ENTRY F1466 20220825 F094F1466 0 1 SUBENT F1466001 20220825 F094F1466 1 1 BIB 14 54 F1466 1 2 TITLE Measurement of cross sections for the reactions F1466 1 3 232Th(3He,p4n)230Pa, 232Th(3He,p2n)232Pa, and F1466 1 4 232Th(3He,2p+pn)233Pa induced by the irradiation of F1466 1 5 a ThO2 target with 3He nuclei F1466 1 6 AUTHOR (M.N.German,V.A.Zagryadskiy,A.V.Kurochkin, F1466 1 7 K.A.Makoveeva,T.Yu.Malamut,V.I.Novikov,I.I.Skobelin, F1466 1 8 V.N.Unezhev) F1466 1 9 INSTITUTE (4RUSKUR) F1466 1 10 REFERENCE (J,PAN,85,12,2022) English translation F1466 1 11 #doi:10.1134/S1063778821060053 F1466 1 12 (J,YF,85,14,2022) Russian original F1466 1 13 #doi:10.31857/S0044002721060052 F1466 1 14 FACILITY (CYCLO,4RUSKUR) U-150 cyclotron F1466 1 15 METHOD (ACTIV) The activity of each protoactinium F1466 1 16 radionuclide was measured several times during three F1466 1 17 half-life periods and determined on the basis of the F1466 1 18 peaks of total photon absorption. F1466 1 19 (STTA) Eleven foils were combined into one single F1466 1 20 stack of targets. F1466 1 21 (EDEG) Aluminum foils with a thickness from 9 to 30 F1466 1 22 mu-m were placed between thorium targets, using as F1466 1 23 beam monitors or degraders. F1466 1 24 (GSPEC) F1466 1 25 INC-SOURCE Average beam current was 0.1 mu-A. Irradiation was F1466 1 26 carried out until a total charge of 0.3 mu-A h was F1466 1 27 reached. F1466 1 28 DETECTOR (HPGE) The measurements were performed on gamma F1466 1 29 spectrometer with ultrapure-germanium detector ORTEC. F1466 1 30 The distance from the target to the detector during F1466 1 31 measurements was from 6 to 40 cm, depending on the F1466 1 32 radiation intensity. F1466 1 33 SAMPLE Targets of thorium oxide with the thickness from 7 to F1466 1 34 11 mg/cm2 and spot diameter of 20 mm deposited by F1466 1 35 means of sedimentation on aluminum foils were used. F1466 1 36 REL-REF (R,,E.Browne+,J,NDS,113,2113,2012)Decay data for Th-230F1466 1 37 are given. F1466 1 38 (R,,E.Browne+,J,NDS,107,2579,2006) Decay data for U-232F1466 1 39 are given. F1466 1 40 (R,,B.Singh+,J,NDS,170,499,2020) Decay data for U-233 F1466 1 41 are given. F1466 1 42 ADD-RES (COMP) Experimental results were compared with F1466 1 43 theoretical data from TENDL-2019. F1466 1 44 ERR-ANALYS (ERR-T) Uncertainties in the experimental values of F1466 1 45 the cross sections were between 13 and 25 % at a F1466 1 46 fiducial probability of 68 % and include: F1466 1 47 (ERR-1,8.,12.) the error in determining the detector F1466 1 48 