ENTRY K2295 20110502 K010K229500000001 SUBENT K2295001 20110502 K010K229500100001 BIB 13 40 K229500100002 TITLE gamma-ray strength function method and its application K229500100003 to 107Pd K229500100004 AUTHOR (H.Utsunomiya, S.Goriely, H.Akimune, H.Harada, K229500100005 F.Kitatani, S.Goko, H.Toyokawa, K.Yamada, T.Kondo, K229500100006 O.Itoh, M.Kamata, T.Yamagata, Y.-W.Lui, I.Daoutidis, K229500100007 D.P.Arteaga, S.Hilaire, A.J.Koning) K229500100008 INSTITUTE (2JPNKON) Department of Physics K229500100009 (2BLGBRU) Institute d'Astronomie et d'Astrophysique K229500100010 (2JPNJAE) K229500100011 (2JPNAIS) K229500100012 (1USATAM) Cyclotron Institute K229500100013 (2FR PAR) Institut de Physique Nucleaire (IN2P3-CNRS) K229500100014 (2FR FR) CEA,DAM,DIF, Arpajon K229500100015 (2NEDNRG) K229500100016 REFERENCE (J,PR/C,82,064610,201012) K229500100017 PART-DET (N) K229500100018 INC-SOURCE (LCS) lambda=532 nm and 1064 nm laser photons K229500100019 SAMPLE - Chemical-form of target is element. K229500100020 - Physical-form of target is solid. K229500100021 METHOD (RINGR) To determine average neutron energies. 20 3He K229500100022 proportional counters coaxially embedded in K229500100023 polyethylene moderator at distance of 3.8, 7.0 K229500100024 and 10.0 cm from beam axis. K229500100025 FACILITY (ESTRG,2JPNAIS) To store electron beam from 520.6 to K229500100026 655.7 MeV at Tsukuba Electron Ring for K229500100027 Accelerating and Storage (TERAS) K229500100028 DETECTOR (PROPC) To detect neutron K229500100029 (HPGE) To measure the energy distribution of the LCS K229500100030 gamma-ray with high-energy photon K229500100031 spectrometer(HHS) K229500100032 (NAICR) To measure the intensity of the LCS gamma-ray K229500100033 ERR-ANALYS (ERR-SYS) Systematic uncertainty K229500100034 (ERR-1) Neutron detection efficiency K229500100035 (ERR-2) Number of incident gamma rays K229500100036 (ERR-S) Statistical uncertainty K229500100037 REL-REF (M,K2111001,A.Makinaga+,J,PR/C,79,025801,2009) K229500100038 Further details of experimental technique K229500100039 HISTORY (20110108R) Received by e-mail from T.Kondo through H. K229500100040 Utsunomiya K229500100041 (20110111C) Ayano Makinaga K229500100042 ENDBIB 40 0 K229500100043 COMMON 3 3 K229500100044 ERR-SYS ERR-1 ERR-2 K229500100045 PER-CENT PER-CENT PER-CENT K229500100046 4.4 3.2 3. K229500100047 ENDCOMMON 3 0 K229500100048 ENDSUBENT 47 0 K229500199999 SUBENT K2295002 20110502 K010K229500200001 BIB 3 9 K229500200002 REACTION 1(46-PD-106(G,N)46-PD-105,,SIG) K229500200003 Corrected for energy spread of LCS beam based on the K229500200004 least square method K229500200005 2(46-PD-106(G,N)46-PD-105,,SIG) K229500200006 Corrected for energy spread of LCS beam based on the K229500200007 Taylor expansion method K229500200008 SAMPLE Target-thickness: 891 mg, 8 mm diameter K229500200009 (46-PD-106,ENR=0.984) K229500200010 STATUS (TABLE) Plotted in Fig.2 of PR/C,vol.82,064610,2010 K229500200011 ENDBIB 9 0 K229500200012 NOCOMMON 0 0 