ENTRY O1719 20081217 O038O171900000001 SUBENT O1719001 20081217 O038O171900100001 BIB 12 38 O171900100002 TITLE Production of medium-mass neutron-rich nuclei in O171900100003 reactions induced by Xe-136 projectiles at 1 A*GeV O171900100004 on beryllium target. O171900100005 AUTHOR (J.Benlliure, M.Fernandez-Ordonez, L.Audouin, O171900100006 A.Boudard, E.Casarejos, J.E.Ducret, T.Enqvist, A.Heinz,O171900100007 D.Henzlova, V.Henzl, A.Kelic, S.Leray, P.Napolitani, O171900100008 J.Pereira, F.Rejmund, M.V.Ricciardi, K.-H.Schmidt, O171900100009 C.Schmitt, C.Stephan, L.Tassan-Got, C.Volant, O171900100010 C.Villagrasa, O.Yordanov) O171900100011 INSTITUTE (2SPNSAU) O171900100012 (2FR PAR) IPN Orsay, IN2P3 O171900100013 (2FR SAC) DAPNIA/SPhN CEA Saclay O171900100014 (2GERGSI) O171900100015 REFERENCE (J,PR/C,78,054605,2008) O171900100016 REL-REF (R,O1589001,P.Napolitani+,J,PR/C,76,064609,2007) O171900100017 Experimental method. O171900100018 SAMPLE A beryllium target with an effective thickness of O171900100019 2. g/cm**2. O171900100020 DETECTOR (MAGSP) Reaction residues with trajectories inside O171900100021 the FRS acceptance for a given magnetic tuning were O171900100022 identified from their magnetic rigidity and time of O171900100023 flight. O171900100024 (SCIN).Two position-sensitive plastic scintillators. O171900100025 (IOCH).An ionization chamber MUSIC. O171900100026 FACILITY (SYNCH,2GERGSI) The SIS18 synchrotron. O171900100027 (FRS,2GERGSI) O171900100028 METHOD (TOF) O171900100029 (ASEP) O171900100030 STATUS (TABLE) Table 1 O171900100031 COMMENT *By authors*.The measured production yields were O171900100032 transformed into production cross sections by O171900100033 normalizing to the number of incident projectiles and O171900100034 target thickness. Before that, the measured yields wereO171900100035 corrected by the FRS acceptance and losses due to the O171900100036 dead time of the data acquisition, reactions in all O171900100037 layers of matter along the FRS, multiple reactions O171900100038 in the target and charge states of the residual nuclei.O171900100039 HISTORY (20081217C) sb O171900100040 ENDBIB 38 0 O171900100041 COMMON 1 3 O171900100042 EN O171900100043 MEV O171900100044 136000. O171900100045 ENDCOMMON 3 0 O171900100046 ENDSUBENT 45 0 O171900199999 SUBENT O1719002 20081217 O038O171900200001 BIB 2 10 O171900200002 REACTION (4-BE-9(54-XE-136,X)ELEM/MASS,,SIG) O171900200003 ERR-ANALYS The uncertainty below 10% on average for the heavy O171900200004 nuclides accounts for all statistical and systematicalO171900200005 contributions: statistics, analysis and fitting of the O171900200006 velocity spectra, procedure of velocity reconstruction O171900200007 (reflected in the uncertainty of the transmission O171900200008 probability), calibration of the beam monitor, O171900200009 secondary reactions in the target and in the beam line.O171900200010 (ERR-T).The uncertainty is reported by authors in tableO171900200011 See detail description above and o1589002. O171900200012 ENDBIB 10 0 O171900200013 NOCOMMON 0 0 O171900200014 DATA 4 111 O171900200015 ELEMENT MASS DATA ERR-T O171900200016 NO-DIM NO-DIM MB MB O171900200017 55. 136. 0.60 0.07 O171900200018 55. 135. 1.55 0.17 O171900200019 55. 134. 2.59 0.29 O171900200020 55. 133. 3.22 0.36 O171900200021 55. 132. 3.16 0.35 O171900200022 54. 135. 109. 12. O171900200023 54. 134. 51.1 5.6 O171900200024 54. 133. 31.7 3.5 O171900200025 54. 132. 28.8 3.2 O171900200026 54. 131. 19.9 2.2 O171900200027 54. 130. 16.7 1.7 O171900200028 54. 129. 13.3 1.5 O171900200029 53. 136. 0.036 0.004 O171900200030 53. 135. 16.7 1.8 O171900200031 53. 134. 16.3 1.8 O171900200032 53. 