ENTRY C2620 20211107 C208C262000000001 SUBENT C2620001 20211107 C208C262000100001 BIB 10 26 C262000100002 TITLE A high-resolution study of isobaric analogue C262000100003 resonances in 41K C262000100004 AUTHOR (G.A.Keyworth,G.C.Kyker Jr,E.G.Bilpuch,H.W.Newson) C262000100005 REFERENCE (J,NP,89,590,1966) C262000100006 #doi:10.1016/0029-5582(66)90934-5 C262000100007 INSTITUTE (1USADKE) C262000100008 FACILITY (VDG,1USADKE) C262000100009 INC-SPECT The effective energy spread in the proton beam itself, C262000100010 in the most favourable cases observed, is 153 eV, C262000100011 before correcting for target thickness, Doppler C262000100012 broadening and the natural width of the resonance. C262000100013 Generally, our total resolution was about 200-250 eV. C262000100014 DETECTOR (SOLST) The detector is at an angle of 135 degrees to C262000100015 the incident beam. The solid angle subtended in this C262000100016 arrangement is about 15 msr. C262000100017 SAMPLE Argon target is on the order of 50 eV thick, C262000100018 operating temperature of 60 degrees K was chosen. C262000100019 ADD-RES Figures with differential cross sections of C262000100020 40Ar(p,p)40Ar and 40Ar(p,alpha)37Cl at 135 degrees at C262000100021 incident proton energies of from 1.63 to 2.60 MeV C262000100022 and 40Ar(p,n)40K at 20 degrees at incident proton C262000100023 energies of from 2.34 to 2.60 MeV (Figs. 4-7) C262000100024 are given in the article, but the quality of the copy C262000100025 available to the compiler is so bad that their C262000100026 digitising is not possible. C262000100027 HISTORY (20210829C) OG C262000100028 ENDBIB 26 0 C262000100029 NOCOMMON 0 0 C262000100030 ENDSUBENT 29 0 C262000199999 SUBENT C2620002 20211107 C208C262000200001 BIB 4 16 C262000200002 REACTION 1(18-AR-40(P,0),,EN) C262000200003 2(18-AR-40(P,0),,J) C262000200004 3(18-AR-40(P,0),,PTY) C262000200005 4(18-AR-40(P,TOT),,WID) C262000200006 5(18-AR-40(P,EL),,WID) C262000200007 6(18-AR-40(P,A),,WID) C262000200008 7(18-AR-40(P,N),,WID) C262000200009 ANALYSIS (AREA,SLA,MLA) C262000200010 ERR-ANALYS (DATA-ERR) No information on source of uncertainty. C262000200011 Relative energies of resonances are accurate to 0.3 keVC262000200012 or better. The partial width for proton capture has C262000200013 been neglected in this analysis. C262000200014 (ERR-1,10.,40.) The proton widths range in precision C262000200015 from about 10% on the widest resonances to about 40% onC262000200016 the very weakest ones. C262000200017 STATUS (TABLE) Tab.1 (p.596) in Nucl.Phys.,89,590,1966. C262000200018 ENDBIB 16 0 C262000200019 COMMON 3 3 C262000200020 DATA-ERR 1DATA-ERR 6DATA-ERR 7 C262000200021 KEV PER-CENT PER-CENT C262000200022 2. 30. 30. C262000200023 ENDCOMMON 3 0 C262000200024 DATA 7 138 C262000200025 DATA 1DATA 2DATA 3DATA 4DATA 5DATA 6C262000200026 DATA 7 C262000200027 MEV NO-DIM NO-DIM EV EV EV C262000200028 EV C262000200029 1.6432 0.5 +1. 20. 20. C262000200030 C262000200031 1.6489 1.5 -1. 6. 5. 1.C262000200032 C262000200033 1.6561 1.5 -1. 35. 35. 1.C262000200034 C262000200035 1.6711 1.5 -1. 25. 25. C262000200036 C262000200037 1.6769 0.5 -1. 40. 40. C262000200038 C262000200039 1.6769 1.5 -1. 20. 20. C262000200040 C262000200041 1.7040 0.5 -1. 25. 25. C262000200042 C262000200043 1.7040 1.5 -1. 15. 15. C262000200044 C262000200045 1.7102 0.5 -1. 100. 100. C262000200046 C262000200047 1.7150 0.5 -1. 50. 50. C262000200048 C262000200049 1.7150 1.5 -1. 35. 35. C262000200050 C262000200051 1.7310 0.5 -1. 