ENTRY F1526 20250120 F100F1526000 1 SUBENT F1526001 20250120 F100F1526001 1 BIB 13 29 F1526001 2 TITLE Measurement of the cross-sections for the formation F1526001 3 of lanthanum radioisotopes in proton induced reactions F1526001 4 on Ba-135 nuclei up to 30 MeV F1526001 5 AUTHOR (I.A.Khomenko,E.S.Kormazeva,V.I.Novikov,R.A.Aliev) F1526001 6 REFERENCE (J,BLI,51,515,2024) English translation F1526001 7 #doi:10.3103/S1068335624601869 F1526001 8 (J,KSF,51,35,2024) Russian original F1526001 9 INSTITUTE (4RUSKUR) F1526001 10 FACILITY (ISOCY,4RUSKUR) U-150 cyclotron F1526001 11 INC-SOURCE Beam current was 191+-12 nA. F1526001 12 SAMPLE (56-BA-135,ENR=0.949) Thin targets of 135BaCO3 F1526001 13 (1.9-4.5 mg/cm2) of isotopic composition 135Ba F1526001 14 (135Ba-94.9%, 136Ba-2.31%, 138Ba-2.01%, 137Ba-0.59%, F1526001 15 134Ba-0.19%) were deposited on an aluminum substrate F1526001 16 (~30 mu-m) by sedimentation method from a suspension F1526001 17 with acetone and collodium. F1526001 18 DETECTOR (HPGE) Gamma spectrometer with an ORTEC GEM 35P4 high F1526001 19 purity germanium was used. F1526001 20 METHOD (STTA,EDEG) Aluminum degraders were placed in a stack F1526001 21 between 7 targets. F1526001 22 (ACTIV) Irradiation time was 30 min. Each target of F1526001 23 135Ba was measured 2-3 times within 2-3 days after the F1526001 24 irradiation. F1526001 25 MONITOR (29-CU-0(P,X)30-ZN-62,,SIG) F1526001 26 (29-CU-0(P,X)30-ZN-65,,SIG) F1526001 27 ADD-RES (COMP) The measured excitation functions were compared F1526001 28 with the data from TENDL-2023 library. F1526001 29 STATUS (APRVD) Entry was approved by Dr. I.A.Khomenko. F1526001 30 HISTORY (20250120C) F1526001 31 ENDBIB 29 0 F1526001 32 NOCOMMON 0 0 F1526001 33 ENDSUBENT 32 0 F152600199999 SUBENT F1526002 20250120 F100F1526002 1 BIB 4 11 F1526002 2 REACTION (56-BA-135(P,3N)57-LA-133,,SIG) F1526002 3 DECAY-DATA (57-LA-133,3.912HR,DG,278.8,0.0244) F1526002 4 ERR-ANALYS (ERR-T) Cross section uncertainties were calculated F1526002 5 as the square root of the sum of the squares of the F1526002 6 individual relative uncertainties and took into accountF1526002 7 (ERR-1) uncertainty of calibration; F1526002 8 (ERR-2) uncertainty of target thickness; F1526002 9 (ERR-3) uncertainty of proton current; F1526002 10 (ERR-4) uncertainty of nuclear data; F1526002 11 (ERR-5,3.,32.) uncertainty of photopeak area. F1526002 12 STATUS (TABLE,,I.A.Khomenko+,J,BLI,51,515,2024) Table 2 F1526002 13 ENDBIB 11 0 F1526002 14 COMMON 4 3 F1526002 15 ERR-1 ERR-2 ERR-3 ERR-4 F1526002 16 PER-CENT PER-CENT PER-CENT PER-CENT F1526002 17 5. 10. 6. 1. F1526002 18 ENDCOMMON 3 0 F1526002 19 DATA 4 3 F1526002 20 EN EN-ERR DATA ERR-T F1526002 21 MEV MEV MB MB F1526002 22 29.8 0.5 1214.8 136.8 F1526002 23 25.0 0.7 1005.2 113.5 F1526002 24 19.8 1.0 15.7 9.7 F1526002 25 ENDDATA 5 0 F1526002 26 ENDSUBENT 25 0 F152600299999 SUBENT F1526003 20250120 F100F1526003 1 BIB 4 11 F1526003 2 REACTION (56-BA-135(P,N)57-LA-135,,SIG) F1526003 3 DECAY-DATA (57-LA-135,19.5HR,DG,480.5,0.0152) F1526003 4 ERR-ANALYS (ERR-T) Cross section uncertainties were calculated F1526003 5 as the square root of the sum of the squares of the F1526003 6 individual relative uncertainties and took into accountF1526003 7 (ERR-1) uncertainty of calibration; F1526003 8 (ERR-2) uncertainty of target thickness; F1526003 9 (ERR-3) uncertainty of proton current; F1526003 10 (ERR-4) uncertainty of nuclear data; F1526003 11 (ERR-5,3.,32.) uncertainty of photopeak area. F1526003 12 STATUS (TABLE,,I.A.Khomenko+,J,BLI,51,515,2024) Table 2 F1526003 13 ENDBIB 11 0 F1526003 14 COMMON 4 3 F1526003 15 ERR-1 ERR-2 ERR-3 ERR-4 F1526003 16 PER-CENT PER-CENT PER-CENT PER-CENT F1526003 17 5. 10. 6. 