ENTRY D6029 20091106 D070D602900000001 SUBENT D6029001 20091106 D070D602900100001 BIB 9 18 D602900100002 TITLE Coupled reaction channel analysis of elastic, D602900100003 inelastic, transfer, and fusion cross sections D602900100004 for 12C + 208Pb D602900100005 AUTHOR (S.Santra,P.Singh,S.Kailas,A.Chatterjee, D602900100006 A.Shrivastava,K.Mahata) D602900100007 INSTITUTE (3INDTRM) Bhabha Atomic Research Centre D602900100008 REFERENCE (J,PR/C,64,024602,20010625) D602900100009 #doi:10.1103/PhysRevC.64.024602 D602900100010 FACILITY (VDG,3INDTRM)Bhabha Atomic Research Centre, BARC-TIFR D602900100011 14UD Pelletron at Mumbai D602900100012 SAMPLE The targets used were prepared by vacuum evaporation D602900100013 of Pb-208 (of thicknes approx. 250 micro-gm/cm2) D602900100014 onto a C-12 backing (of thickness approx. D602900100015 40 micro-gm/cm2) D602900100016 METHOD (EDE) D602900100017 STATUS (CURVE) Data were digitized from figures D602900100018 HISTORY (20091106C)compiled by Gaurav Aggarwal, Sachin Chachra D602900100019 Sanat Kumar Pandit D602900100020 ENDBIB 18 0 D602900100021 NOCOMMON 0 0 D602900100022 ENDSUBENT 21 0 D602900199999 SUBENT D6029002 20091106 D070D602900200001 BIB 4 18 D602900200002 REACTION (82-PB-208(6-C-12,EL)82-PB-208,,DA,,RTH) D602900200003 DETECTOR (TELES,SIBAR,SIBAR)Three telescopes (DeltaE-E) of D602900200004 silicon surface barrier (SSB) detectors were set up D602900200005 inside a 1 m diameter scattering chamber for measuring D602900200006 the Projectile-like particles. A monitor (single SSB) D602900200007 detector was mounted at 20 deg with respect to beam D602900200008 direction for normalization. A second monitor at 25 degD602900200009 was mounted on the wall of the scattering chamber. D602900200010 The angular distributions were measured in the range D602900200011 20deg to 173 deg(lab). The angular resolution was aboutD602900200012 0.5 deg. The detector thicknesses were typically 20 to D602900200013 45 micro-metre for DeltaE and 300 to 2000 micro-metre D602900200014 for E detectors. Proper gain matching in DeltaE and E D602900200015 signals led to a total energy resolution of D602900200016 approx. 500 keV. D602900200017 ERR-ANALYS (ANG-ERR-D) Digitizing error D602900200018 (ERR-DIG) Digitizing error D602900200019 STATUS (CURVE)Fig1 D602900200020 ENDBIB 18 0 D602900200021 COMMON 2 3 D602900200022 ANG-ERR-D ERR-DIG D602900200023 ADEG PER-CENT D602900200024 0.5 0.2 D602900200025 ENDCOMMON 3 0 D602900200026 DATA 4 115 D602900200027 EN ANG-CM DATA DATA-ERR D602900200028 MEV ADEG NO-DIM NO-DIM D602900200029 58.9 83.9 1. 