ENTRY G4089 20210602 G047G408900000001 SUBENT G4089001 20210602 G047G408900100001 BIB 10 17 G408900100002 TITLE Study of the cross sections for (gamma,n) -reactions G408900100003 on p-nuclei 120Te, 136Ce in the giant E1-resonance G408900100004 energy region G408900100005 AUTHOR (V.M.Mazur,Z.M.Bigan,P.S.Derechkey,V.A.Zheltonozhsky, G408900100006 A.M.Savrasov) G408900100007 INSTITUTE (4UKRIJD,4UKRIEP) G408900100008 REFERENCE (J,YFE,20,228,2019) G408900100009 #doi:10.15407/jnpae2019.03.228 G408900100010 INC-SOURCE (BRST) G408900100011 FACILITY (MICRT,4UKRIEP) The M-30 microtron G408900100012 METHOD (ACTIV) Induced gamma-activity was measured. G408900100013 DETECTOR (HPGE) The resolution of the detector was about 2 keV G408900100014 for gamma lines 1.173 and 1.332 MeV G408900100015 ADD-RES (COMP) Experimental data are compared with theoretical G408900100016 predictions calculated with TALYS-1.9 code. G408900100017 HISTORY (20200914R) Data were received from A.M.Savrasov. G408900100018 (20200915C)UkrNDC G408900100019 ENDBIB 17 0 G408900100020 NOCOMMON 0 0 G408900100021 ENDSUBENT 20 0 G408900199999 SUBENT G4089002 20210602 G047G408900200001 BIB 6 17 G408900200002 REACTION ((52-TE-120(G,N)52-TE-119,,SIG,,BRA)/ G408900200003 (52-TE-130(G,N)52-TE-129,,SIG,,BRA)) G408900200004 SAMPLE Disks of vitreous TeO2 with a diameter of 25 mm and G408900200005 2 mm thick. G408900200006 DECAY-DATA (52-TE-119-M,4.70D,DG,1212.,0.661) G408900200007 (52-TE-119-G,16.05HR,DG,644.,0.840) G408900200008 (52-TE-129-M,33.6D,DG,696.,0.0306) G408900200009 wrongly printed as 33.6 hr in the article table G408900200010 (52-TE-129-G,69.3MIN,DG,459.,0.077) G408900200011 REL-REF (R,,R.B.Firestone+,B,FIRESTONE,,,1996) G408900200012 ERR-ANALYS (ERR-1,,0.5) The standard error is less 0.5% and does G408900200013 not exceed the size of the point. G408900200014 (ERR-2,,0.05) Determination of the mass of the samples.G408900200015 (ERR-3) Detector efficiency 2%. G408900200016 (ERR-4,,0.5) Half-life <= 0.5%. G408900200017 (ERR-5,,1.) Gamma line intensity <= 1%. G408900200018 STATUS (TABLE) Fig.2a in Yad.Fiz. ta Energetika,20,228,2019 G408900200019 ENDBIB 17 0 G408900200020 COMMON 1 3 G408900200021 ERR-3 G408900200022 PER-CENT G408900200023 2. G408900200024 ENDCOMMON 3 0 G408900200025 DATA 2 16 G408900200026 EN-MAX DATA G408900200027 MEV NO-DIM G408900200028 11.0 0.11 G408900200029 11.5 0.20 G408900200030 12.0 0.29 G408900200031 12.5 0.38 G408900200032 13.0 0.46 G408900200033 13.5 0.51 G408900200034 14.0 0.56 G408900200035 14.5 0.58 G408900200036 15.0 0.62 G408900200037 15.5 0.64 G408900200038 16.0 0.68 G408900200039 16.5 0.70 G408900200040 17.0 0.73 G408900200041 17.5 0.76 G408900200042 18.0 0.79 G408900200043 18.5 0.82 G408900200044 ENDDATA 18 0 G408900200045 ENDSUBENT 44 0 G408900299999 SUBENT G4089003 20210602 G047G408900300001 BIB 7 11 G408900300002 REACTION (52-TE-120(G,N)52-TE-119,,SIG,,BRS) G408900300003 MONITOR (52-TE-130(G,N)52-TE-129,,SIG,,BRS) G408900300004 MONIT-REF ((MONIT)G4042001,V.M.Mazur+,J,PR/C,87,044604,2013) G408900300005 ANALYSIS Unfolding was carried out by the inverse matrix method G408900300006 ADD-RES The following parameter values were obtained as a G408900300007 result of fitting for reaction 120Te(gamma,n)119Te: G408900300008 Sigma0 = 262.0+-2.0 mb, E0 = 15.4+-0.1 MeV, G408900300009 Width0 = 5.33+-0.10 MeV. G408900300010 ERR-ANALYS (DATA-ERR) No information on sources of uncertainties G408900300011 STATUS (DEP,G4089002) G408900300012 (TABLE) Fig.3a in Yad.Fiz. ta Energetika,20,228,2019 G408900300013 ENDBIB 11 0 G408900300014 NOCOMMON 0 0 G408900300015 DATA 3 24 G408900300016 EN DATA DATA-ERR G408900300017 MEV MB MB G408900300018 10.25 0.41 G408900300019 10.50 3.34 2.0 G408900300020 10.75 14.90 4.0 G408900300021 11.00 22.28 6.0 G408900300022 11.25 29.40 7.0 G408900300023 11.50 47.90 8.0 G408900300024 11.75 59.30 8.0 G408900300025 12.00 74.27 8.0 G408900300026 12.50 96.18 10.0 G408900300027 13.00 132.57 10.0 G408900300028 13.50 169.33 10.0 G408900300029 14.00 202.01 10.0 G408900300030 14.50 230.61 10.0 G408900300031 15.00 251.40 10.0 G408900300032 15.50 258.09 12.0 G408900300033 16.00 249.54 12.0 G408900300034 16.50 229.86 14.0 G408900300035 17.00 203.87 14.0 G408900300036 17.50 177.50 16.0 G408900300037 18.00 152.62 16.0 G408900300038 18.50 112.51 18.0 G408900300039 19.00 78.35 18.0 G408900300040 19.50 41.96 20.0 G408900300041 20.00 22.28 20.0 G408900300042 ENDDATA 26 0 G408900300043 ENDSUBENT 42 0 G408900399999 SUBENT G4089004 20210602 G047G408900400001 BIB 6 15 G408900400002 REACTION ((58-CE-136(G,N)58-CE-135,,SIG,,BRA)/ G408900400003 (58-CE-140(G,N)58-CE-139,,SIG,,BRA)) G408900400004 SAMPLE Disks of high-purity cerium oxide CeO2 weighing 2 g G408900400005 and with a diameter of 20 mm, pressed into G408900400006 thin-walled caprolon cassettes G408900400007 DECAY-DATA (58-CE-135-G,17.7HR,DG,265.,0.442) G408900400008 (58-CE-139-G,137.6D,DG,165.8,0.801) G408900400009 REL-REF (R,,R.B.Firestone+,B,FIRESTONE,,,1996) G408900400010 ERR-ANALYS (ERR-1,,0.5) The standard error is less 0.5% and does G408900400011 not exceed the size of the point. G408900400012 (ERR-2,,0.05) Determination of the mass of the samples.G408900400013 (ERR-3) Detector efficiency 2%. G408900400014 (ERR-4,,0.5) Half-life <= 0.5%. G408900400015 (ERR-5,,1.) Gamma line intensity <= 1%. G408900400016 STATUS (TABLE) Fig.2b in Yad.Fiz. ta Energetika,20,228,2019 G408900400017 ENDBIB 15 0 G408900400018 COMMON 1 3 G408900400019 ERR-3 G408900400020 PER-CENT G408900400021 2. G408900400022 ENDCOMMON 3 0 G408900400023 DATA 2 28 G408900400024 EN-MAX DATA G408900400025 MEV NO-DIM G408900400026 10.25 0.0193 G408900400027 10.50 0.062 G408900400028 10.50 0.0668 G408900400029 10.75 0.162 G408900400030 10.75 0.156 G408900400031 11.00 