ENTRY G0032 20120229 G024G003200000001 SUBENT G0032001 20120229 G024G003200100001 BIB 15 40 G003200100002 TITLE Dipole strength in 78Se below the neutron separation G003200100003 energy from a combined analysis of 77Se(n,g) and G003200100004 78Se(g,g') experiments G003200100005 AUTHOR (G.Schramm, R.Massarczyk, A.R.Junghans, T.Belgya, G003200100006 R.Beyer, E.Birgersson, E.Grosse, M.Kempe, Z.Kis, G003200100007 K.Kosev, M.Krticka, A.Matic, K.D.Schilling, G003200100008 R.Schwengner, L.Szentmiklosi, A.Wagner, J.L.Weil) G003200100009 INSTITUTE (2GERZFK,3HUNII ,2GERDRE,3CZRCHU) G003200100010 REFERENCE (J,PR/C,85,014311,2012) G003200100011 REL-REF (O,31721001,G.Schramm+,J,PR/C,85,014311,2012) G003200100012 Neutron capture data measured at Budapest given G003200100013 FACILITY (LINAC,2GERZFK) ELBE G003200100014 INC-SOURCE (BRST) E0=11.5 MeV and 520 uA on 4 um thick Nb radiatorG003200100015 INC-SPECT Energy at centre of the bin is coded as incident energyG003200100016 SAMPLE (34-SE-78,ENR=0.9939) 2002 mg G003200100017 (5-B-11,ENR=0.995) 212.5 mg and 105.6 mg disks G003200100018 DETECTOR (HPGE) Detection of scattered photon at 90 and 127 deg;G003200100019 100% relative efficiency G003200100020 ANALYSIS 1. Determine the photon fluence at the target position.G003200100021 2. Subtract the room background. G003200100022 3. Correct the measured spectrum for detector response G003200100023 and efficiency. G003200100024 4. Subtract the non-nuclear (atomic) background. G003200100025 5. Subtract inelastic transitions and correct for G003200100026 branching, angular distribution effects, and elasticG003200100027 enhancement. G003200100028 6. Normalize to a known cross section. G003200100029 MONITOR (5-B-11(G,SCT),PAR,ARE) G003200100030 MONIT-REF (,F.Ajzenberg-Selove,J,NP/A,506,1,1990) G003200100031 (L0147001,G.Rusev+,J,PR/C,79,047601,2009) G003200100032 ERR-ANALYS (ERR-T) Total uncertainty including G003200100033 (ERR-1) Statistical uncertainty in the counts of the G003200100034 11B line used for normalization (3%) G003200100035 (ERR-2)(Estimated) uncertainty in the simulated ground G003200100036 state branching ratios (9%) G003200100037 (ERR-3) simulated detector efficiency (5%) G003200100038 (ERR-4,,5.)(Estimated) uncertainty in the simulated G003200100039 yield of inel. transitions (5% for every exc.energy) G003200100040 HISTORY (20120222C) On G003200100041 (20120229R) On. Received from Ronald Schwengner G003200100042 ENDBIB 40 0 G003200100043 COMMON 4 3 G003200100044 E-NRM ERR-1 ERR-2 ERR-3 G003200100045 MEV PER-CENT PER-CENT PER-CENT G003200100046 8.92 3. 9. 5. G003200100047 ENDCOMMON 3 0 G003200100048 ENDSUBENT 47 0 G003200199999 SUBENT G0032002 20120229 G024G003200200001 BIB 3 11 G003200200002 REACTION 1(34-SE-78(G,EL)34-SE-78,,SIG) G003200200003 2(34-SE-78(G,SCT)34-SE-78,,SIG) G003200200004 Sum of elastic and inelastic transitions G003200200005 MISC-COL (MISC) Uncorrected cross section, corrected for G003200200006 - detector response and efficiency; G003200200007 - room background; G003200200008 - atomic background (Compton and pair creation) G003200200009 , but uncorrected for G003200200010 - inelastic