efficiency; F1466 1 49 (ERR-2,10.,15.) the error in determining the areas F1466 1 50 under the peaks of total photon absorption in the F1466 1 51 spectrum; F1466 1 52 (ERR-3,3.,18.) the error in the quantum yields used F1466 1 53 to determine the activities. F1466 1 54 STATUS (APRVD) Entry was approved by Dr. K.A.Makoveeva F1466 1 55 HISTORY (20220825C) F1466 1 56 ENDBIB 54 0 F1466 1 57 NOCOMMON 0 0 F1466 1 58 ENDSUBENT 57 0 F1466 199999 SUBENT F1466002 20220825 F094F1466 2 1 BIB 4 5 F1466 2 2 REACTION (90-TH-232(HE3,X)91-PA-230,,SIG) F1466 2 3 RAD-DET (90-TH-230,DG) F1466 2 4 DECAY-DATA (91-PA-230,17.4D) F1466 2 5 (90-TH-230,,DG,951.88,0.296) F1466 2 6 STATUS (TABLE) Tbl.1 from Phys.At.Nuclei, 85,12,2022 F1466 2 7 ENDBIB 5 0 F1466 2 8 NOCOMMON 0 0 F1466 2 9 DATA 3 11 F1466 2 10 EN DATA ERR-T F1466 2 11 MEV MB MB F1466 2 12 57.1 46. 7. F1466 2 13 55.5 37. 8. F1466 2 14 53.8 39. 7. F1466 2 15 52.1 43. 9. F1466 2 16 50.4 34. 8. F1466 2 17 48.5 34. 8. F1466 2 18 46.7 24. 6. F1466 2 19 45.1 20. 5. F1466 2 20 43.3 12. 3. F1466 2 21 41.5 8. 2. F1466 2 22 39.5 5. 1. F1466 2 23 ENDDATA 13 0 F1466 2 24 ENDSUBENT 23 0 F1466 299999 SUBENT F1466003 20220825 F094F1466 3 1 BIB 4 4 F1466 3 2 REACTION (90-TH-232(HE3,X)91-PA-232,,SIG) F1466 3 3 RAD-DET (92-U-232,DG) F1466 3 4 DECAY-DATA (92-U-232,,DG,894.35,0.196) F1466 3 5 STATUS (TABLE) Tbl.1 from Phys.At.Nuclei, 85,12,2022 F1466 3 6 ENDBIB 4 0 F1466 3 7 NOCOMMON 0 0 F1466 3 8 DATA 3 11 F1466 3 9 EN DATA ERR-T F1466 3 10 MEV MB MB F1466 3 11 57.1 53. 11. F1466 3 12 55.5 43. 9. F1466 3 13 53.8 54. 10. F1466 3 14 52.1 67. 12. F1466 3 15 50.4 59. 10. F1466 3 16 48.5 88. 15. F1466 3 17 46.7 80. 13. F1466 3 18 45.1 94. 15. F1466 3 19 43.3 84. 13. F1466 3 20 41.5 97. 15. F1466 3 21 39.5 105. 16. F1466 3 22 ENDDATA 13 0 F1466 3 23 ENDSUBENT 22 0 F1466 399999 SUBENT F1466004 20220825 F094F1466 4 1 BIB 4 4 F1466 4 2 REACTION (90-TH-232(HE3,X)91-PA-233,,SIG) F1466 4 3 RAD-DET (92-U-233,DG) F1466 4 4 DECAY-DATA (92-U-233,,DG,311.9,0.382) F1466 4 5 STATUS (TABLE) Tbl.1 from Phys.At.Nuclei, 85,12,2022 F1466 4 6 ENDBIB 4 0 F1466 4 7 NOCOMMON 0 0 F1466 4 8 DATA 3 11 F1466 4 9 EN DATA ERR-T F1466 4 10 MEV MB MB F1466 4 11 57.1 38. 9. F1466 4 12 55.5 46. 11. F1466 4 13 53.8 47. 10. F1466 4 14 52.1 64. 14. F1466 4 15 50.4 58. 12. F1466 4 16 48.5 75. 14. F1466 4 17 46.7 67. 12. F1466 4 18 45.1 75. 13. F1466 4 19 43.3 62. 10. F1466 4 20 41.5 65. 12. F1466 4 21 39.5 65. 11. F1466 4 22 ENDDATA 13 0 F1466 4 23 ENDSUBENT 22 0 F1466 499999 ENDENTRY 4 0 F146699999999