1.55E-02 D602900200030 58.9 94.0 0.998 2.23E-02 D602900200031 58.9 103.9 1.0128 2.18E-02 D602900200032 58.9 113.6 0.9922 2.16E-02 D602900200033 58.9 123.5 0.9989 2.08E-02 D602900200034 58.9 133.2 1.0284 1.88E-02 D602900200035 58.9 142.8 0.9451 1.73E-02 D602900200036 58.9 152.3 0.8255 2.39E-02 D602900200037 58.9 155.0 0.7752 2.12E-02 D602900200038 58.9 161.8 0.7621 1.92E-02 D602900200039 58.9 164.4 0.7512 1.74E-02 D602900200040 58.9 171.2 0.7428 1.75E-02 D602900200041 58.9 173.9 0.6958 1.53E-02 D602900200042 60.9 53.2 1.0381 1.63E-02 D602900200043 60.9 63.5 1.024 1.81E-02 D602900200044 60.9 73.8 0.9561 1.88E-02 D602900200045 60.9 83.9 1.0096 1.45E-02 D602900200046 60.9 94.0 0.9552 1.84E-02 D602900200047 60.9 103.9 0.9271 1.81E-02 D602900200048 60.9 113.6 1.0454 1.9E-02 D602900200049 60.9 123.5 0.8921 1.9E-02 D602900200050 60.9 133.2 0.6806 1.58E-02 D602900200051 60.9 142.8 0.5373 1.3E-02 D602900200052 60.9 155.0 0.3193 1.01E-02 D602900200053 60.9 164.4 0.3084 8.9E-03 D602900200054 60.9 173.9 0.2594 7.3E-03 D602900200055 62.9 42.8 1.01 1.93E-02 D602900200056 62.9 53.2 1.0438 2.21E-02 D602900200057 62.9 63.5 0.9875 2.53E-02 D602900200058 62.9 73.8 1.0438 2.11E-02 D602900200059 62.9 83.9 0.9275 2.08E-02 D602900200060 62.9 93.7 0.9727 2.06E-02 D602900200061 62.9 103.9 0.9641 2.03E-02 D602900200062 62.9 113.6 0.8429 1.66E-02 D602900200063 62.9 123.5 0.5103 1.53E-02 D602900200064 62.9 133.2 0.343 1.2E-02 D602900200065 62.9 142.8 0.2081 8.6E-02 D602900200066 64.9 32.3 1.0381 1.39E-02 D602900200067 64.9 37.6 0.9764 1.09E-02 D602900200068 64.9 42.8 1.0195 1.46E-02 D602900200069 64.9 48.0 0.981 1.19E-02 D602900200070 64.9 53.2 1.0104 1.6E-02 D602900200071 64.9 58.4 0.9893 1.33E-02 D602900200072 64.9 63.5 0.9903 1.29E-02 D602900200073 64.9 73.8 1.0024 1.41E-02 D602900200074 64.9 78.9 0.9704 1.8E-02 D602900200075 64.9 83.9 1.158 1.79E-02 D602900200076 64.9 89.0 1.0845 2.1E-02 D602900200077 64.9 91.0 1.1325 1.41E-02 D602900200078 64.9 100.9 0.85 1.39E-02 D602900200079 64.9 103.9 0.75 1.26E-02 D602900200080 64.9 108.8 0.5695 1.09E-02 D602900200081 64.9 113.6 0.492 1.15E-02 D602900200082 64.9 118.6 0.388 9.1E-03 D602900200083 64.9 123.5 0.2481 7.9E-03 D602900200084 64.9 128.3 0.21 6.E-03 D602900200085 64.9 133.2 0.1734 6.2E-03 D602900200086 69.9 21.8 0.979 1.81E-02 D602900200087 69.9 27.1 1.008 1.59E-02 D602900200088 69.9 32.3 1.044 2.26E-02 D602900200089 69.9 37.6 1.058 1.78E-02 D602900200090 69.9 42.8 1.033 2.38E-02 D602900200091 69.9 48.0 1.044 1.93E-02 D602900200092 69.9 53.2 1.008 1.2E-02 D602900200093 69.9 58.4 0.9519 1.04E-02 D602900200094 69.9 63.5 0.9637 1.3E-02 D602900200095 69.9 68.7 0.9944 1.23E-02 D602900200096 69.9 73.8 1.132 1.62E-02 D602900200097 69.9 78.9 1.044 1.4E-02 D602900200098 69.9 83.9 0.9553 1.2E-02 D602900200099 69.9 89.0 0.7464 1.17E-02 D602900200100 69.9 94.0 0.5259 9.5E-03 D602900200101 69.9 98.9 0.3488 1.25E-02 D602900200102 69.9 103.9 0.2023 6.E-03 D602900200103 69.9 108.8 0.165 