transition; G003200200011 - branching ratio to the elastic transition. G003200200012 STATUS (TABLE) Plotted in Phys.Rev.C85(2012)014311 G003200200013 ENDBIB 11 0 G003200200014 NOCOMMON 0 0 G003200200015 DATA 7 33 G003200200016 EN DATA 1ERR-T 1DATA 2ERR-T 2MISC G003200200017 MISC-ERR G003200200018 MEV MB MB MB MB MB G003200200019 MB G003200200020 4.100 1.27015 1.26966 2.57558 2.57458 6.46554 G003200200021 0.37717 G003200200022 4.300 0.99529 0.99481 2.07758 2.07658 6.26451 G003200200023 0.36477 G003200200024 4.500 1.81987 1.73342 3.83801 3.65569 6.59159 G003200200025 0.38276 G003200200026 4.700 1.45033 1.44987 3.17511 3.17411 6.47643 G003200200027 0.37547 G003200200028 4.900 1.63953 1.57020 3.65422 3.49971 6.52842 G003200200029 0.37799 G003200200030 5.100 2.40625 1.52613 5.56941 3.53231 7.14340 G003200200031 0.41319 G003200200032 5.300 1.27478 1.27435 3.02197 3.02097 6.14921 G003200200033 0.35574 G003200200034 5.500 2.03224 1.34707 4.99069 3.30809 6.72581 G003200200035 0.38879 G003200200036 5.700 1.80409 1.27163 4.55973 3.21396 6.43616 G003200200037 0.37203 G003200200038 5.900 1.64202 1.19710 4.36176 3.17990 6.48740 G003200200039 0.37490 G003200200040 6.100 2.10190 1.14167 5.74082 3.11820 6.75137 G003200200041 0.39003 G003200200042 6.300 2.02313 1.06643 5.78612 3.04999 6.64148 G003200200043 0.38369 G003200200044 6.500 1.63387 0.98906 4.84363 2.93208 6.27855 G003200200045 0.36280 G003200200046 6.700 2.69994 0.97728 8.37366 3.03097 7.13358 G003200200047 0.41208 G003200200048 6.900 1.96358 0.85655 6.33182 2.76204 6.17326 G003200200049 0.35680 G003200200050 7.100 2.25822 0.80243 7.71981 2.74315 6.19769 G003200200051 0.35823 G003200200052 7.300 2.72644 0.78383 9.78841 2.81409 6.50486 G003200200053 0.37610 G003200200054 7.500 2.78324 0.69709 10.37901 2.59953 6.06856 G003200200055 0.35087 G003200200056 7.700 3.29049 0.69881 12.80513 2.71946 6.39626 G003200200057 0.36980 G003200200058 7.900 3.65631 0.66975 15.24573 2.79264 6.39590 G003200200059 0.36985 G003200200060 8.100 4.12113 0.66702 17.93409 2.90272 6.56969 G003200200061 0.37995 G003200200062 8.300 3.59213 0.56253 16.59041 2.59809 5.63173 G003200200063 0.32598 G003200200064 8.500 3.71931 0.55383 18.19633 2.70958 5.65474 G003200200065 0.32741 G003200200066 8.700 3.20027 0.46365 16.74350 2.42576 4.74713 G003200200067 0.27522 G003200200068 8.900 3.10620 0.42697 17.55986 2.41373 4.38549 G003200200069 0.25509 G003200200070 9.100 2.68128 0.34729 16.86129 2.18394 3.57847 G003200200071 0.20812 G003200200072 9.300 2.93833 0.34346 20.48034 2.39395 3.48896 G003200200073 0.20311 G003200200074 9.500 2.69404 0.30832 20.66941 2.36548 3.11083 G003200200075 0.18149 G003200200076 9.700 2.73079 0.30046 22.97578 2.52791 2.98149 G003200200077 0.17422 G003200200078 9.900 2.54218 0.26987 24.87458 2.64057 2.62152 G003200200079 0.15370 G003200200080 10.100 1.92842 0.20126 20.54163 2.14388 1.92842 G003200200081 0.11403 G003200200082 10.300 1.69587 0.17738 20.44126 2.13804 1.69587 G003200200083 0.10096 G003200200084 10.500 1.02902 0.10858 13.57228 1.43213 1.02902 G003200200085 0.06292 G003200200086 ENDDATA 70 0 G003200200087 ENDSUBENT 86 0 G003200299999 ENDENTRY 2 0 G003299999999