ENTRY K2164 20231113 K216400000001 SUBENT K2164001 20231113 20240316 K216400100001 BIB 14 43 K216400100002 TITLE Gamma-ray strength function for 116,117Sn with the K216400100003 pygmy dipole resonance balanced in the photoneutron K216400100004 and neutron capture channels K216400100005 AUTHOR (H.Utsunomiya, S.Goriely, M.Kamata, T.Kondo, O.Itoh, K216400100006 H.Akimune, T.Yamagata, H.Toyokawa, Y.-W.Lui, K216400100007 S.Hilaire, A.J.Koning) K216400100008 INSTITUTE (2JPNKON,2BLGBRU,2JPNAIS,1USATAM,2FR BRC,2NEDNRG) K216400100009 REFERENCE (J,PR/C,80,055806,2009) K216400100010 Main reference. See also TITLE and AUTHOR. K216400100011 (S,AIP-1238,234,2010) M.Kamata+, Same data given K216400100012 (S,AIP-1120,183,2009) K216400100013 H.Utsunomiya+, Conf.Proc. of ASR2008 K216400100014 (S,AIP-1090,637,2008) K216400100015 H.Utsunomiya+, Preliminary data given K216400100016 PART-DET (N) K216400100017 INC-SOURCE (LCS) lambda=532 nm and 1064 nm laser photons K216400100018 SAMPLE - Chemical-form of target is element. K216400100019 - Physical-form of target is solid. K216400100020 METHOD (RINGR) To determine average neutron energies. 20 3He K216400100021 proportional counters coaxially embedded in K216400100022 polyethylene moderator at distance of 3.8, 7.0 K216400100023 and 10.0 cm from beam axis. K216400100024 FACILITY (ESTRG,2JPNAIS) To store electron beam from 506.3 to K216400100025 763.0 MeV at Tsukuba Electron Ring for K216400100026 Accelerating and Storage (TERAS) K216400100027 DETECTOR (PROPC) To detect neutron K216400100028 (HPGE) To measure the energy distribution of the LCS K216400100029 gamma-ray K216400100030 (NAICR) To measure the intensity of the LCS gamma-ray K216400100031 ERR-ANALYS - Total systematic uncertainty: 4.4 - 5.9 % K216400100032 - Uncertainty of the time variation of the LCS beam K216400100033 energy distribution (a few percentages) K216400100034 (ERR-1) Neutron detection efficiency K216400100035 (ERR-2) Number of incident gamma rays K216400100036 (ERR-S) Statistical uncertainty K216400100037 REL-REF (M,,A.Makinaga+,J,PR/C,79,025801,2009) K216400100038 Further details of experimental technique K216400100039 STATUS (APRVD) Proofread by Hiroaki Utsunomiya (2010.01.16) K216400100040 HISTORY (20091224R) Received by e-mail from H.Utsunomiya K216400100041 (20091225C) Ayano Makinaga K216400100042 (20100721A) REFERENCE: AIP-1120 and -1238 added K216400100043 (20231109A) MA: modified REFERENCE and INSTITUTE in K216400100044 001; REACTION in 002-003. K216400100045 ENDBIB 43 0 K216400100046 COMMON 2 3 K216400100047 ERR-1 ERR-2 K216400100048 PER-CENT PER-CENT K216400100049 3.2 3. K216400100050 ENDCOMMON 3 0 K216400100051 ENDSUBENT 50 0 K216400199999 SUBENT K2164002 20231113 20240316 K216400200001 BIB 4 12 K216400200002 REACTION 1(50-SN-116(G,N)50-SN-115,,SIG) K216400200003 Corrected for energy spread of LCS beam based on the K216400200004 Taylor expansion method K216400200005 2(50-SN-116(G,N)50-SN-115,,SIG) K216400200006 Corrected for energy spread of LCS beam based on the K216400200007 least square method K216400200008 3(50-SN-116(G,N)50-SN-115,,SIG,,AV) K216400200009 Average cross sections for two methods K216400200010 SAMPLE Target-thickness is 1991 mg/cm2. K216400200011 (50-SN-116,ENR=0.9755) K216400200012 STATUS (TABLE) Plotted