ENTRY G0029 20110902 G025G002900000001 SUBENT G0029001 20110902 G025G002900100001 BIB 16 36 G002900100002 TITLE Fragmentation and systematics of the pygmy dipole G002900100003 resonance in the stable N=82 isotones G002900100004 AUTHOR (D.Savran, M.Elvers, J.Endres, M.Fritzsche, B.Loeher, G002900100005 N.Pietralla, V.Yu.Ponomarev, C.Romig, G002900100006 L.Schnorrenberger, K.Sonnabend, A.Zilges) G002900100007 INSTITUTE (2GERGSI,2GERKLN,2GERTHD,2GERFRK) G002900100008 (2GERGER) Frankfurt Institute for Advanced Studies, G002900100009 Frankfurt G002900100010 REFERENCE (J,PR/C,84,024326,2011) Data given in table G002900100011 (J,PRL,100,232501,2008) Spectrum in figure G002900100012 FACILITY (LINAC,2GERTHD) Electron linear accelerator S-DALINAC G002900100013 INC-SOURCE (BRST) End point energy at 8.2 and 9.2 MeV G002900100014 INC-SPECT Bremsstrahlung spectrum G002900100015 SAMPLE (54-XE-136,ENR=0.999) filled in high-pressure gas G002900100016 containers made of titanium. 2.2925 g in total. G002900100017 DETECTOR (HPGE) Equiped with a bismuth germanate (BGO) anti- G002900100018 Compton shield with heavy passive shielding G002900100019 ANALYSIS No systematic deviations observed between the G002900100020 measurements at the two different end-point energies, G002900100021 and thus, the results for the single experiments have G002900100022 been combined. G002900100023 MONITOR (5-B-11(G,EL),,ARE) G002900100024 136Xe target was sandwiched between two 11B targets G002900100025 with a total mass of 0.77 g. G002900100026 Product of the simulated photon spectrum and G002900100027 efficiency is fitted to the experimental values at G002900100028 the 11B energies in order to yield an absolute G002900100029 calibration the entire energy region G002900100030 MONIT-REF (,F.Ajzenberg-Selove,J,NP/A,506,1,1990) G002900100031 COMMENT Denitz Savran (2011-09-02): G002900100032 The experiments at different endpoint energies did G002900100033 not give hints on clear identification of inelastic G002900100034 transition. G002900100035 ERR-ANALYS (DATA-ERR) No information on source of uncertainty G002900100036 STATUS (APRVD) Denitz Savran (2011-09-02) G002900100037 HISTORY (20110901C) On G002900100038 ENDBIB 36 0 G002900100039 NOCOMMON 0 0 G002900100040 ENDSUBENT 39 0 G002900199999 SUBENT G0029002 20110902 G025G002900200001 BIB 3 9 G002900200002 REACTION 1(54-XE-136(G,0),,EN) G002900200003 2((54-XE-136(G,EL)54-XE-136,,DA)// G002900200004 (54-XE-136(G,EL)54-XE-136,,DA)) G002900200005 3((54-XE-136(G,EL),,WID,,SQ)/ G002900200006 (54-XE-136(G,TOT),,WID)) G002900200007 ADD-RES (STRUC) Spin J of the resonances are clearly assigned G002900200008 to 1 except for the following resonances (keV): G002900200009 3626, 5458, 6003, 6030 G002900200010 STATUS (TABLE) Table I of Phys.Rev.C84(2011)024326 G002900200011 ENDBIB 9 0 G002900200012 COMMON 2 3 G002900200013 ANG-NM 2ANG-DN 2 G002900200014 ADEG ADEG G002900200015 90. 130. G002900200016 ENDCOMMON 3 0 G002900200017 DATA 6 77 G002900200018 DATA 1DATA-ERR 1DATA 2DATA-ERR 2DATA 3DATA-ERR 3G002900200019 KEV KEV NO-DIM NO-DIM EV EV G002900200020 3626. 1. 1.20 0.45 0.027 0.006 G002900200021 3738. 1. 0.93 0.13 0.057 0.005 G002900200022 4473. 1. 0.95 0.09 0.120 0.008 G002900200023 4711. 1. 0.76 0.05 0.217 0.013 G002900200024 4890. 1. 