ENTRY G0052 20160827 G036G005200000001 SUBENT G0052001 20160827 G036G005200100001 BIB 10 28 G005200100002 TITLE Role of electric and magnetic dipole strength G005200100003 functions in the 114Cd(g,g') and 113Cd(n,g) reactions G005200100004 AUTHOR (R.Massarczyk, G.Schramm, T.Belgya, R.Schwengner, G005200100005 R.Beyer, D.Bemmerer, Z.Elekes, E.Grosse, R.Hannaske, G005200100006 A.R.Junghans, Z.Kis, T.Koegler, C.Lorenz, K.Schmidt, G005200100007 L.Szentmiklosi, A.Wagner, J.L.Weil) G005200100008 INSTITUTE (2GERZFK,2GERDRE,3HUNKFI) G005200100009 REFERENCE (J,PR/C,93,014301,2016) G005200100010 FACILITY (LINAC,2GERZFK) gammaELBE G005200100011 INC-SOURCE (BRST) 10.5 MeV electrons onto a Nb foil (12 um thick) G005200100012 SAMPLE Enriched 11B powder for photon fluence determination. G005200100013 (48-CD-114,ENR=0.9937) 114Cd (2.001 g, enriched to G005200100014 99.37%). G005200100015 DETECTOR (HPGE) Two pairs of HPGe detectors at 90 deg and G005200100016 127 deg with respect to the photon beam G005200100017 (BGO) Veto detector against cosmic ray G005200100018 CORRECTION Corrections made for the measured yield Y(E,dE) at G005200100019 photon energy E and its interval dE: G005200100020 - subtraction of ambient background, G005200100021 - unfolding by detector response, G005200100022 - correction for the full-energy detection efficiency,G005200100023 - subtraction of non-nuclear (atomic) background, G005200100024 - subtraction of inelastic transitions from higher, G005200100025 energy state E" -> E, G005200100026 - correction for the ground state branching ratio G005200100027 b0=Y(E->0)/Y(all transitions from E). G005200100028 HISTORY (20160827R) On. Data Received from Ralph Massarczyk G005200100029 (20160827C) On G005200100030 ENDBIB 28 0 G005200100031 NOCOMMON 0 0 G005200100032 ENDSUBENT 31 0 G005200199999 SUBENT G0052002 20160827 G036G005200200001 BIB 3 6 G005200200002 REACTION (48-CD-114(G,SCT)48-CD-114,,SIG) G005200200003 STATUS (TABLE) Plotted in Fig.4 of Phys.Rev.C93(2016)014301 G005200200004 ERR-ANALYS (DATA-ERR) Uncertainties due to counting statistics G005200200005 (typically on the percent level) and corrections. G005200200006 The main uncertainty comes from the correction for the G005200200007 inelastic transitions. G005200200008 ENDBIB 6 0 G005200200009 NOCOMMON 0 0 G005200200010 DATA 3 52 G005200200011 EN DATA DATA-ERR G005200200012 MEV MB MB G005200200013 4.0 3.85 1.99 G005200200014 4.1 3.75 1.95 G005200200015 4.2 3.88 1.96 G005200200016 4.3 3.77 1.91 G005200200017 4.4 3.83 1.92 G005200200018 4.5 3.52 1.87 G005200200019 4.6 4.60 1.98 G005200200020 4.7 4.36 1.94 G005200200021 4.8 4.06 1.91 G005200200022 4.9 4.14 1.90 G005200200023 5.0 3.93 1.87 G005200200024 5.1 3.44 1.82 G005200200025 5.2 3.79 1.84 G005200200026 5.3 3.66 1.82 G005200200027 5.4 3.41 1.79 G005200200028 5.5 4.07 1.84 G005200200029 5.6 4.49 1.87 G005200200030 5.7 4.27 1.84 G005200200031 5.8 5.52 1.93 G005200200032 5.9 5.04 1.87 G005200200033 6.0 5.08 1.86 G005200200034 6.1 6.45 1.95 G005200200035 6.2 6.03 1.91 G005200200036 6.3 5.88 1.87 G005200200037 6.4 7.06 1.94 G005200200038 6.5 7.03 1.91 G005200200039 6.6 7.27 1.90 G005200200040 6.7 7.81 1.92 G005200200041 6.8 8.32 1.92 G005200200042 6.9 8.62 1.92 G005200200043 7.0 8.88 1.90 G005200200044 7.1 8.97 1.88 G005200200045 7.2 9.91 1.90 G005200200046 7.3 9.47 1.85 G005200200047 7.4 9.62 1.86 G005200200048 7.5 12.57 1.91 G005200200049 7.6 12.33 1.87 G005200200050 7.7 13.02 1.86 G005200200051 7.8 13.39 1.84 G005200200052 7.9 13.46 1.80 G005200200053 8.0 13.60 1.77 G005200200054 8.1 14.59 1.74 G005200200055 8.2 14.36 1.71 G005200200056 8.3 15.33 1.66 G005200200057 8.4 15.45 1.65 G005200200058 8.5 16.46 1.59 G005200200059 8.6 16.91 1.56 G005200200060 8.7 17.87 1.43 G005200200061 8.8 18.75 1.37 G005200200062 8.9 20.01 1.27 G005200200063 9.0 21.62 1.29 G005200200064 9.1 21.38 1.27 G005200200065 ENDDATA 54 0 G005200200066 ENDSUBENT 65 0 G005200299999 ENDENTRY 2 0 G005299999999