ENTRY A0554 20051026 A061A055400000001 SUBENT A0554001 20051026 A061A055400100001 BIB 9 26 A055400100002 TITLE No evidence of break-up effects on the fusion of 9-Be A055400100003 with medium-light nuclei. A055400100004 AUTHOR (R.M.Anjos, C.Muri, J.Lubian, P.R.S.Gomes, I.Padron, A055400100005 J.J.S.Alves, G.V.Marti, J.O.Fernandes Niello, A055400100006 A.J.Pacheco, O.A.Capurro, D.Abriola, J.E.Testoni, A055400100007 M.Ramires, R.Liguori Neto, N.Added) A055400100008 REFERENCE (J,PL/B,534,45,2002) A055400100009 (J,PR/C,70,054605,2004) Elastic Scattering Data A055400100010 REL-REF (R,,A.GAVRON,J,PR/C,21,230,1980) A055400100011 Statistical code PACE. A055400100012 INSTITUTE (3BZLUFF) Instituto de Fisica A055400100013 (3ARGCNE) Laboratorio TANDAR A055400100014 (3BZLUSP) Departamento de Fisica Nuclear A055400100015 METHOD (EDE) The resolution in both experiments was good A055400100016 enough to separate events differing by one unity of A055400100017 atomic number. A055400100018 (SITA) See SAMPLE A055400100019 PART-DET (RSD) A055400100020 STATUS (TABLE) A055400100021 HISTORY (20030802C) A055400100022 (20030815R) Data tables were received from J.Lubian A055400100023 (20030820R) Data table for elastic scattering were A055400100024 received from J.Lubian A055400100025 (20051026A) Additional reference is added. FACILITY is A055400100026 Added to SUBENT A0554005 A055400100027 (20051026U) Last checking has been done. A055400100028 ENDBIB 26 0 A055400100029 NOCOMMON 0 0 A055400100030 ENDSUBENT 29 0 A055400199999 SUBENT A0554002 20030831 0000A055400200001 BIB 9 25 A055400200002 REACTION (13-AL-27(4-BE-9,FUS),,SIG) A055400200003 FACILITY (VDGT,3ARGCNE) The 20UD TANDAR laboratory. A055400200004 DETECTOR (TELES,IOCH,SIBAR) A large ionization champer, A055400200005 followed by a surface barrier detector. A055400200006 SAMPLE The aluminum target thickness was approximately 80 A055400200007 microgramm/cm**2, a thin gold layer of 10 A055400200008 microgramm/cm**2 was evaporated on it for normalizationA055400200009 purposes. A055400200010 REL-REF (R,,R.M.ANJOS+,J,PR/C,42,354,1990) A055400200011 The data for 27-Al+11-B. A055400200012 (R,,M.C.S.FIGUIERA+,J,NP/A,561,453,1993) A055400200013 The data for 9-Be+29-Si. A055400200014 ANALYSIS (INTAD) Angular distributions were obtained A055400200015 at four different angles (10, 12, 15, 20). The maxima A055400200016 of the angular distributions were located near 12 A055400200017 degree, and therefore the experimental angular A055400200018 distributions covered around 80% of the complete A055400200019 angular distribution. A055400200020 CORRECTION The extrapolation to the most forward part of the A055400200021 distributions were performed with the use of the shape A055400200022 of the theoretical predictions obtained by the A055400200023 statistical code PACE. A055400200024 ERR-ANALYS (ERR-T) The precision of this method allows the A055400200025 evaluation of the complete angular distribution. A055400200026 ADD-RES (COMP) With data 9-Be+29-Si and 11-B+27-Al A055400200027 ENDBIB 25 0 A055400200028 NOCOMMON 0 0 A055400200029 DATA 3 10 A055400200030 EN-CM DATA ERR-T A055400200031 MEV MB MB A055400200032 24.75 1059. 63. A055400200033 26.25 1103. 66. A055400200034 28.12 1141. 