9.E-03 D602900200104 69.9 113.6 9.E-02 3.1E-03 D602900200105 69.9 118.6 5.3E-02 4.5E-03 D602900200106 69.9 128.3 2.78E-02 3.5E-03 D602900200107 69.9 138.0 1.54E-02 2.5E-03 D602900200108 74.9 21.8 1.064 1.77E-02 D602900200109 74.9 27.1 1.029 1.74E-02 D602900200110 74.9 32.3 1.067 1.87E-02 D602900200111 74.9 37.6 1.019 1.78E-02 D602900200112 74.9 42.8 1.094 2.04E-02 D602900200113 74.9 48.0 1.075 1.98E-02 D602900200114 74.9 53.2 0.901 1.24E-02 D602900200115 74.9 58.4 0.915 1.28E-02 D602900200116 74.9 63.5 1.102 1.62E-02 D602900200117 74.9 68.7 1.092 1.63E-02 D602900200118 74.9 73.8 0.9088 1.56E-02 D602900200119 74.9 78.9 0.6131 1.24E-02 D602900200120 74.9 83.9 0.3898 9.1E-03 D602900200121 74.9 94.0 0.1202 5.3E-03 D602900200122 74.9 98.9 6.5E-02 2.9E-03 D602900200123 74.9 103.9 3.47E-02 3.E-03 D602900200124 84.9 21.8 1.0283 1.24E-02 D602900200125 84.9 27.1 0.9979 1.01E-02 D602900200126 84.9 32.3 0.9507 1.22E-02 D602900200127 84.9 37.6 1.0204 1.32E-02 D602900200128 84.9 42.8 0.8944 1.23E-02 D602900200129 84.9 48.0 1.0189 1.48E-02 D602900200130 84.9 50.6 1.1319 1.43E-02 D602900200131 84.9 53.2 1.0654 1.61E-02 D602900200132 84.9 55.8 1.117 1.43E-02 D602900200133 84.9 58.4 0.9392 1.54E-02 D602900200134 84.9 61.0 0.7589 1.19E-02 D602900200135 84.9 63.5 0.634 7.9E-03 D602900200136 84.9 66.1 0.4292 8.6E-03 D602900200137 84.9 71.2 0.2163 6.2E-03 D602900200138 84.9 73.8 0.1482 4.E-03 D602900200139 84.9 76.3 0.1032 4.4E-03 D602900200140 84.9 78.9 7.64E-02 2.8E-03 D602900200141 84.9 83.9 2.28E-02 1.7E-03 D602900200142 84.9 89.0 1.16E-02 1.2E-03 D602900200143 84.9 98.9 3.58E-03 7.E-04 D602900200144 ENDDATA 117 0 D602900200145 ENDSUBENT 144 0 D602900299999 SUBENT D6029003 20091105 D070D602900300001 BIB 3 5 D602900300002 REACTION (82-PB-208(6-C-12,F),,SIG) D602900300003 DETECTOR (TELES,SIBAR,SIBAR)Two telescopes (DeltaE-E) of SSB D602900300004 detectors were used.One monitor (single SSB detector) D602900300005 was kept at 40 deg for normalization. D602900300006 STATUS (CURVE)Fig4 D602900300007 ENDBIB 5 0 D602900300008 NOCOMMON 0 0 D602900300009 DATA 3 6 D602900300010 EN DATA DATA-ERR D602900300011 MEV MB MB D602900300012 58.9 1.20 0.3 D602900300013 60.9 8.13 1.5 D602900300014 62.9 17.71 3.3 D602900300015 65.0 34.05 4.8 D602900300016 72.0 155.0 14.7 D602900300017 79.0 361.0 34.3 D602900300018 ENDDATA 8 0 D602900300019 ENDSUBENT 18 0 D602900399999 SUBENT D6029004 20091105 D070D602900400001 BIB 3 17 D602900400002 REACTION (82-PB-208(6-C-12,2N)88-RA-218,,SIG) D602900400003 DETECTOR (TELES,SIBAR,SIBAR)Two telescopes (DeltaE-E) of SSB D602900400004 detectors were used.The residue cross sections for D602900400005 the 2n channel have been measured in the present work D602900400006 by alpha counting at energies 58.9, 60.9, and 62.9 MeV