85. 11.1 1.8 F1515002 72 3. 90. 10.6 1.7 F1515002 73 3. 95. 10.9 1.7 F1515002 74 3. 100. 10. 1.6 F1515002 75 3. 105. 8.86 1.4 F1515002 76 3. 110. 8.66 1.4 F1515002 77 3. 115. 10. 1.6 F1515002 78 3. 120. 9.92 1.6 F1515002 79 3. 125. 11.1 1.8 F1515002 80 3. 130. 11. 1.8 F1515002 81 3. 140. 10.4 1.7 F1515002 82 3. 150. 10.3 1.6 F1515002 83 3. 155. 7.65 1.2 F1515002 84 3. 160. 6.66 1.1 F1515002 85 3. 165. 5.65 0.9 F1515002 86 3. 170. 5. 0.8 F1515002 87 3.5 10. 83. 12. F1515002 88 3.5 15. 71. 11. F1515002 89 3.5 20. 52. 5. F1515002 90 3.5 25. 40.2 3.2 F1515002 91 3.5 30. 33.5 2.7 F1515002 92 3.5 35. 30.9 2.5 F1515002 93 3.5 40. 29.9 2.4 F1515002 94 3.5 45. 28.3 2.3 F1515002 95 3.5 50. 27. 2.2 F1515002 96 3.5 55. 21.7 1.7 F1515002 97 3.5 60. 18.4 1.5 F1515002 98 3.5 65. 14. 1.1 F1515002 99 3.5 70. 10.5 0.9 F1515002 100 3.5 80. 9.4 0.8 F1515002 101 3.5 85. 8.1 0.7 F1515002 102 3.5 90. 7.6 0.6 F1515002 103 3.5 95. 7. 0.6 F1515002 104 3.5 100. 6.2 0.5 F1515002 105 3.5 105. 5.5 0.4 F1515002 106 3.5 110. 5.6 0.4 F1515002 107 3.5 115. 5.6 0.4 F1515002 108 3.5 120. 6.4 0.5 F1515002 109 3.5 125. 6.4 0.5 F1515002 110 3.5 130. 7.5 0.6 F1515002 111 3.5 140. 8.7 0.7 F1515002 112 3.5 150. 9. 0.7 F1515002 113 3.5 155. 8.6 0.7 F1515002 114 3.5 160. 7.5 0.6 F1515002 115 3.5 165. 6.3 0.5 F1515002 116 3.5 170. 6.2 0.5 F1515002 117 4. 10. 92. 6.5 F1515002 118 4. 15. 80. 5.7 F1515002 119 4. 20. 63. 4.5 F1515002 120 4. 25. 48. 3.4 F1515002 121 4. 30. 36.1 2.6 F1515002 122 4. 35. 36.5 2.6 F1515002 123 4. 40. 33.5 2.4 F1515002 124 4. 45. 28. 2. F1515002 125 4. 50. 24.8 1.8 F1515002 126 4. 55. 20.3 1.4 F1515002 127 4. 60. 16.4 1.2 F1515002 128 4. 70. 12.5 0.9 F1515002 129 4. 80. 10.6 0.8 F1515002 130 4. 85. 9.2 0.7 F1515002 131 4. 90. 9.2 0.7 F1515002 132 4. 95. 8.4 0.6 F1515002 133 4. 100. 8.6 0.6 F1515002 134 4. 105. 6.7 0.5 F1515002 135 4. 115. 6.1 0.4 F1515002 136 4. 120. 6.2 0.4 F1515002 137 4. 125. 6.5 0.5 F1515002 138 4. 130. 7.7 0.5 F1515002 139 4. 140. 9. 0.6 F1515002 140 4. 150. 8.1 0.6 F1515002 141 4. 155. 9.3 0.7 F1515002 142 4. 160. 8.4 0.6 F1515002 143 4. 165. 7.9 0.6 F1515002 144 4. 170. 7. 0.5 F1515002 145 4.5 10. 85. 13. F1515002 146 4.5 15. 67. 10. F1515002 147 4.5 20. 48. 5. F1515002 148 4.5 25. 37.1 3. F1515002 149 4.5 30. 34.1 2.7 F1515002 150 4.5 40. 26.2 2.1 F1515002 151 4.5 50. 23. 2. F1515002 152 4.5 55. 23. 2. F1515002 153 4.5 60. 21. 2. F1515002 154 4.5 70. 16.9 1.4 F1515002 155 4.5 75. 16. 1. F1515002 156 4.5 80. 13.7 1.1 F1515002 157 4.5 90. 10. 1. F1515002 158 4.5 100. 8.9 0.7 F1515002 159 4.5 110. 8.6 0.7 F1515002 160 4.5 120. 8.9 0.7 F1515002 161 4.5 130. 7.9 0.6 F1515002 162 4.5 140. 7.4 0.6 F1515002 163 4.5 150. 