68. A055400200035 30. 1161. 70. A055400200036 31.87 1147. 79. A055400200037 33.75 1182. 82. A055400200038 35.62 1140. 79. A055400200039 37.5 1153. 87. A055400200040 39.37 1151. 86. A055400200041 41.25 1147. 86. A055400200042 ENDDATA 12 0 A055400200043 ENDSUBENT 42 0 A055400299999 SUBENT A0554003 20030831 0000A055400300001 BIB 9 24 A055400300002 REACTION (4-BE-9(9-F-19,FUS),,SIG) A055400300003 FACILITY (VDGT,3BZLUSP) 8UD pelletron laboratory A055400300004 DETECTOR (TELES,IOCH,PSSSD) A large anode-splitted ionization A055400300005 chamber and a position sensitive silicon detector. A055400300006 SAMPLE The 9-Be target thickness was approximately 80 A055400300007 microgramm/cm**2, deposited onto carbon backing of ~10 A055400300008 microgramm/cm**2, a thin gold layer of 10 A055400300009 microgramm/cm**2 was evaporated on it for normalizationA055400300010 purposes. A055400300011 REL-REF (R,,R.M.ANJOS+,J,PR/C,49,2018,1994) A055400300012 The data for 18-O+10-B and 17-O+11-B. A055400300013 ANALYSIS (INTAD) Angular distributions were obtained in the A055400300014 range 7 - 37 degrees. The maxima of the angular A055400300015 distributions were located near 12 degree, and A055400300016 therefore the experimental angular distributions A055400300017 covered around 80% of the complete angular A055400300018 distribution. A055400300019 CORRECTION The extrapolation to the most forward part of the A055400300020 distributions were performed with the use of the shape A055400300021 of the theoretical predictions obtained by the A055400300022 statistical code PACE. A055400300023 ERR-ANALYS (ERR-T) The precision of this method allows the A055400300024 evaluation of the complete angular distribution. A055400300025 ADD-RES (COMP) With data 18-O+10-B and 17-O+11-B. A055400300026 ENDBIB 24 0 A055400300027 NOCOMMON 0 0 A055400300028 DATA 3 7 A055400300029 EN-CM DATA ERR-T A055400300030 MEV MB MB A055400300031 15.43 927. 75. A055400300032 16.71 967. 79. A055400300033 18. 1030. 90. A055400300034 19.29 1074. 85. A055400300035 20.57 1115. 88. A055400300036 21.86 1146. 91. A055400300037 23.14 1110. 95. A055400300038 ENDDATA 9 0 A055400300039 ENDSUBENT 38 0 A055400399999 SUBENT A0554004 20030831 0000A055400400001 BIB 9 24 A055400400002 REACTION (6-C-12(9-F-19,FUS),,SIG) Figure 1 A055400400003 FACILITY (VDGT,3BZLUSP) 8UD pelletron laboratory A055400400004 DETECTOR (TELES,IOCH,PSSSD) A large anode-splitted ionization A055400400005 chamber and a position sensitive silicon detector. A055400400006 SAMPLE The 9-Be target thickness was approximately 80 A055400400007 microgramm/cm**2, deposited onto carbon backing of ~10 A055400400008 microgramm/cm**2, a thin gold layer of 10 A055400400009 microgramm/cm**2 was evaporated on it for normalizationA055400400010 purposes. A055400400011 REL-REF (R,,P.SPERR+,J,PRL,37,321,1976) A055400400012 The data for 12-C+19-F A055400400013 ANALYSIS (INTAD) Angular distributions were obtained in the A055400400014 range 7 - 37 degrees. The maxima of the angular A055400400015 distributions were located near 12 degree, and A055400400016 therefore the experimental angular distributions A055400400017 covered around 80% of the complete angular A055400400018 distribution. A055400400019 