D602900400007 to supplement the ER measurement. For ER measurements, D602900400008 three targets (with thin aluminum catcher foils on the D602900400009 back) were irradiated at different energies (58.9, D602900400010 60.9, and 62.9 MeV) for 5 hours each to populate the D602900400011 compound nucleus 220Ra. After two-neutron evaporation D602900400012 and a decay of the daughter and grand daughter, the D602900400013 CN populates PO-210, which has a half-life of 138 d. D602900400014 The alpha activity of PO-210 has been measured to D602900400015 determine the 2n evaporation residue (ER) cross D602900400016 sections. The activity of catcher foil was also taken D602900400017 into account. D602900400018 STATUS (TABLE)Table-III D602900400019 ENDBIB 17 0 D602900400020 NOCOMMON 0 0 D602900400021 DATA 3 3 D602900400022 EN DATA DATA-ERR D602900400023 MEV MB MB D602900400024 58.9 10.4 2.1 D602900400025 60.9 35.0 7.0 D602900400026 62.9 27.0 5.4 D602900400027 ENDDATA 5 0 D602900400028 ENDSUBENT 27 0 D602900499999 SUBENT D6029005 20091105 D070D602900500001 BIB 5 12 D602900500002 REACTION (82-PB-208(6-C-12,FUS)88-RA-220,,SIG,,,DERIV) D602900500003 COMMENT Fusion cross section data has been derived by adding D602900500004 fission cross section with the corresponding D602900500005 evaporation residues (ERs) at all the energies. ER for D602900500006 2n was measured in this experiment, others (for 3n, 4n,D602900500007 and 5n) were taken from lit. (see REL-REF) D602900500008 REL-REF (R,E1522001,T.Nomura+,J,NP/A,217,(2),253,1973) D602900500009 ERR-ANALYS (EN-ERR-DIG) Digitizing error D602900500010 (ERR-DIG) Digitizing error D602900500011 STATUS (CURVE)Fig4 D602900500012 (DEP,D6029003) D602900500013 (DEP,D6029004) D602900500014 ENDBIB 12 0 D602900500015 COMMON 2 3 D602900500016 EN-ERR-DIG ERR-DIG D602900500017 MEV PER-CENT D602900500018 0.06 0.2 D602900500019 ENDCOMMON 3 0 D602900500020 DATA 3 6 D602900500021 EN-CM DATA DATA-ERR D602900500022 MEV MB MB D602900500023 55.76 14.68 3.24 D602900500024 57.69 73.357 13.67 D602900500025 59.61 145.23 27.06 D602900500026 61.48 216.26 22.67 D602900500027 68.09 552.44 49.28 D602900500028 74.70 712.47 74.68 D602900500029 ENDDATA 8 0 D602900500030 ENDSUBENT 29 0 D602900599999 SUBENT D6029006 20091106 D070D602900600001 BIB 4 18 D602900600002 REACTION (82-PB-208(6-C-12,INL)82-PB-208,PAR,DA) fig5,6,7 D602900600003 DETECTOR (TELES,SIBAR,SIBAR)Three telescopes (DeltaE-E) of D602900600004 silicon surface barrier (SSB) detectors were set up D602900600005 inside a 1 m diameter scattering chamber for measuring D602900600006 the Projectile-like particles. A monitor (single SSB) D602900600007 detector was mounted at 20 deg with respect to beam D602900600008 direction for normalization. A second monitor at 25 