6.8 0.5 F1515002 164 4.5 160. 6.3 0.5 F1515002 165 4.5 170. 5.6 0.4 F1515002 166 5. 10. 104. 16. F1515002 167 5. 15. 87. 13. F1515002 168 5. 20. 71. 7. F1515002 169 5. 27.6 43. 4. F1515002 170 5. 30. 36. 3. F1515002 171 5. 35. 26.9 2.2 F1515002 172 5. 47.6 23. 2. F1515002 173 5. 50. 21.8 1.7 F1515002 174 5. 60. 19. 1.5 F1515002 175 5. 67.6 17. 1.4 F1515002 176 5. 75. 14.7 1.2 F1515002 177 5. 80. 11.1 0.9 F1515002 178 5. 80. 10.4 0.8 F1515002 179 5. 95. 8.4 0.7 F1515002 180 5. 100. 7.4 0.6 F1515002 181 5. 100. 7.2 0.6 F1515002 182 5. 105. 7.1 0.6 F1515002 183 5. 115. 7. 0.6 F1515002 184 5. 120. 7.4 0.6 F1515002 185 5. 120. 7.3 0.6 F1515002 186 5. 125. 7.2 0.6 F1515002 187 5. 135. 7.4 0.6 F1515002 188 5. 145. 7.5 0.6 F1515002 189 5. 150. 6.9 0.6 F1515002 190 5. 160. 5.8 0.5 F1515002 191 5. 170. 4.5 0.4 F1515002 192 5.5 10. 96. 14. F1515002 193 5.5 15. 68. 10. F1515002 194 5.5 20. 54. 5. F1515002 195 5.5 25. 40. 3. F1515002 196 5.5 30. 32. 3. F1515002 197 5.5 35. 29.8 2.4 F1515002 198 5.5 40. 26.3 2.1 F1515002 199 5.5 45. 22. 2. F1515002 200 5.5 50. 20.6 1.7 F1515002 201 5.5 55. 18.1 1.4 F1515002 202 5.5 60. 15.8 1.3 F1515002 203 5.5 70. 11.8 0.9 F1515002 204 5.5 75. 10.2 0.8 F1515002 205 5.5 80. 8.4 0.7 F1515002 206 5.5 90. 8.4 0.7 F1515002 207 5.5 95. 7.9 0.6 F1515002 208 5.5 100. 7.5 0.6 F1515002 209 5.5 105. 8.3 0.6 F1515002 210 5.5 110. 8. 0.6 F1515002 211 5.5 120. 8.3 0.7 F1515002 212 5.5 125. 8.2 0.7 F1515002 213 5.5 130. 7.1 0.6 F1515002 214 5.5 140. 6.1 0.5 F1515002 215 5.5 150. 5.8 0.5 F1515002 216 5.5 160. 4.8 0.4 F1515002 217 5.5 170. 4.7 0.4 F1515002 218 6. 10. 113. 16.9 F1515002 219 6. 15.5 73. 10.9 F1515002 220 6. 20. 57. 5.7 F1515002 221 6. 25. 38. 3. F1515002 222 6. 27.6 35. 2.8 F1515002 223 6. 30. 32. 2.6 F1515002 224 6. 40. 25.3 2. F1515002 225 6. 47.6 20. 1.6 F1515002 226 6. 50. 19. 1.5 F1515002 227 6. 55. 19.6 1.6 F1515002 228 6. 60. 17.6 1.4 F1515002 229 6. 67.6 11.7 0.9 F1515002 230 6. 70. 9.9 0.8 F1515002 231 6. 75. 9. 0.7 F1515002 232 6. 80. 8.3 0.7 F1515002 233 6. 90. 7.4 0.6 F1515002 234 6. 95. 8.1 0.6 F1515002 235 6. 100. 7.6 0.6 F1515002 236 6. 100. 7.8 0.6 F1515002 237 6. 105. 7.3 0.6 F1515002 238 6. 115. 6.7 0.5 F1515002 239 6. 120. 6.1 0.5 F1515002 240 6. 120. 7. 0.6 F1515002 241 6. 125. 6.4 0.5 F1515002 242 6. 140. 6.2 0.5 F1515002 243 6. 145. 5.6 0.4 F1515002 244 6. 150. 5.5 0.4 F1515002 245 6. 160. 5.2 0.4 F1515002 246 6. 170. 5.5 0.4 F1515002 247 6.5 10. 111. 17. F1515002 248 6.5 15. 83. 12. F1515002 249 6.5 20. 65. 6. F1515002 250 6.5 25. 43. 3. F1515002 251 6.5 30. 26. 2. F1515002 252 6.5 35. 23. 2. F1515002 253 6.5 40. 22. 2. F1515002 254 6.5 45. 20. 2. F1515002 255 6.5 50. 20.6 1.6 F1515002 256 6.5 55. 