32. 30. 2.C262000200052 C262000200053 1.7310 1.5 -1. 21. 20. 1.C262000200054 C262000200055 1.7332 1.5 -1. 60. 60. C262000200056 C262000200057 1.7461 0.5 -1. 80. 80. C262000200058 C262000200059 1.7461 1.5 -1. 50. 50. C262000200060 C262000200061 1.7485 0.5 -1. 75. 70. 5.C262000200062 C262000200063 1.7664 1.5 -1. 20. 20. C262000200064 C262000200065 1.7728 0.5 -1. 34. 30. 4.C262000200066 C262000200067 1.7956 1.5 -1. 100. 100. 1.C262000200068 C262000200069 1.8072 0.5 -1. 50. 50. C262000200070 C262000200071 1.8108 1.5 -1. 40. 40. 1.C262000200072 C262000200073 1.8147 1.5 -1. 150. 150. 1.C262000200074 C262000200075 1.8219 0.5 -1. 23. 18. 5.C262000200076 C262000200077 1.8219 1.5 -1. 12. 10. 2.C262000200078 C262000200079 1.8294 0.5 -1. 60. 60. C262000200080 C262000200081 1.8294 1.5 -1. 40. 40. C262000200082 C262000200083 1.8330 1.5 -1. 46. 45. 1.C262000200084 C262000200085 1.8353 1.5 -1. 70. 70. C262000200086 C262000200087 1.8419 0.5 -1. 100. 100. C262000200088 C262000200089 1.8419 1.5 -1. 70. 70. C262000200090 C262000200091 1.8491 0.5 -1. 357. 350. 7.C262000200092 C262000200093 1.8514 1.5 -1. 30. 30. C262000200094 C262000200095 1.8597 1.5 -1. 800. 800. 4.C262000200096 C262000200097 1.8738 1.5 -1. 1250. 1250. C262000200098 C262000200099 1.8762 0.5 +1. 60. 60. C262000200100 C262000200101 1.8762 1.5 -1. 140. 140. C262000200102 C262000200103 1.8770 1.5 -1. 450. 450. 1.C262000200104 C262000200105 1.8843 1.5 -1. 30. 30. 1.C262000200106 C262000200107 1.8941 1.5 -1. 70. 70. 1.C262000200108 C262000200109 1.8974 1.5 -1. 400. 400. 3.C262000200110 C262000200111 1.9017 0.5 +1. 20. 15. 5.C262000200112 C262000200113 1.9138 0.5 +1. 130. 125. 5.C262000200114 C262000200115 1.9149 0.5 +1. 19. 15. 4.C262000200116 C262000200117 1.9234 0.5 -1. 66. 60. 6.C262000200118 C262000200119 1.9252 1.5 -1. 52. 50. 2.C262000200120 C262000200121 1.9318 0.5 -1. 45. 45. C262000200122 C262000200123 1.9581 0.5 -1. 62. 60. 2.C262000200124 C262000200125 1.9835 0.5 -1. 190. 80. 11.C262000200126 C262000200127 1.9906 0.5 +1. 12. 12. C262000200128 C262000200129 1.9906 1.5 -1. 20. 20. C262000200130 C262000200131 2.0069 0.5 -1. 50. 50. C262000200132 C262000200133 2.0099 0.5 +1. 70. 70. C262000200134 C262000200135 2.0338 0.5 -1. 53. 50. C262000200136 C262000200137 2.0338 0.5 +1. 100. 100. C262000200138 C262000200139 2.0338 1.5 -1. 175. 175. C262000200140 C262000200141 2.0378 1.5 -1. 40. 35. 5.C262000200142 C262000200143 2.0450 0.5 -1. 23. 20. 3.C262000200144 C262000200145 2.0628 0.5 -1. 130. 130. C262000200146 C262000200147 2.0826 0.5 -1. 150. 150. 2.C262000200148 C262000200149 2.0871 1.5 -1. 155. 155. 1.C262000200150 C262000200151 2.0990 1.5 -1. 70. 70. 1.C262000200152 C262000200153 2.1080 0.5 -1. 114. 110. 4.C262000200154 C262000200155 2.1211 1.5 -1. 21. 20. 1.C262000200156 C262000200157 2.1235 0.5 +1. 23. 20. 3.C262000200158 C262000200159 2.1235 1.5 -1. 36. 35. 1.C262000200160 C262000200161 2.1290 1.5 -1. 69. 60. 9.C262000200162 C262000200163 2.1456 1.5 -1. 70. 70. C262000200164 C262000200165 2.1511 0.5 -1. 29. 22. 7.C262000200166 C262000200167 2.1543 0.5 +1. 60. 60. C262000200168 C262000200169 2.1713 0.5 -1. 60. 60. C262000200170 C262000200171 2.1762 0.5 -1. 50. 50. C262000200172 C262000200173 2.1851 0.5 -1. 120. 120. C262000200174 C262000200175 2.1851 1.5 -1. 70. 70. C262000200176 C262000200177 2.2102 0.5 +1. 60. 60. C262000200178 C262000200179 2.2160 0.5 +1. 110. 110. C262000200180 C262000200181 2.2302 0.5 -1. 300. 