degD602900600009 was mounted on the wall of the scattering chamber. D602900600010 The angular distributions were measured in the range D602900600011 20deg to 173 deg(lab). The angular resolution was aboutD602900600012 0.5 deg. The detector thicknesses were typically 20 to D602900600013 45 micro-metre for DeltaE and 300 to 2000 micro-metre D602900600014 for E detectors. Proper gain matching in DeltaE and E D602900600015 signals led to a total energy resolution of D602900600016 approx. 500 keV. D602900600017 ERR-ANALYS (ANG-ERR-D) Digitizing error D602900600018 (ERR-DIG) Digitizing error D602900600019 STATUS (CURVE)Fig5,6,7 D602900600020 ENDBIB 18 0 D602900600021 COMMON 3 3 D602900600022 E-LVL ANG-ERR-D ERR-DIG D602900600023 MEV ADEG MB/SR D602900600024 2.62 0.5 0.02 D602900600025 ENDCOMMON 3 0 D602900600026 DATA 4 29 D602900600027 EN ANG-CM DATA-CM DATA-ERR D602900600028 MEV ADEG MB/SR MB/SR D602900600029 62.9 63.5 2.05 0.84 D602900600030 62.9 83.9 2.39 0.62 D602900600031 62.9 103.6 3.17 0.54 D602900600032 62.9 113.6 1.48 0.28 D602900600033 62.9 123.5 2.00 0.28 D602900600034 62.9 133.2 2.63 0.37 D602900600035 62.9 142.7 2.02 0.28 D602900600036 64.9 73.8 5.97 0.72 D602900600037 64.9 78.8 6.11 0.87 D602900600038 64.9 83.9 4.25 0.60 D602900600039 64.9 100.9 2.13 0.28 D602900600040 64.9 108.8 3.78 0.38 D602900600041 64.9 113.6 4.16 0.42 D602900600042 64.9 118.6 3.35 0.32 D602900600043 64.9 133.2 2.07 0.23 D602900600044 64.9 137.9 1.43 0.17 D602900600045 64.9 147.5 0.99 0.13 D602900600046 64.9 152.3 0.89 0.14 D602900600047 64.9 161.6 0.69 0.11 D602900600048 84.9 48.0 10.9 1.09 D602900600049 84.9 58.4 5.98 0.73 D602900600050 84.9 60.9 5.57 0.66 D602900600051 84.9 66.1 5.65 0.62 D602900600052 84.9 71.2 3.53 0.48 D602900600053 84.9 73.8 2.67 0.32 D602900600054 84.9 76.3 2.3 0.36 D602900600055 84.9 83.9 0.95 0.16 D602900600056 84.9 88.9 0.36 0.09 D602900600057 84.9 98.9 0.17 0.05 D602900600058 ENDDATA 31 0 D602900600059 ENDSUBENT 58 0 D602900699999 SUBENT D6029007 20091106 D070D602900700001 BIB 5 19 D602900700002 REACTION (82-PB-208(6-C-12,6-C-13)82-PB-207,PAR,DA) D602900700003 DETECTOR (TELES,SIBAR,SIBAR)Three telescopes (DeltaE-E) of D602900700004 silicon surface barrier (SSB) detectors were set up D602900700005 inside a 1 m diameter scattering chamber for measuring D602900700006 the Projectile-like particles. A monitor (single SSB) D602900700007 detector was mounted at 20 deg with respect to beam D602900700008 direction for normalization. A second monitor at 25 degD602900700009 was mounted on the wall of the scattering chamber. D602900700010 The angular distributions were measured in the range D602900700011 20deg to 173 deg(lab). The angular resolution was aboutD602900700012 0.5 deg. The detector thicknesses were typically 20 to D602900700013 45 micro-metre for DeltaE and 300 to 2000 micro-metre D602900700014 for E detectors. Proper gain matching in DeltaE and E D602900700015 signals led to a total energy resolution of D602900700016 approx. 