ENTRY D5065 20110913 D079D506500000001 SUBENT D5065001 20110913 D079D506500100001 BIB 12 49 D506500100002 TITLE Energy distribution of the E1-transition strengths in D506500100003 the 46Ti nucleus D506500100004 AUTHOR (I.D.Fedorets,S.S.Ratkevich) D506500100005 INSTITUTE (4UKRKHU) D506500100006 REFERENCE (J,YF,71,1353,2008) D506500100007 (J,PAN,71,1325,2008) D506500100008 #doi:10.1134/S1063778808080024 D506500100009 #NSR 2008FE15 D506500100010 FACILITY (VDG,4UKRKFT)measurements were performed at an D506500100011 electrostatic accelerator in the range of incident- D506500100012 proton energies between 1.2 and 3.1MeV, the step in D506500100013 energy being variable and equal to the proton energy D506500100014 loss in a target. D506500100015 METHOD (SITA,EXTB) D506500100016 DETECTOR (GELI,NAICR) The spectra of gamma rays were measured byD506500100017 a pair spectrometer that consisted of Ge(Li) detector D506500100018 63 cm3 in volume surrounded by a four-section ring D506500100019 NaI(Tl)detector. D506500100020 SAMPLE Scandium films 1.2 and 1.7 micro-m thick obtained D506500100021 according to a procedure within which a thermal D506500100022 reduction of the scandium oxide Sc2O3 with thorium in D506500100023 a vacuum was followed by evaporation in a vacuum D506500100024 onto a tantalum substrate were used as targets. D506500100025 ADD-RES (STRUC,COMP) Radiative strength functions for E1 D506500100026 transitions populating these states are determined. TheD506500100027 resulting data are compared with predictions of variousD506500100028 models. D506500100029 ERR-ANALYS (ERR-T) total error includes: D506500100030 (ERR-1) uncertainty in the absolute efficiency of the D506500100031 pair gamma spectrometer D506500100032 (ERR-S) statistical error D506500100033 (ERR-2) the errors in determining the target thickness D506500100034 (ERR-3) the errors in the charge deposited onto D506500100035 the target D506500100036 COMMENT The proton energy losses in a target were 40 to 80 keV D506500100037 in the energy range under study, and this in fact D506500100038 determined the widths of gamma lines in the spectra. D506500100039 For the degree of averaging to be adequate, the spectraD506500100040 of gamma rays measured at different proton energies D506500100041 were shifted in energy until the positions of gamma D506500100042 lines corresponding to primary gamma transitions becameD506500100043 coincident, whereupon the spectra in question were D506500100044 summed. Primary transition intensities averaged over D506500100045 many compound nucleus resonances were determined via D506500100046 this summation of the spectra. Summation of six spectraD506500100047 led to the averaging interval deltaEp = 320 keV at Ep =D506500100048 2.63 MeV. D506500100049 HISTORY (20090109C)UKRNDC D506500100050 (20110203U) VS. DOI identifier corrected D506500100051 ENDBIB 49 0 D506500100052 COMMON 6 3 D506500100053 EN EN-RSL ERR-S ERR-1 ERR-2 ERR-3 D506500100054 MEV MEV PER-CENT PER-CENT PER-CENT PER-CENT D506500100055 2.63 0.320 8.0 15.0 5.0 5.0 D506500100056 ENDCOMMON 3 0 D506500100057 ENDSUBENT 56 0 D506500199999 SUBENT D5065002 20110913 D079D506500200001 BIB 4 4 D506500200002 REACTION (21-SC-45(P,G)22-TI-46,PAR,SIG) D506500200003 EN-SEC (E-LVL,22-TI-46) D506500200004 STATUS (TABLE) Table from text D506500200005 HISTORY (20110909A) VS. E-LVL(-ERR): MEV -> KEV. D506500200006 ENDBIB 4 0 D506500200007 NOCOMMON 0 0 D506500200008 DATA 4 51 D506500200009 E-LVL E-LVL-ERR DATA ERR-T D506500200010 KEV KEV MICRO-B MICRO-B D506500200011 0.0 1.0 1.0 D506500200012 889. 2. 21. 4. D506500200013 2010. 2. 43. 9. D506500200014 2962. 4. 6. 1. D506500200015 3059. 4. 17. 3. D506500200016 3236. 5. 5. 1. D506500200017 3299. 4. 16. 3. D506500200018 3441. 5. 19. 4. D506500200019 3569. 5. 11. 2. D506500200020 3580. 4. 16. 3. D506500200021 3610. 5. 3. 1. D506500200022 3677. 5. 4. 1. D506500200023 3724. 3. 14. 3. D506500200024 3826. 5. 19. 4. D506500200025 3845. 5. 3. 1. D506500200026 3852. 4. 20. 4. D506500200027 3889. 5. 5. 1. D506500200028 3906. 5. 3. 1. D506500200029 3942. 4. 13. 3. D506500200030 4003. 5. 10. 2. D506500200031 4025. 5. 3. 1. D506500200032 4039. 5. 9. 2. D506500200033 4130. 8. 3. 1. D506500200034 4179. 8. 6. 1. D506500200035 4192. 8. 7. 1. D506500200036 4323. 15. 11. 1. D506500200037 4372. 4. 6. 1. D506500200038 4417. 4. 17. 4. D506500200039 4523. 4. 11. 2. D506500200040 4527. 5. 11. 2. D506500200041 4617. 7. 3. 1. D506500200042 4662. 5. 14. 3. D506500200043 4697. 5. 8. 2. D506500200044 4726. 5. 17. 4. D506500200045 4791. 14. 8. 2. D506500200046 4827. 5. 7. 2. D506500200047 4845. 8. 3. 1. D506500200048 4950. 12. 2. 1. D506500200049 5024. 5. 8. 2. D506500200050 5079. 5. 11. 2. D506500200051 5154. 10. 2. 1. D506500200052 5180. 10. 9. 2. D506500200053 5206. 10. 3. 1. D506500200054 5230. 12. 2. 1. D506500200055 5280. 5. 9. 2. D506500200056 5313. 12. 11. 2. D506500200057 5361. 12. 10. 2. D506500200058 5409. 20. 4. 1. D506500200059 5515. 11. 2. 1. D506500200060 5530. 10. 9. 2. D506500200061 5550. 10. 39. 8. D506500200062 ENDDATA 53 0 D506500200063 ENDSUBENT 62 0 D506500299999 ENDENTRY 2 0 D506599999999