0.258 G408900400032 11.00 0.259 G408900400033 11.25 0.311 G408900400034 11.25 0.337 G408900400035 11.50 0.364 G408900400036 11.75 0.405 G408900400037 12.00 0.447 G408900400038 12.50 0.516 G408900400039 13.00 0.57 G408900400040 13.50 0.635 G408900400041 14.00 0.663 G408900400042 14.50 0.684 G408900400043 14.50 0.677 G408900400044 14.50 0.668 G408900400045 15.00 0.706 G408900400046 15.00 0.618 G408900400047 15.50 0.713 G408900400048 16.00 0.711 G408900400049 16.00 0.712 G408900400050 16.50 0.719 G408900400051 17.00 0.724 G408900400052 17.50 0.722 G408900400053 18.00 0.732 G408900400054 ENDDATA 30 0 G408900400055 ENDSUBENT 54 0 G408900499999 SUBENT G4089005 20210602 G047G408900500001 BIB 8 14 G408900500002 REACTION (58-CE-136(G,N)58-CE-135,,SIG,,BRS) G408900500003 MONITOR (58-CE-140(G,N)58-CE-139,,SIG,,BRS) G408900500004 MONIT-REF ((MONIT)G4059001,V.M.Mazur+,J,YFE,18,146,2017) G408900500005 ANALYSIS Unfolding was carried out by the inverse matrix method G408900500006 SAMPLE Disks of high-purity cerium oxide CeO2 weighing 2 g G408900500007 and with a diameter of 20 mm, pressed into G408900500008 thin-walled caprolon cassettes G408900500009 ADD-RES The following parameter values were obtained as a G408900500010 result of fitting for reaction 136Ce(gamma,n)135Ce: G408900500011 Sigma0 = 294,1+-4,4 mb, E0=15,10+-0.09 MeV, G408900500012 Width0 = 4.41+-0.14 MeV. G408900500013 ERR-ANALYS (DATA-ERR) No information on sources of uncertainties G408900500014 STATUS (DEP,G4089004) G408900500015 (TABLE) Fig.3b in Yad.Fiz. ta Energetika,20,228,2019 G408900500016 ENDBIB 14 0 G408900500017 NOCOMMON 0 0 G408900500018 DATA 3 33 G408900500019 EN DATA DATA-ERR G408900500020 MEV MB MB G408900500021 10.125 11.183 2.0 G408900500022 10.375 42.927 4.0 G408900500023 10.625 59.516 4.0 G408900500024 10.875 63.027 5.0 G408900500025 11.125 60.507 5.0 G408900500026 11.375 76.364 6.0 G408900500027 11.625 88.049 6.0 G408900500028 11.875 97.798 6.0 G408900500029 12.125 110.219 7.0 G408900500030 12.375 118.138 7.0 G408900500031 12.625 129.495 7.0 G408900500032 12.875 149.515 8.0 G408900500033 13.125 164.569 8.0 G408900500034 13.375 185.942 10.0 G408900500035 13.625 205.042 10.0 G408900500036 13.875 225.583 11.0 G408900500037 14.125 248.901 12.0 G408900500038 14.375 264.268 12.0 G408900500039 14.625 279.555 13.0 G408900500040 14.875 296.492 14.0 G408900500041 15.125 298.263 15.0 G408900500042 15.375 290.695 16.0 G408900500043 15.625 273.509 17.0 G408900500044 15.875 259.573 18.0 G408900500045 16.125 235.047 19.0 G408900500046 16.375 219.211 20.0 G408900500047 16.625 210.100 21.0 G408900500048 16.875 183.100 22.0 G408900500049 17.125 137.996 22.0 G408900500050 17.375 117.829 16.0 G408900500051 17.625 94.941 18.0 G408900500052 17.875 75.029 18.0 G408900500053 18.125 63.975 18.0 G408900500054 ENDDATA 35 0 G408900500055 ENDSUBENT 54 0 G408900599999 ENDENTRY 5 0 G408999999999