1. F1526003 18 ENDCOMMON 3 0 F1526003 19 DATA 4 7 F1526003 20 EN EN-ERR DATA ERR-T F1526003 21 MEV MEV MB MB F1526003 22 29.8 0.5 71.2 11.3 F1526003 23 25.0 0.7 107.7 15.5 F1526003 24 19.8 1.0 121.3 16.5 F1526003 25 12.1 1.5 783.9 91.0 F1526003 26 9.5 1.7 423.5 51.9 F1526003 27 6.7 2.2 61.8 12.0 F1526003 28 3.5 3.0 3.3 2.0 F1526003 29 ENDDATA 9 0 F1526003 30 ENDSUBENT 29 0 F152600399999 SUBENT F1526004 20250120 F100F1526004 1 BIB 4 11 F1526004 2 REACTION (56-BA-135(P,X)56-BA-133-M,CUM,SIG) F1526004 3 DECAY-DATA (56-BA-133-M,38.93HR,DG,275.9,0.177) F1526004 4 ERR-ANALYS (ERR-T) Cross section uncertainties were calculated F1526004 5 as the square root of the sum of the squares of the F1526004 6 individual relative uncertainties and took into accountF1526004 7 (ERR-1) uncertainty of calibration; F1526004 8 (ERR-2) uncertainty of target thickness; F1526004 9 (ERR-3) uncertainty of proton current; F1526004 10 (ERR-4) uncertainty of nuclear data; F1526004 11 (ERR-5,3.,32.) uncertainty of photopeak area. F1526004 12 STATUS (TABLE,,I.A.Khomenko+,J,BLI,51,515,2024) Table 2 F1526004 13 ENDBIB 11 0 F1526004 14 COMMON 4 3 F1526004 15 ERR-1 ERR-2 ERR-3 ERR-4 F1526004 16 PER-CENT PER-CENT PER-CENT PER-CENT F1526004 17 5. 10. 6. 1. F1526004 18 ENDCOMMON 3 0 F1526004 19 DATA 4 3 F1526004 20 EN EN-ERR DATA ERR-T F1526004 21 MEV MEV MB MB F1526004 22 29.8 0.5 39.5 4.6 F1526004 23 25.0 0.7 9.6 1.3 F1526004 24 19.8 1.0 0.7 0.5 F1526004 25 ENDDATA 5 0 F1526004 26 ENDSUBENT 25 0 F152600499999 SUBENT F1526005 20250120 F100F1526005 1 BIB 4 11 F1526005 2 REACTION (56-BA-135(P,INL)56-BA-135-M,,SIG) F1526005 3 DECAY-DATA (56-BA-135-M,28.7HR,DG,268.2,0.016) F1526005 4 ERR-ANALYS (ERR-T) Cross section uncertainties were calculated F1526005 5 as the square root of the sum of the squares of the F1526005 6 individual relative uncertainties and took into accountF1526005 7 (ERR-1) uncertainty of calibration; F1526005 8 (ERR-2) uncertainty of target thickness; F1526005 9 (ERR-3) uncertainty of proton current; F1526005 10 (ERR-4) uncertainty of nuclear data; F1526005 11 (ERR-5,3.,32.) uncertainty of photopeak area. F1526005 12 STATUS (TABLE,,I.A.Khomenko+,J,BLI,51,515,2024) Table 2 F1526005 13 ENDBIB 11 0 F1526005 14 COMMON 4 3 F1526005 15 ERR-1 ERR-2 ERR-3 ERR-4 F1526005 16 PER-CENT PER-CENT PER-CENT PER-CENT F1526005 17 5. 10. 6. 1. F1526005 18 ENDCOMMON 3 0 F1526005 19 DATA 4 7 F1526005 20 EN EN-ERR DATA ERR-T F1526005 21 MEV MEV MB MB F1526005 22 29.8 0.5 41.9 4.9 F1526005 23 25.0 0.7 45.3 5.3 F1526005 24 19.8 1.0 36.4 4.3 F1526005 25 12.1 1.5 10.4 1.4 F1526005 26 9.5 1.7 3.4 0.9 F1526005 27 6.7 2.2 1.4 0.6 F1526005 28 3.5 3.0 1.9 0.4 F1526005 29 ENDDATA 9 0 F1526005 30 ENDSUBENT 29 0 F152600599999 SUBENT F1526006 20250120 F100F1526006 1 BIB 4 6 F1526006 2 REACTION (56-BA-135(P,N)57-LA-135,,TTY,,PHY,DERIV) F1526006 3 DECAY-DATA (57-LA-135,19.5HR,DG,480.5,0.0152) F1526006 4 ANALYSIS (INTEF) F1526006 5 STATUS (TABLE,,I.A.Khomenko+,J,BLI,51,515,2024) Data from F1526006 6 text p. 516. F1526006 7 (DEP,F1526003) Excitation function F1526006 8 ENDBIB 6 0 F1526006 9 NOCOMMON 0 0 F1526006 10 DATA 3 1 F1526006 11 EN-MAX EN-MIN DATA F1526006 12 MEV MEV MBQ/MUAHR F1526006 13 29.8 3.5 428. F1526006 14 ENDDATA 3 0 F1526006 15 ENDSUBENT 14 0 F152600699999 SUBENT F1526007 20250120 F100F1526007 1 BIB 4 6 F1526007 2 REACTION (56-BA-135(P,3N)57-LA-133,,TTY,,PHY,DERIV) F1526007 3 DECAY-DATA (57-LA-133,3.912HR,DG,278.8,0.0244) F1526007 4 ANALYSIS (INTEF) F1526007 5 STATUS (TABLE,,I.A.Khomenko+,J,BLI,51,515,2024) Data from F1526007 6 text p. 516. F1526007 7 (DEP,F1526002) Excitation function F1526007 8 ENDBIB 6 0 F1526007 9 NOCOMMON 0 0 F1526007 10 DATA 3 1 F1526007 11 EN-MAX EN-MIN DATA F1526007 12 MEV MEV GBQ/MUAHR F1526007 13 29.8 19.8 3.9 F1526007 14 ENDDATA 3 0 F1526007 15 ENDSUBENT 14 0 F152600799999 ENDENTRY 7 0 F152699999999