18.9 1.5 F1515002 257 6.5 60. 15.5 1.2 F1515002 258 6.5 65. 10.2 0.8 F1515002 259 6.5 70. 7.5 0.6 F1515002 260 6.5 80. 6.6 0.5 F1515002 261 6.5 90. 6.3 0.5 F1515002 262 6.5 95. 6.1 0.5 F1515002 263 6.5 100. 7. 0.5 F1515002 264 6.5 105. 7.6 0.6 F1515002 265 6.5 110. 7.7 0.6 F1515002 266 6.5 115. 7.5 0.6 F1515002 267 6.5 120. 7.3 0.6 F1515002 268 6.5 130. 5.7 0.5 F1515002 269 6.5 145. 4.9 0.4 F1515002 270 6.5 150. 4.5 0.4 F1515002 271 6.5 155. 5. 0.4 F1515002 272 6.5 160. 5.3 0.4 F1515002 273 6.5 170. 6.8 0.5 F1515002 274 7. 10. 108. 16. F1515002 275 7. 15. 80. 12. F1515002 276 7. 20. 67. 7. F1515002 277 7. 27.6 44. 4. F1515002 278 7. 30. 35. 3. F1515002 279 7. 35. 32. 3. F1515002 280 7. 40. 27.2 2.2 F1515002 281 7. 47.6 26. 2. F1515002 282 7. 50. 22.8 1.8 F1515002 283 7. 55. 18.8 1.5 F1515002 284 7. 60. 14.9 1.2 F1515002 285 7. 65. 13. 1. F1515002 286 7. 67.6 12.2 1. F1515002 287 7. 75. 12. 1. F1515002 288 7. 80. 9.8 0.8 F1515002 289 7. 80. 10.4 0.8 F1515002 290 7. 90. 8. 0.7 F1515002 291 7. 95. 7.7 0.7 F1515002 292 7. 100. 6.4 0.5 F1515002 293 7. 100. 6.6 0.5 F1515002 294 7. 105. 6.9 0.6 F1515002 295 7. 110. 6.7 0.6 F1515002 296 7. 120. 5.4 0.4 F1515002 297 7. 120. 5.9 0.5 F1515002 298 7. 130. 5.4 0.4 F1515002 299 7. 140. 5.3 0.4 F1515002 300 7. 150. 5.2 0.4 F1515002 301 7. 155. 4.6 0.4 F1515002 302 7. 160. 4.8 0.4 F1515002 303 7. 170. 5.3 0.4 F1515002 304 8. 10. 120. 10.8 F1515002 305 8. 15. 120. 10.8 F1515002 306 8. 20. 110. 9.9 F1515002 307 8. 25. 70. 6.3 F1515002 308 8. 30. 42. 3.8 F1515002 309 8. 40. 33.8391 3. F1515002 310 8. 45. 29.8 2.7 F1515002 311 8. 50. 23.661 2.1 F1515002 312 8. 60. 16.4226 1.5 F1515002 313 8. 70. 10.8339 1. F1515002 314 8. 80. 8.9 0.8 F1515002 315 8. 90. 7.1896 0.6 F1515002 316 8. 100. 4.86 0.4 F1515002 317 8. 110. 4.757 0.4 F1515002 318 8. 120. 4.56 0.4 F1515002 319 8. 130. 4.3344 0.4 F1515002 320 8. 135. 3.5108 0.3 F1515002 321 8. 140. 3.341 0.3 F1515002 322 8. 150. 3.3 0.3 F1515002 323 8. 160. 3.5 0.3 F1515002 324 8. 170. 2.9841 0.3 F1515002 325 9. 10. 127. 25. F1515002 326 9. 15. 113. 21. F1515002 327 9. 20. 75. 14. F1515002 328 9. 25. 51. 4. F1515002 329 9. 30. 30.7 2.4 F1515002 330 9. 35. 28. 2.2 F1515002 331 9. 40. 26.4 2.1 F1515002 332 9. 45. 26.4 2.1 F1515002 333 9. 50. 21.2 2. F1515002 334 9. 55. 17.8 1.4 F1515002 335 9. 60. 12.4 1. F1515002 336 9. 70. 6.6 0.5 F1515002 337 9. 75. 7.4 0.6 F1515002 338 9. 80. 7.75 0.6 F1515002 339 9. 90. 7.9 0.6 F1515002 340 9. 100. 6.9 0.6 F1515002 341 9. 105. 7.4 0.6 F1515002 342 9. 120. 5.34 0.4 F1515002 343 9. 130. 5.2 0.4 F1515002 344 9. 140. 4.4 0.4 F1515002 345 9. 150. 4.9 0.4 F1515002 346 9. 160. 3.6 0.3 F1515002 347 9. 170. 