500 keV. D602900700017 ERR-ANALYS (ANG-ERR-D) Digitizing error D602900700018 (ERR-DIG) Digitizing error D602900700019 STATUS (CURVE)Fig5,6,7 D602900700020 EN-SEC (E-LVL,82-PB-207) D602900700021 ENDBIB 19 0 D602900700022 COMMON 2 3 D602900700023 ANG-ERR-D ERR-DIG D602900700024 ADEG MB/SR D602900700025 0.5 0.02 D602900700026 ENDCOMMON 3 0 D602900700027 DATA 6 60 D602900700028 E-LVL E-LVL EN ANG-CM DATA-CM DATA-ERR D602900700029 MEV MEV MEV ADEG MB/SR MB/SR D602900700030 0. 62.9 103.8 0.17 0.13D602900700031 0. 62.9 113.9 0.38 0.15D602900700032 0. 62.9 123.7 0.32 0.11D602900700033 0. 62.9 133.2 0.22 6.E-02D602900700034 0. 62.9 142.9 0.2 9.E-02D602900700035 0. 64.9 91.1 9.E-02 7.E-02D602900700036 0. 64.9 101.2 0.26 0.1D602900700037 0. 64.9 109.0 0.66 0.16D602900700038 0. 64.9 118.8 0.36 0.1D602900700039 0. 64.9 123.7 0.35 0.1D602900700040 0. 64.9 128.5 0.23 8.E-02D602900700041 0. 64.9 138.1 0.22 7.E-02D602900700042 0. 64.9 142.9 0.16 8.E-02D602900700043 0. 64.9 147.6 0.1 4.E-02D602900700044 0. 64.9 152.4 0.12 5.E-02D602900700045 0. 64.9 161.8 7.E-02 4.E-02D602900700046 0. 84.9 48.1 0.11 0.11D602900700047 0. 84.9 50.8 0.54 0.22D602900700048 0. 84.9 53.4 2.2 0.43D602900700049 0. 84.9 55.9 4.86 0.63D602900700050 0. 84.9 58.5 4.31 0.62D602900700051 0. 84.9 61.1 2.93 0.39D602900700052 0. 84.9 63.7 2.87 0.35D602900700053 0. 84.9 66.3 2. 0.37D602900700054 0. 84.9 71.4 1.22 0.28D602900700055 0. 84.9 73.9 1. 0.19D602900700056 0. 84.9 76.5 0.69 0.2D602900700057 0. 84.9 79.0 0.44 0.11D602900700058 0. 84.9 84.1 0.22 8.E-02D602900700059 0. 84.9 89.1 0.1 5.E-02D602900700060 0.59 0.9 62.9 103.8 0.8 0.26D602900700061 0.59 0.9 62.9 113.9 1.04 0.24D602900700062 0.59 0.9 62.9 123.8 0.84 0.18D602900700063 0.59 0.9 62.9 133.2 0.67 0.19D602900700064 0.59 0.9 62.9 142.9 0.79 0.18D602900700065 0.59 0.9 64.9 91.1 1.05 0.22D602900700066 0.59 0.9 64.9 101.2 1.65 0.25D602900700067 0.59 0.9 64.9 109.0 1.48 0.23D602900700068 0.59 0.9 64.9 118.8 1.21 0.19D602900700069 0.59 0.9 64.9 123.7 0.5 0.13D602900700070 0.59 0.9 64.9 128.5 0.58 0.13D602900700071 0.59 0.9 64.9 138.1 0.52 0.1D602900700072 0.59 0.9 64.9 142.9 0.31 9.E-02D602900700073 0.59 0.9 64.9 147.6 0.39 8.E-02D602900700074 0.59 0.9 64.9 152.4 0.33 8.E-02D602900700075 0.59 0.9 64.9 161.8 0.43 9.E-02D602900700076 0.59 0.9 84.9 48.1 0.76 8.E-02D602900700077 0.59 0.9 84.9 50.8 1.63 0.16D602900700078 0.59 0.9 84.9 53.4 4.49 0.45D602900700079 0.59 0.9 84.9 55.9 7. 