CORRECTION The extrapolation to the most forward part of the A055400400020 distributions were performed with the use of the shape A055400400021 of the theoretical predictions obtained by the A055400400022 statistical code PACE. A055400400023 ERR-ANALYS (ERR-T) The precision of this method allows the A055400400024 evaluation of the complete angular distribution. A055400400025 FLAG (1.) The datum from REL-REF A055400400026 ENDBIB 24 0 A055400400027 NOCOMMON 0 0 A055400400028 DATA 4 16 A055400400029 EN-CM DATA ERR-T FLAG A055400400030 MEV MB MB NO-DIM A055400400031 11.68 567. 38. 1. A055400400032 13.47 759. 42. 1. A055400400033 15.33 899. 54. 1. A055400400034 17.37 1000. 65. 1. A055400400035 18.58 1020. 82. A055400400036 19.23 1097. 72. 1. A055400400037 20.13 1045. 85. A055400400038 21.28 1123. 74. 1. A055400400039 21.68 1115. 91. A055400400040 23.1 1185. 80. 1. A055400400041 23.22 1142. 95. A055400400042 24.77 1161. 94. A055400400043 24.94 1205. 80. 1. A055400400044 26.32 1120. 92. A055400400045 27.01 1133. 98. 1. A055400400046 27.87 1075. 86. A055400400047 ENDDATA 18 0 A055400400048 ENDSUBENT 47 0 A055400499999 SUBENT A0554005 20051026 A061A055400500001 BIB 3 4 A055400500002 REACTION (13-AL-27(4-BE-9,EL)13-AL-27,,DA,,RTH) A055400500003 FACILITY (VDGT,3BZLUSP) 8 UD Pelletron. A055400500004 (ACCEL,3ARGCNE) 20 UD accelerator of TANDAR Laboratory.A055400500005 ERR-ANALYS (ERR-T) The uncertainty is given in data table. A055400500006 ENDBIB 4 0 A055400500007 NOCOMMON 0 0 A055400500008 DATA 4 134 A055400500009 EN ANG-CM DATA-CM ERR-T A055400500010 MEV ADEG NO-DIM NO-DIM A055400500011 12. 19.95 1. 0.06 A055400500012 12. 26.55 0.979 0.059 A055400500013 12. 33.1 0.945 0.057 A055400500014 12. 39.59 0.955 0.076 A055400500015 12. 46.02 0.982 0.078 A055400500016 12. 52.37 1.021 0.082 A055400500017 12. 58.63 0.973 0.078 A055400500018 12. 64.79 0.959 0.077 A055400500019 12. 70.85 0.956 0.076 A055400500020 12. 76.78 0.901 0.072 A055400500021 12. 82.58 0.773 0.077 A055400500022 12. 88.25 0.658 0.066 A055400500023 12. 93.78 0.595 0.059 A055400500024 12. 99.16 0.561 0.056 A055400500025 12. 104.39 0.469 0.047 A055400500026 12. 109.47 0.399 0.04 A055400500027 12. 114.39 0.453 0.045 A055400500028 14. 19.95 1. 0.06 A055400500029 14. 26.55 0.97 0.058 A055400500030 14. 33.1 0.943 0.056 A055400500031 14. 39.59 0.972 0.077 A055400500032 14. 46.02 1.045 0.083 A055400500033 14. 52.37 0.974 0.078 A055400500034 14. 58.63 0.823 0.066 A055400500035 14. 64.79 0.654 0.052 A055400500036 14. 70.85 0.608 0.048 A055400500037 14. 70.85 0.621 0.05 A055400500038 14. 76.78 0.511 0.041 A055400500039 14. 82.58 0.392 0.039 A055400500040 14. 88.25 0.343 0.034 A055400500041 14. 93.78 0.286 0.028 A055400500042 14. 99.16 0.231 0.023 A055400500043 14. 104.39 0.172 0.017 A055400500044 14. 109.47 0.137 0.014 A055400500045 14. 114.39 0.127 0.013 A055400500046 18. 13.32 1. 0.06 A055400500047 18. 19.95 0.982 0.059 A055400500048 18. 26.55 0.929 0.055 A055400500049 18. 33.1 0.874 0.052 A055400500050 18. 39.59 0.702 0.056 A055400500051 18. 46.02 0.528 0.042 A055400500052 18. 52.37 0.366 0.029 A055400500053 18. 58.63 0.27 0.022 A055400500054 18. 64.79 0.21 0.017 A055400500055 18. 70.85 0.15 0.012 A055400500056 18. 