ENTRY S0234 20211229 S030S023400000001 SUBENT S0234001 20211229 S030S023400100001 BIB 12 39 S023400100002 TITLE Measurement and analysis of the isomeric cross S023400100003 section ratios for the 94Tc nucleus S023400100004 AUTHOR (G.S.Li,Y.D.Fang,X.H.Zhou,A.Diaz-Torres,A.Rohilla, S023400100005 M.L.Liu,N.T.Zhang,Y.H.Zhang,J.G.Wang,B.S.Gao, S023400100006 Y.H.Qiang,S.Guo,S.C.Wang,Y.Zheng,J.Lubian,H.O.Soler) S023400100007 INSTITUTE (3CPRIMP,3CPRUCA,2UK SUR,3BZLUFF) S023400100008 REFERENCE (J,PR/C,102,054607,2020) S023400100009 #doi:10.1103/PhysRevC.102.054607 S023400100010 FACILITY (CYCLO,3CPRIMP) Heavy Ion Research Facility in S023400100011 Lanzhou (HIRFL) S023400100012 INC-SOURCE The collimated 9Be beam with an initial energy of S023400100013 50.4 MeV was delivered by HIRFL. The average beam S023400100014 current was about 13 enA. S023400100015 SAMPLE Five 89Y targets with thickness of about 1.0 mg/cm2. S023400100016 METHOD (STTA,ACTIV,GSPEC) The offline gamma-ray spectroscopy S023400100017 in continuation to the online stacked-foil activation S023400100018 method. The irradiation lasted about 12 h. S023400100019 (BCINT) The beam flux was extracted using a precise S023400100020 current-integrator device from the charge collected S023400100021 at the Faraday cup, which is biased with a negative S023400100022 400 V electrode and installed at the back of targets. S023400100023 DETECTOR (SI) Two silicon detectors were mounted at +-30 deg S023400100024 with respect to the beam line to cross-check the beam S023400100025 flux that impinged on the targets. S023400100026 (HPGE) For performing offline measurements, a setup S023400100027 formed by five high-purity germanium (HPGe) detector S023400100028 groups was used. Each group composed of two HPGe S023400100029 detectors placed at an angle of 180 deg to each S023400100030 other. The gamma sources of 60Co, 133Ba, and 152Eu S023400100031 were used to calculate the absolute efficiency of the S023400100032 detectors. S023400100033 ERR-ANALYS (ERR-T) The systematic uncertainties are added in S023400100034 quadrature to the statistical errors to get the total S023400100035 errors S023400100036 (ERR-1) Target thickness, about 3.% S023400100037 (ERR-2) Beam intensity, about 3.% S023400100038 (ERR-3) Detector efficiency, about 3.% S023400100039 STATUS (TABLE) Table I of Phys.Rev.C102(2020)054607 S023400100040 HISTORY (20211229C) Wang Jimin (CNDC) S023400100041 ENDBIB 39 0 S023400100042 COMMON 3 3 S023400100043 ERR-1 ERR-2 ERR-3 S023400100044 PER-CENT PER-CENT PER-CENT S023400100045 3. 3. 3. S023400100046 ENDCOMMON 3 0 S023400100047 ENDSUBENT 46 0 S023400199999 SUBENT S0234002 20211229 S030S023400200001 BIB 2 5 S023400200002 REACTION 1(39-Y-89(4-BE-9,4N)43-TC-94-G,,SIG) S023400200003 2(39-Y-89(4-BE-9,4N)43-TC-94-M,,SIG) S023400200004 3(39-Y-89(4-BE-9,4N)43-TC-94-M/G,,SIG/RAT) S023400200005 DECAY-DATA1(43-TC-94-G,293.MIN,DG,916.0,0.076) S023400200006 2(43-TC-94-M,52.MIN,DG,1868.7,0.057) S023400200007 ENDBIB 5 0 S023400200008 NOCOMMON 0 0 S023400200009 DATA 7 5 S023400200010 EN DATA 1ERR-T 1DATA 2ERR-T 2DATA 3S023400200011 ERR-T 3 S023400200012 MEV MB MB MB MB NO-DIM S023400200013 NO-DIM S023400200014 50.1 463. 35. 18. 3. 0.039S023400200015 0.008 S023400200016 49.1 460. 33. 16. 3. 0.036S023400200017 0.006 S023400200018 48.1 419. 26. 22. 2. 0.053S023400200019 0.007 S023400200020 47.0 412. 24. 24. 2. 0.059S023400200021 0.005 S023400200022 45.9 427. 27. 23. 3. 0.053S023400200023 0.007 S023400200024 ENDDATA 14 0 S023400200025 ENDSUBENT 24 0 S023400299999 ENDENTRY 2 0 S023499999999