133. 18.8 2.1 O171900200033 53. 132. 18.1 2.0 O171900200034 53. 131. 18.9 2.1 O171900200035 53. 130. 17.1 1.9 O171900200036 53. 129. 18.6 2.1 O171900200037 53. 128. 15.9 1.8 O171900200038 53. 127. 15.5 1.7 O171900200039 52. 135. 0.0027 0.0003 O171900200040 52. 134. 0.30 0.03 O171900200041 52. 133. 1.18 0.13 O171900200042 52. 132. 2.55 0.12 O171900200043 52. 130. 5.24 0.58 O171900200044 52. 129. 6.97 0.78 O171900200045 52. 128. 7.54 0.83 O171900200046 52. 127. 9.60 0.99 O171900200047 52. 126. 7.54 0.83 O171900200048 52. 125. 10.9 1.2 O171900200049 51. 134. 0.0000309 0.0000037 O171900200050 51. 133. 0.00669 0.00073 O171900200051 51. 132. 0.0449 0.0049 O171900200052 51. 131. 0.19 0.02 O171900200053 51. 130. 0.42 0.05 O171900200054 51. 129. 0.84 0.09 O171900200055 51. 127. 2.22 0.25 O171900200056 51. 126. 3.02 0.33 O171900200057 51. 125. 4.10 0.45 O171900200058 51. 124. 5.31 0.59 O171900200059 51. 123. 6.25 0.69 O171900200060 50. 132. 0.000119 0.000013 O171900200061 50. 131. 0.00122 0.00013 O171900200062 50. 130. 0.00729 0.00081 O171900200063 50. 129. 0.0275 0.0030 O171900200064 50. 128. 0.0745 0.0092 O171900200065 50. 127. 0.18 0.02 O171900200066 50. 125. 0.64 0.08 O171900200067 50. 124. 1.04 0.13 O171900200068 50. 123. 1.56 0.18 O171900200069 50. 122. 2.28 0.26 O171900200070 50. 121. 3.17 0.35 O171900200071 50. 120. 4.23 0.47 O171900200072 49. 131. 0.00000675 0.00000077 O171900200073 49. 130. 0.0000535 0.0000063 O171900200074 49. 129. 0.000365 0.000041 O171900200075 49. 128. 0.00178 0.00019 O171900200076 49. 127. 0.00649 0.00072 O171900200077 49. 126. 0.0189 0.0057 O171900200078 49. 125. 0.0580 0.0075 O171900200079 49. 124. 0.13 0.07 O171900200080 49. 122. 0.38 0.05 O171900200081 49. 121. 0.63 0.07 O171900200082 49. 120. 1.03 0.12 O171900200083 49. 119. 1.58 0.18 O171900200084 49. 118. 2.24 0.25 O171900200085 48. 130. 0.0000001390.000000030 O171900200086 48. 129. 0.00000257 0.00000031 O171900200087 48. 128. 0.0000206 0.0000023 O171900200088 48. 127. 0.0000830 0.0000097 O171900200089 48. 126. 0.000377 0.000024 O171900200090 48. 125. 0.00136 0.00016 O171900200091 48. 124. 0.00488 0.0005 O171900200092 48. 123. 0.0129 0.0039 O171900200093 48. 121. 0.0803 0.0040 O171900200094 48. 119. 0.29 0.04 O171900200095 48. 118. 0.44 0.05 O171900200096 48. 117. 0.83 0.10 O171900200097 48. 116. 1.18 0.13 O171900200098 48. 115. 1.78 0.20 O171900200099 47. 128. 6.77E-08 2.17E-08 O171900200100 47. 127. 8.19E-08 1.16E-08 O171900200101 47. 126. 5.47E-06 6.30E-07 O171900200102 47. 125. 2.73E-05 3.30E-06 O171900200103 47. 124. 9.61E-05 1.10E-06 O171900200104 47. 123. 3.46E-04 4.10E-05 O171900200105 47. 122. 9.28E-04 2.32E-04 O171900200106 46. 125. 9.38E-08 2.71E-08 O171900200107 46. 124. 1.34E-06 7.20E-07 O171900200108 46. 123. 6.25E-06 7.20E-07 O171900200109 46. 122. 2.96E-05 2.00E-06 O171900200110 46. 121. 9.92E-05 1.20E-06 O171900200111 46. 120. 2.67E-04 5.30E-05 O171900200112 46. 119. 6.61E-04 1.98E-04 O171900200113 45. 122. 2.05E-07 4.70E-08 O171900200114 45. 121. 1.49E-06 1.90E-07 O171900200115 45. 120. 5.36E-06 6.20E-07 O171900200116 45. 119. 1.86E-05 2.20E-06 O171900200117 45. 118. 5.26E-05 6.30E-06 O171900200118 45. 117. 1.36E-04 3.20E-05 O171900200119 44. 119. 2.72E-07 5.20E-08 O171900200120 44. 118. 1.42E-06 1.80E-07 O171900200121 43. 117. 5.28E-08 2.08E-08 O171900200122 43. 116. 2.23E-07 4.60E-08 O171900200123 43. 115. 3.43E-06 4.50E-07 O171900200124 42. 113. 2.59E-07 5.10E-08 O171900200125 41. 111. 4.08E-08 1.72E-08 O171900200126 41. 110. 2.51E-07 5.10E-08 O171900200127 40. 108. 6.05E-08 2.24E-08 O171900200128 ENDDATA 113 0 O171900200129 ENDSUBENT 128 0 O171900299999 ENDENTRY 2 0 O171999999999