0.81 0.07 0.175 0.011 G002900200025 4929. 1. 0.77 0.04 0.341 0.019 G002900200026 5128. 1. 0.75 0.06 0.199 0.013 G002900200027 5187. 1. 0.71 0.10 0.088 0.008 G002900200028 5322. 1. 0.76 0.01 1.66 0.09 G002900200029 5352. 1. 0.74 0.17 0.072 0.009 G002900200030 5458. 1. 1.44 0.44 0.122 0.017 G002900200031 5608. 1. 0.72 0.04 0.491 0.029 G002900200032 5639. 1. 0.75 0.09 0.210 0.017 G002900200033 5651. 1. 0.72 0.05 0.441 0.026 G002900200034 5728. 1. 0.74 0.05 0.382 0.024 G002900200035 5801. 1. 0.77 0.03 2.02 0.11 G002900200036 5872. 1. 0.77 0.02 2.05 0.11 G002900200037 5888. 1. 0.78 0.02 2.59 0.13 G002900200038 5914. 1. 0.80 0.02 1.36 0.07 G002900200039 6003. 1. 1.19 0.33 0.126 0.018 G002900200040 6030. 1. 1.71 0.78 0.088 0.016 G002900200041 6105. 1. 0.97 0.28 0.159 0.026 G002900200042 6115. 1. 0.82 0.06 0.661 0.048 G002900200043 6127. 1. 0.88 0.05 1.10 0.07 G002900200044 6227. 1. 0.97 0.35 0.304 0.050 G002900200045 6254. 1. 0.63 0.16 0.236 0.032 G002900200046 6301. 1. 0.80 0.03 1.99 0.11 G002900200047 6310. 1. 0.89 0.08 0.629 0.042 G002900200048 6324. 1. 0.75 0.13 0.214 0.022 G002900200049 6354. 1. 0.78 0.05 0.796 0.047 G002900200050 6372. 1. 0.82 0.43 0.108 0.030 G002900200051 6430. 1. 0.80 0.06 0.643 0.040 G002900200052 6455. 1. 0.74 0.03 1.38 0.08 G002900200053 6493. 1. 0.73 0.02 2.62 0.14 G002900200054 6509. 1. 0.74 0.07 0.489 0.034 G002900200055 6527. 1. 0.82 0.10 0.410 0.032 G002900200056 6562. 1. 0.73 0.02 2.43 0.13 G002900200057 6577. 1. 0.70 0.05 0.703 0.043 G002900200058 6665. 1. 0.77 0.03 1.81 0.10 G002900200059 6684. 1. 0.70 0.12 0.482 0.047 G002900200060 6691. 1. 0.81 0.06 1.19 0.08 G002900200061 6704. 1. 0.75 0.04 1.32 0.08 G002900200062 6715. 1. 0.85 0.06 1.17 0.07 G002900200063 6734. 1. 0.80 0.07 0.673 0.044 G002900200064 6771. 1. 0.83 0.02 3.46 0.18 G002900200065 6797. 1. 0.81 0.09 0.542 0.040 G002900200066 6808. 1. 0.77 0.23 0.190 0.028 G002900200067 6861. 1. 0.70 0.11 0.407 0.038 G002900200068 6869. 1. 0.79 0.09 0.621 0.048 G002900200069 6884. 1. 0.71 0.10 0.342 0.029 G002900200070 6942. 1. 0.68 0.06 0.668 0.045 G002900200071 6968. 1. 0.47 0.06 0.338 0.030 G002900200072 7013. 1. 0.79 0.06 1.01 0.06 G002900200073 7023. 1. 0.64 0.06 0.683 0.047 G002900200074 7053. 1. 0.74 0.10 0.398 0.033 G002900200075 7071. 1. 0.99 0.11 0.670 0.049 G002900200076 7082. 1. 0.86 0.05 1.44 0.08 G002900200077 7094. 1. 0.90 0.25 0.283 0.044 G002900200078 7121. 1. 0.79 0.11 0.394 0.034 G002900200079 7134. 1. 0.84 0.26 0.247 0.042 G002900200080 7165. 1. 0.77 0.02 3.43 0.18 G002900200081 7193. 1. 1.01 0.19 0.74 0.08 G002900200082 7200. 1. 0.73 0.11 0.84 0.08 G002900200083 7212. 1. 1.15 0.22 0.91 0.09 G002900200084 7232. 1. 0.81 0.06 1.00 0.07 G002900200085 7245. 1. 0.79 0.12 0.361 0.038 G002900200086 7343. 1. 0.69 0.13 0.292 0.031 G002900200087 7370. 1. 0.83 0.14 0.357 0.035 G002900200088 7692. 1. 0.59 0.06 0.78 0.06 G002900200089 7727. 1. 0.80 0.06 1.69 0.11 G002900200090 7883. 1. 0.93 0.17 0.80 0.09 G002900200091 7908. 1. 0.83 0.08 1.65 0.14 G002900200092 7990. 1. 0.98 0.20 0.75 0.09 G002900200093 8024. 1. 0.76 0.08 1.40 0.12 G002900200094 8051. 1. 0.93 0.13 1.11 0.11 G002900200095 8066. 1. 0.75 0.12 0.86 0.09 G002900200096 8093. 1. 0.77 0.10 1.02 0.10 G002900200097 ENDDATA 79 0 G002900200098 ENDSUBENT 97 0 G002900299999 ENDENTRY 2 0 G002999999999