ENTRY K2403 20130906 K013K240300000001 SUBENT K2403001 20130906 K013K240300100001 BIB 16 45 K240300100002 TITLE Evidence for radiative coupling of the pygmy dipole K240300100003 resonance to excited states K240300100004 AUTHOR (C.T.Angell, S.L.Hammond, H.J.Karwowski, J.H.Kelley, K240300100005 M.Krticka, E.Kwan, A.Makinaga, G.Rusev) K240300100006 INSTITUTE (1USANCA) Department of Physics and Astronomy K240300100007 (1USATNL) K240300100008 (1USAUCX) Department of Nuclear Engineering K240300100009 (2JPNJAE) Quantum Beam Science Directorate K240300100010 (1USANCS) Department of Physics K240300100011 (3CZRCHU) Faculty of Mathematics and Physics K240300100012 (1USADKE) Department of Physics K240300100013 (2JPNKON) Department of Physics K240300100014 REFERENCE (J,PR/C,86,051302,2012) K240300100015 PART-DET (N) K240300100016 INC-SOURCE (LCS) lambda=532 and 1064 nm laser photons were used. K240300100017 SAMPLE - Chemical-form of target: Nd2O3 K240300100018 - Physical-form of target is solid. K240300100019 - Target-thickness: 3g K240300100020 - Backing is aluminium. K240300100021 (60-ND-142,ENR=0.99) K240300100022 METHOD (RINGR) To determine average neutron energies. 20 3He K240300100023 proportional counters coaxially embedded in K240300100024 polyethylene moderator at distance of 3.8, 7.0 K240300100025 and 10.0 cm from beam axis. K240300100026 FACILITY (ESTRG,2JPNAIS) Tsukuba Electron Ring for Accelerating K240300100027 and Storage (TERAS). K240300100028 DETECTOR (PROPC) To detect neutron. K240300100029 (NAICR) To monitor the photon flux. K240300100030 (HPGE) To determine the energy distribution. K240300100031 CORRECTION Corrected for energy spread of LCS beam based on the K240300100032 Taylor expansion method K240300100033 ERR-ANALYS Uncertainty to beam-size effect (a few percentages) K240300100034 (ERR-1) Due to neutron detection efficiency K240300100035 (ERR-2) Due to number of incident gamma rays K240300100036 (ERR-S) Statistical uncertainty K240300100037 ADD-RES (COMP) Statistical model K240300100038 REL-REF (M,K2111001,A.Makinaga+,J,PR/C,79,025801,2009) K240300100039 (O,L0182001,C.T.Angell+,J,PR/C,86,051302,2012) K240300100040 Data from HIgS, Duke K240300100041 STATUS (APRVD) Approved by A. Makinaga 2013.05.01 K240300100042 (TABLE) Plotted in Fig.2 of Phys. Rev. C, 86, 051302, K240300100043 2012 K240300100044 HISTORY (20130417C) M.O. & A.Makinaga K240300100045 (20130424R) Numerical data were given by e-mail from K240300100046 Dr. C.T.Angell K240300100047 ENDBIB 45 0 K240300100048 COMMON 2 3 K240300100049 ERR-1 ERR-2 K240300100050 PER-CENT PER-CENT K240300100051 3.2 3. K240300100052 ENDCOMMON 3 0 K240300100053 ENDSUBENT 52 0 K240300199999 SUBENT K2403002 20130906 K013K240300200001 BIB 1 1 K240300200002 REACTION (60-ND-142(G,N)60-ND-141,,SIG) K240300200003 ENDBIB 1 0 K240300200004 NOCOMMON 0 0 K240300200005 DATA 3 15 K240300200006 EN DATA ERR-S K240300200007 MEV MB MB K240300200008 9.86 22.3 1.5 K240300200009 9.90 36.1 0.9 K240300200010 9.95 32.2 1.0 K240300200011 10.12 37.8 1.1 K240300200012 10.28 42.6 1.0 K240300200013 10.46 46.5 1.9 K240300200014 10.74 54.9 5.0 K240300200015 11.09 58.5 1.9 K240300200016 11.40 70.1 1.9 K240300200017 11.73 85.5 2.0 K240300200018 12.16 100.1 2.8 K240300200019 12.30 116.2 4.5 K240300200020 12.76 152.3 5.8 K240300200021 13.00 178.7 3.2 K240300200022 13.26 198.7 4.8 K240300200023 ENDDATA 17 0 K240300200024 ENDSUBENT 23 0 K240300299999 ENDENTRY 2 0 K240399999999