3.8 0.3 F1515002 348 10. 10. 125. 27. F1515002 349 10. 15. 106. 19. F1515002 350 10. 20. 70. 7. F1515002 351 10. 25. 43. 4. F1515002 352 10. 30. 26. 2. F1515002 353 10. 40. 21. 2. F1515002 354 10. 45. 20. 2.1 F1515002 355 10. 50. 18. 2. F1515002 356 10. 55. 17. 1. F1515002 357 10. 60. 9.2 0.8 F1515002 358 10. 70. 5.3 0.4 F1515002 359 10. 80. 5. 0.4 F1515002 360 10. 90. 5.6 0.5 F1515002 361 10. 100. 5.5 0.5 F1515002 362 10. 110. 5.9 0.5 F1515002 363 10. 120. 6. 0.5 F1515002 364 10. 130. 5. 0.4 F1515002 365 10. 140. 3.9 0.3 F1515002 366 10. 150. 3.7 0.3 F1515002 367 10. 160. 3.5 0.3 F1515002 368 10. 170. 3.7 0.3 F1515002 369 ENDDATA 338 0 F1515002 370 ENDSUBENT 369 0 F151500299999 SUBENT F1515003 20250113 F100F1515003 1 BIB 7 13 F1515003 2 REACTION (4-BE-9(D,X)1-H-3,,SIG) F1515003 3 SAMPLE Self-supporting beryllium target with 658+-33 mu-g/cm2 F1515003 4 thick deposited on a thin SiO backing was used. F1515003 5 DETECTOR (SI,TELES) Six telescopes of dE-E detectors were F1515003 6 used. dE detectors thickness was 12-14 mu-m, F1515003 7 E detectors thickness was 1.2 mm. F1515003 8 METHOD (EDE) F1515003 9 PART-DET (T) F1515003 10 ERR-ANALYS (DATA-ERR) Total error of the cross sections, about 3% F1515003 11 STATUS (TABLE,,L.N.Generalov+,J,BAS,88,1332,2024) Data were F1515003 12 presented by authors. The same on fig. 8 from F1515003 13 Bull.Rus.Ac.Sci.Phys. 88,1332,2024. F1515003 14 (DEP,F1515002) Differential cross sections are given. F1515003 15 ENDBIB 13 0 F1515003 16 NOCOMMON 0 0 F1515003 17 DATA 3 13 F1515003 18 EN DATA DATA-ERR F1515003 19 MEV MB MB F1515003 20 2. 186. 5.58 F1515003 21 3. 217. 6.51 F1515003 22 3.5 183. 5.49 F1515003 23 4. 198. 5.94 F1515003 24 4.5 199. 5.97 F1515003 25 5. 200. 6. F1515003 26 5.5 175. 5.25 F1515003 27 6. 171. 5.13 F1515003 28 6.5 164. 4.92 F1515003 29 7. 186. 5.58 F1515003 30 8. 200. 6. F1515003 31 9. 172. 5.16 F1515003 32 10. 146. 4.38 F1515003 33 ENDDATA 15 0 F1515003 34 ENDSUBENT 33 0 F151500399999 SUBENT F1515004 20250113 F100F1515004 1 BIB 8 42 F1515004 2 REACTION (4-BE-9(D,X)1-H-3,,SIG) F1515004 3 SAMPLE The target was a thick (1 mm) layer of high-purity F1515004 4 beryllium opaque to the beam of deuterons and fast F1515004 5 tritons produced in reaction 9Be(d,xt). F1515004 6 METHOD (ACTIV) Secondary activation method is used. The fast F1515004 7 tritons produced in 9Be(d,xt) reaction interact with F1515004 8 Be nuclei in the same layer where they originate and F1515004 9 9Be(t,a)8Li reaction was induced. F1515004 10 (BCINT) The target was placed in a cylindrical F1515004 11 scattering vacuum chamber (100 mm in diameter with a F1515004 12 steel wall 1 mm thick) that functioned as a Faraday