K229500200013 DATA 5 9 K229500200014 EN DATA 1ERR-S 1DATA 2ERR-S 2 K229500200015 MEV MB MB MB MB K229500200016 9.66 9.49 2.26 8.07 2.38 K229500200017 9.84 16.61 1.22 14.69 1.24 K229500200018 10.00 17.22 0.91 15.93 0.91 K229500200019 10.28 20.86 0.81 20.60 0.80 K229500200020 10.81 21.47 0.76 22.35 0.72 K229500200021 11.16 30.30 1.46 32.85 1.40 K229500200022 11.99 50.59 2.30 54.09 2.20 K229500200023 12.63 74.02 2.61 75.83 2.47 K229500200024 13.74 120.80 4.47 117.46 4.29 K229500200025 ENDDATA 11 0 K229500200026 ENDSUBENT 25 0 K229500299999 SUBENT K2295003 20110502 K010K229500300001 BIB 3 9 K229500300002 REACTION 1(46-PD-105(G,N)46-PD-104,,SIG) K229500300003 Corrected for energy spread of LCS beam based on the K229500300004 least square method K229500300005 2(46-PD-105(G,N)46-PD-104,,SIG) K229500300006 Corrected for energy spread of LCS beam based on the K229500300007 Taylor expansion method K229500300008 SAMPLE Target-thickness: 498 mg, 6 mm in diameter K229500300009 (46-PD-105,ENR=0.984) K229500300010 STATUS (TABLE) Plotted in Fig.4 of PR/C,vol.82,064610,2010 K229500300011 ENDBIB 9 0 K229500300012 NOCOMMON 0 0 K229500300013 DATA 5 13 K229500300014 EN DATA 1ERR-S 1DATA 2ERR-S 2 K229500300015 MEV MB MB MB MB K229500300016 7.13 0.74 0.53 0.98 0.57 K229500300017 7.26 0.75 0.17 0.86 0.17 K229500300018 7.42 1.29 0.15 1.38 0.15 K229500300019 7.72 4.13 0.18 4.16 0.18 K229500300020 8.08 6.37 0.23 6.09 0.21 K229500300021 8.56 9.26 0.89 8.58 0.84 K229500300022 9.06 11.36 1.42 10.28 1.48 K229500300023 9.31 15.22 0.87 13.88 0.82 K229500300024 9.43 14.23 0.88 12.50 0.81 K229500300025 9.44 14.21 0.88 12.50 0.80 K229500300026 9.88 18.75 1.19 16.96 1.10 K229500300027 10.46 18.62 0.75 17.99 0.68 K229500300028 10.73 24.68 1.29 25.67 1.20 K229500300029 ENDDATA 15 0 K229500300030 ENDSUBENT 29 0 K229500399999 SUBENT K2295004 20110502 K010K229500400001 BIB 3 9 K229500400002 REACTION 1(46-PD-108(G,N)46-PD-107,,SIG) K229500400003 Corrected for energy spread of LCS beam based on the K229500400004 least square method K229500400005 2(46-PD-108(G,N)46-PD-107,,SIG) K229500400006 Corrected for energy spread of LCS beam based on the K229500400007 Taylor expansion method K229500400008 SAMPLE Target-thickness: 731 mg, 8 mm in diameter K229500400009 (46-PD-108,ENR=0.996) K229500400010 STATUS (TABLE) Plotted in Fig.6 of PR/C,vol.82,064610,2010 K229500400011 ENDBIB 9 0 K229500400012 NOCOMMON 0 0 K229500400013 DATA 5 10 K229500400014 EN DATA 1ERR-S 1DATA 2ERR-S 2 K229500400015 MEV MB MB MB MB K229500400016 9.35 11.37 1.29 11.32 1.34 K229500400017 9.50 16.69 1.44 16.71 1.48 K229500400018 9.71 18.12 0.93 18.27 0.95 K229500400019 9.89 25.53 1.45 25.80 1.46 K229500400020 10.21 23.77 0.76 24.19 0.75 K229500400021 10.74 31.43 1.18 31.71 1.13 K229500400022 11.07 37.73 1.38 38.53 1.32 K229500400023 11.97 62.44 1.75 63.02 1.66 K229500400024 12.61 86.35 2.79 84.54 2.59 K229500400025 13.73 140.24 5.00 137.08 4.71 K229500400026 ENDDATA 12 0 K229500400027 ENDSUBENT 26 0 K229500499999 ENDENTRY 4 0 K229599999999