300. C262000200182 C262000200183 2.2462 0.5 +1. 50. 50. C262000200184 C262000200185 2.2643 1.5 -1. 22. 20. 2.C262000200186 C262000200187 2.2662 0.5 +1. 210. 210. C262000200188 C262000200189 2.2770 0.5 +1. 20. 15. 5.C262000200190 C262000200191 2.2815 0.5 +1. 42. 40. 2.C262000200192 C262000200193 2.2901 1.5 +1. 90. 30. 60.C262000200194 C262000200195 2.2914 1.5 -1. 30. 30. C262000200196 C262000200197 2.3012 0.5 +1. 15. 15. C262000200198 C262000200199 2.3048 0.5 -1. 220. 220. 1.C262000200200 C262000200201 2.3107 1.5 +1. 80. 30. 50.C262000200202 C262000200203 2.3166 0.5 -1. 70. 70. C262000200204 C262000200205 2.3204 0.5 +1. 65. 65. C262000200206 C262000200207 2.3258 1.5 +1. 31. 30. 1.C262000200208 C262000200209 2.3299 0.5 +1. 51. 50. 1.C262000200210 C262000200211 2.3466 0.5 +1. 275. 275. C262000200212 C262000200213 2.3542 0.5 +1. 200. 200. C262000200214 C262000200215 2.3575 0.5 -1. 830. 830. C262000200216 C262000200217 2.3601 0.5 -1. 130. 130. 1.C262000200218 C262000200219 2.3739 0.5 -1. 65. 55. 10.C262000200220 C262000200221 2.3830 0.5 +1. 150. 140. 9.C262000200222 C262000200223 2.3901 0.5 -1. 40. 35. 5.C262000200224 C262000200225 2.4034 0.5 +1. 77. 70. 4.C262000200226 3. C262000200227 2.4042 0.5 -1. 100. 100. 1.C262000200228 C262000200229 2.4107 0.5 +1. 150. 150. 3.C262000200230 C262000200231 2.4127 0.5 -1. 250. 250. 1.C262000200232 C262000200233 2.4163 0.5 -1. 75. 70. 5.C262000200234 C262000200235 2.4349 0.5 +1. 600. 600. C262000200236 C262000200237 2.4449 1.5 -1. 750. 750. 6.C262000200238 1. C262000200239 2.4507 0.5 +1. 1000. 1000. 13.C262000200240 C262000200241 2.4535 0.5 +1. 750. 750. C262000200242 C262000200243 2.4558 1.5 -1. 150. 140. 9.C262000200244 2. C262000200245 2.4605 0.5 -1. 80. 40. 5.C262000200246 35. C262000200247 2.4642 0.5 +1. 360. 340. 18.C262000200248 C262000200249 2.4727 0.5 -1. 410. 410. C262000200250 1. C262000200251 2.4804 0.5 +1. 175. 170. 6.C262000200252 C262000200253 2.4804 1.5 -1. 270. 270. 2.C262000200254 C262000200255 2.4818 0.5 -1. 100. 90. 11.C262000200256 C262000200257 2.4863 1.5 -1. 230. 225. 6.C262000200258 C262000200259 2.4918 0.5 -1. 80. 40. 25.C262000200260 15. C262000200261 2.4955 1.5 -1. 45. 25. 15.C262000200262 5. C262000200263 2.5000 0.5 -1. 1400. 1400. 9.C262000200264 C262000200265 2.5021 1.5 -1. 190. 175. 7.C262000200266 6. C262000200267 2.5111 0.5 +1. 200. 45. 125.C262000200268 30. C262000200269 2.5210 0.5 +1. 70. 50. 15.C262000200270 5. C262000200271 2.5314 1.5 -1. 35. 25. 4.C262000200272 6. C262000200273 2.5446 0.5 -1. 200. 40. 100.C262000200274 60. C262000200275 2.5446 1.5 -1. 70. 20. 30.C262000200276 20. C262000200277 2.5459 0.5 -1. 60. 35. 12.C262000200278 13. C262000200279 2.5459 1.5 -1. 35. 25. 5.C262000200280 5. C262000200281 2.5489 0.5 -1. 100. 90. 4.C262000200282 6. C262000200283 2.5570 0.5 -1. 250. 180. 53.C262000200284 15. C262000200285 2.5590 0.5 +1. 30. 25. 5.C262000200286 C262000200287 2.5599 0.5 -1. 170. 55. 15.C262000200288 100. C262000200289 2.5686 0.5 +1. 45. 40. 5.C262000200290 C262000200291 2.5816 1.5 -1. 270. 250. 13.C262000200292 4. C262000200293 2.5878 0.5 -1. 50. 30. 10.C262000200294 10. C262000200295 2.5938 0.5 +1. 43. 40. 3.C262000200296 C262000200297 2.5956 0.5 -1. 650. 650. 2.C262000200298 C262000200299 2.5975 0.5 +1. 175. 175. 1.C262000200300 C262000200301 2.5998 0.5 -1. 140. 90. 47.C262000200302 C262000200303 2.6020 1.5 +1. 125. 75. 35.C262000200304 15. C262000200305 ENDDATA 280 0 C262000200306 ENDSUBENT 305 0 C262000299999 ENDENTRY 2 0 C262099999999