F1515004 13 cup. F1515004 14 (BSPEC) Beta-particles from Li-8 decay were registered.F1515004 15 DETECTOR (SCIN) A plastic scintillator (40 mm in diameter, F1515004 16 h=50 mm) + PMT-93 placed in a lead protective F1515004 17 cylinder (100 mm external diameter, 55 mm internal F1515004 18 diameter and 79 mm high) was used as the F1515004 19 beta-particle detector. The end of the detector's F1515004 20 body was covered with aluminum foil (0.1 mm thick). F1515004 21 The detector was fixed at an angle of 120 degree to F1515004 22 the direction of a beam of accelerated deuterons or F1515004 23 tritons at various distances R from the target. A F1515004 24 window made from lavsan film 0.1 mm thick was in the F1515004 25 chamber's wall in that direction. F1515004 26 RAD-DET (3-LI-8,B-) F1515004 27 ANALYSIS (DECAY) Beta-decay curves from Li-8 were analyzed and F1515004 28 absolute yields Ydx8Li and Ytx8Li were determined. F1515004 29 Linear incident triton energy dependence of Li-8 F1515004 30 yield was assumed to obtain 9Be(d,xt) reaction total F1515004 31 cross section. F1515004 32 ERR-ANALYS (ERR-T) Total error of the cross section. F1515004 33 (ERR-1) Error of the beam current measurement F1515004 34 (ERR-2) Error of the absolute yield of Li-8 nuclei F1515004 35 from secondary reaction 9Be(t,x)8Li F1515004 36 (ERR-3) Error of the absolute yield of Li-8 nuclei F1515004 37 from reaction 9Be(d,x)8Li F1515004 38 (ERR-4) Error of the measurement of the ratio of the F1515004 39 efficiency of recording beta-particles from the 8Li F1515004 40 decay produced in deuteron and triton irradiations F1515004 41 STATUS (TABLE,,L.N.Generalov+,J,BAS,88,1332,2024) Table 3 F1515004 42 from the reference. The same on fig.8 of Bull.Russ. F1515004 43 Ac.Sci.Phys. 88,1332,2024. F1515004 44 ENDBIB 42 0 F1515004 45 COMMON 4 3 F1515004 46 ERR-1 ERR-2 ERR-3 ERR-4 F1515004 47 PER-CENT PER-CENT PER-CENT PER-CENT F1515004 48 2. 4. 7. 6. F1515004 49 ENDCOMMON 3 0 F1515004 50 DATA 3 22 F1515004 51 EN DATA ERR-T F1515004 52 MEV MB MB F1515004 53 1.5 160. 13. F1515004 54 2.25 162. 13. F1515004 55 2.75 182. 15. F1515004 56 3.25 210. 17. F1515004 57 3.75 187. 15. F1515004 58 4.25 225. 18. F1515004 59 4.5 177. 15. F1515004 60 5. 194. 16. F1515004 61 5.5 200. 17. F1515004 62 6. 182. 15. F1515004 63 6.5 182. 15. F1515004 64 7. 176. 15. F1515004 65 7.5 182. 15. F1515004 66 8. 171. 14. F1515004 67 8.5 171. 14. F1515004 68 9. 156. 13. F1515004 69 9.5 129. 11. F1515004 70 10. 144. 12. F1515004 71 10.5 157. 13. F1515004 72 11. 131. 11. F1515004 73 11.5 106. 9. F1515004 74 12. 85. 9. F1515004 75 ENDDATA 24 0 F1515004 76 ENDSUBENT 75 0 F151500499999 ENDENTRY 4 0 F151599999999