in Fig.2 of J,PR/C,80,055806,2009 K216400200013 HISTORY (20231109A) MA: SF8: AV added. K216400200014 ENDBIB 12 0 K216400200015 NOCOMMON 0 0 K216400200016 DATA 7 10 K216400200017 EN DATA 1ERR-S 1DATA 2ERR-S 2DATA 3K216400200018 ERR-S 3 K216400200019 MEV MB MB MB MB MB K216400200020 MB K216400200021 9.63 18.80 1.22 18.54 1.20 18.67K216400200022 1.21 K216400200023 9.74 21.84 2.79 21.23 2.71 21.54K216400200024 2.75 K216400200025 9.89 19.75 0.52 18.63 0.49 19.19K216400200026 0.51 K216400200027 10.01 21.25 1.15 20.23 1.09 20.74K216400200028 1.12 K216400200029 10.32 25.49 1.01 24.53 0.97 25.01K216400200030 0.99 K216400200031 10.53 23.68 1.71 22.85 1.65 23.26K216400200032 1.68 K216400200033 10.94 32.79 1.72 33.76 1.77 33.27K216400200034 1.75 K216400200035 11.40 39.63 2.30 41.39 2.40 40.51K216400200036 2.35 K216400200037 11.74 44.83 2.34 48.39 2.53 46.61K216400200038 2.43 K216400200039 12.35 77.37 3.71 78.59 3.77 77.98K216400200040 3.74 K216400200041 ENDDATA 24 0 K216400200042 ENDSUBENT 41 0 K216400299999 SUBENT K2164003 20231113 20240316 K216400300001 BIB 4 12 K216400300002 REACTION 1(50-SN-117(G,N)50-SN-116,,SIG) K216400300003 Corrected for energy spread of LCS beam based on the K216400300004 Taylor expansion method K216400300005 2(50-SN-117(G,N)50-SN-116,,SIG) K216400300006 Corrected for energy spread of LCS beam based on the K216400300007 least square method K216400300008 3(50-SN-117(G,N)50-SN-116,,SIG,,AV) K216400300009 Average cross sections for two methods K216400300010 SAMPLE Target-thickness is 1992 mg/cm2. K216400300011 (50-SN-117,ENR=0.901) K216400300012 STATUS (TABLE) Plotted in Fig.3 of J,PR/C,80,055806,2009 K216400300013 HISTORY (20231109A) MA: SF8: AV added. K216400300014 ENDBIB 12 0 K216400300015 NOCOMMON 0 0 K216400300016 DATA 7 20 K216400300017 EN DATA 1ERR-S 1DATA 2ERR-S 2DATA 3K216400300018 ERR-S 3 K216400300019 MEV MB MB MB MB MB K216400300020 MB K216400300021 7.09 8.50 0.52 9.41 0.58 8.96K216400300022 0.55 K216400300023 7.23 9.07 0.44 9.44 0.46 9.25K216400300024 0.45 K216400300025 7.23 9.35 0.35 9.75 0.36 9.55K216400300026 0.36 K216400300027 7.35 10.76 0.93 10.87 0.94 10.82K216400300028 0.94 K216400300029 7.55 11.02 0.28 10.73 0.27 10.87K216400300030 0.28 K216400300031 7.68 11.53 0.42 10.93 0.40 11.23K216400300032 0.41 K216400300033 7.89 12.16 0.45 11.42 0.42 11.79K216400300034 0.44 K216400300035 8.14 13.27 0.38 12.15 0.34 12.71K216400300036 0.36 K216400300037 8.40 14.17 0.57 13.14 0.53 13.66K216400300038 0.55 K216400300039 8.61 14.21 1.07 13.12 0.99 13.67K216400300040 1.03 K216400300041 8.75 15.91 0.46 14.77 0.43 15.34K216400300042 0.45 K216400300043 9.10 19.53 2.14 18.27 2.00 18.90K216400300044 2.07 K216400300045 9.21 17.75 0.45 16.82 0.42 17.29K216400300046 0.43 K216400300047 9.43 20.56 0.88 19.62 0.84 20.09K216400300048 0.86 K216400300049 9.86 23.51 1.13 23.11 1.11 23.31K216400300050 1.12 K216400300051 9.96 23.66 1.99 23.58 1.99 23.62K216400300052 1.99 K216400300053 10.51 29.29 1.55 30.97 1.64 30.13K216400300054 1.59 K216400300055 11.14 38.50 2.27 39.98 2.35 39.24K216400300056 2.31 K216400300057 11.50 46.68 2.27 49.35 2.40 48.01K216400300058 2.33 K216400300059 12.12 74.45 3.98 73.69 3.94 74.07K216400300060 3.96 K216400300061 ENDDATA 44 0 K216400300062 ENDSUBENT 61 0 K216400399999 ENDENTRY 3 0 K216499999999