76.78 0.1 0.008 A055400500057 18. 82.58 0.081 0.008 A055400500058 18. 88.25 0.054 0.005 A055400500059 18. 93.78 0.028 0.003 A055400500060 18. 99.16 0.014 0.001 A055400500061 18. 104.39 0.02 0.002 A055400500062 22. 13.32 1. 0.06 A055400500063 22. 19.95 1.059 0.063 A055400500064 22. 26.55 0.844 0.051 A055400500065 22. 33.1 0.595 0.036 A055400500066 22. 39.59 0.421 0.034 A055400500067 22. 46.02 0.292 0.023 A055400500068 22. 52.37 0.173 0.014 A055400500069 22. 58.63 0.113 0.009 A055400500070 22. 64.79 0.085 0.007 A055400500071 22. 70.85 0.046 0.004 A055400500072 22. 76.78 0.034 0.003 A055400500073 25. 13.32 1. 0.06 A055400500074 25. 19.95 1.049 0.063 A055400500075 25. 26.55 0.67 0.04 A055400500076 25. 33.1 0.424 0.025 A055400500077 25. 39.59 0.269 0.022 A055400500078 25. 46.02 0.174 0.014 A055400500079 25. 52.37 0.108 0.002 A055400500080 25. 58.63 0.069 0.005 A055400500081 25. 64.79 0.044 0.004 A055400500082 25. 70.85 0.026 0.002 A055400500083 25. 76.78 0.015 0.001 A055400500084 28. 13.32 1. 0.06 A055400500085 28. 19.95 0.82 0.049 A055400500086 28. 26.55 0.468 0.028 A055400500087 28. 33.1 0.232 0.014 A055400500088 28. 39.59 0.142 0.008 A055400500089 28. 46.02 0.081 0.006 A055400500090 28. 52.37 0.059 0.005 A055400500091 28. 58.63 0.028 0.002 A055400500092 28. 64.79 0.018 0.001 A055400500093 28. 70.85 0.007 0.0006 A055400500094 32. 13.32 1. 0.06 A055400500095 32. 16.64 0.763 0.046 A055400500096 32. 19.95 0.579 0.035 A055400500097 32. 23.25 0.371 0.022 A055400500098 32. 26.55 0.319 0.019 A055400500099 32. 29.83 0.214 0.013 A055400500100 32. 33.1 0.145 0.009 A055400500101 32. 36.35 0.115 0.007 A055400500102 32. 39.59 0.083 0.005 A055400500103 32. 42.82 0.056 0.005 A055400500104 32. 46.02 0.045 0.004 A055400500105 32. 49.21 0.035 0.003 A055400500106 32. 52.37 0.027 0.002 A055400500107 32. 55.51 0.018 0.001 A055400500108 32. 58.63 0.014 0.001 A055400500109 32. 61.73 0.009 0.0007 A055400500110 32. 64.79 0.007 0.0006 A055400500111 32. 67.83 0.006 0.0005 A055400500112 33. 13.32 1. 0.06 A055400500113 33. 13.32 1. 0.068 A055400500114 33. 15.97 0.996 0.068 A055400500115 33. 16.64 0.816 0.048 A055400500116 33. 19.95 0.532 0.032 A055400500117 33. 19.95 0.801 0.057 A055400500118 33. 23.25 0.39 0.023 A055400500119 33. 26.55 0.275 0.016 A055400500120 33. 26.55 0.48 0.033 A055400500121 33. 29.83 0.174 0.01 A055400500122 33. 33.1 0.126 0.007 A055400500123 33. 33.1 0.185 0.015 A055400500124 33. 36.35 0.1 0.006 A055400500125 33. 39.59 0.059 0.003 A055400500126 33. 42.82 0.048 0.004 A055400500127 33. 46.02 0.032 0.002 A055400500128 33. 49.21 0.023 0.002 A055400500129 33. 52.37 0.019 0.001 A055400500130 33. 55.51 0.016 0.001 A055400500131 33. 58.63 0.01 0.0008 A055400500132 33. 61.73 0.007 0.0006 A055400500133 33. 64.79 0.005 0.0004 A055400500134 33. 67.83 0.008 0.0006 A055400500135 40. 13.32 0.779 0.046 A055400500136 40. 13.32 0.781 0.047 A055400500137 40. 15.97 0.523 0.031 A055400500138 40. 15.97 0.843 0.051 A055400500139 40. 19.95 0.313 0.019 A055400500140 40. 19.95 0.425 0.026 A055400500141 40. 26.55 0.121 0.01 A055400500142 40. 26.55 0.191 0.015 A055400500143 40. 33.1 0.039 0.003 A055400500144 40. 33.1 0.109 0.009 A055400500145 ENDDATA 136 0 A055400500146 ENDSUBENT 145 0 A055400599999 ENDENTRY 5 0 A055499999999