0.7D602900700080 0.59 0.9 84.9 58.5 8.74 0.87D602900700081 0.59 0.9 84.9 61.1 9.75 0.98D602900700082 0.59 0.9 84.9 63.7 9.17 0.92D602900700083 0.59 0.9 84.9 66.3 6.27 0.63D602900700084 0.59 0.9 84.9 71.4 4.3 0.43D602900700085 0.59 0.9 84.9 73.9 3.33 0.33D602900700086 0.59 0.9 84.9 76.5 2.88 0.29D602900700087 0.59 0.9 84.9 79.0 2.16 0.22D602900700088 0.59 0.9 84.9 84.1 0.39 4.E-02D602900700089 0.59 0.9 84.9 89.1 0.29 3.E-02D602900700090 ENDDATA 62 0 D602900700091 ENDSUBENT 90 0 D602900799999 SUBENT D6029008 20091106 D070D602900800001 BIB 5 19 D602900800002 REACTION (82-PB-208(6-C-12,5-B-11)83-BI-209,PAR,DA) D602900800003 DETECTOR (TELES,SIBAR,SIBAR)Three telescopes (DeltaE-E) of D602900800004 silicon surface barrier (SSB) detectors were set up D602900800005 inside a 1 m diameter scattering chamber for measuring D602900800006 the Projectile-like particles. A monitor (single SSB) D602900800007 detector was mounted at 20 deg with respect to beam D602900800008 direction for normalization. A second monitor at 25 degD602900800009 was mounted on the wall of the scattering chamber. D602900800010 The angular distributions were measured in the range D602900800011 20deg to 173 deg(lab). The angular resolution was aboutD602900800012 0.5 deg. The detector thicknesses were typically 20 to D602900800013 45 micro-metre for DeltaE and 300 to 2000 micro-metre D602900800014 for E detectors. Proper gain matching in DeltaE and E D602900800015 signals led to a total energy resolution of D602900800016 approx. 500 keV. D602900800017 ERR-ANALYS (ANG-ERR-D) Digitizing error D602900800018 (ERR-DIG) Digitizing error D602900800019 STATUS (CURVE)Fig5,6,7 D602900800020 EN-SEC (E-LVL,83-BI-209) D602900800021 ENDBIB 19 0 D602900800022 COMMON 2 3 D602900800023 ANG-ERR-D ERR-DIG D602900800024 ADEG MB/SR D602900800025 0.5 0.02 D602900800026 ENDCOMMON 3 0 D602900800027 DATA 5 84 D602900800028 E-LVL EN ANG-CM DATA-CM DATA-ERR D602900800029 MEV MEV ADEG MB/SR MB/SR D602900800030 0. 62.9 104.1 8.E-02 8.E-02 D602900800031 0. 62.9 113.9 0.36 0.17 D602900800032 0. 62.9 123.7 0.38 0.11 D602900800033 0. 62.9 133.3 0.41 0.15 D602900800034 0. 62.9 142.9 0.64 0.15 D602900800035 0. 64.9 91.1 0.14 8.E-02 D602900800036 0. 64.9 101.2 0.52 0.14 D602900800037 0. 64.9 109.0 0.63 0.15 D602900800038 0. 64.9 118.8 0.73 0.15 D602900800039 0. 64.9 123.7 0.66 0.14 D602900800040 0. 64.9 128.5 0.57 0.13 D602900800041 0. 64.9 138.1 0.57 0.13 D602900800042 0. 64.9 142.9 0.35 7.E-02 D602900800043 0. 64.9 147.6 0.44 9.E-02 D602900800044 0. 64.9 152.4 0.37 9.E-02 D602900800045 0. 64.9 161.8 9.E-02 4.E-02 D602900800046 0. 84.9 48.1 0.41 0.22 D602900800047 0. 84.9 53.4 1.1 0.31 D602900800048 0. 84.9 55.9 1.54 0.35 D602900800049 0. 84.9 58.5 1.5 0.28 D602900800050 0. 84.9 61.1 1.87 0.39 D602900800051 0. 84.9 63.7 1.42 0.25 D602900800052 0. 84.9 66.3 0.82 0.21 D602900800053 0. 84.9 71.4 0.59 0.19 D602900800054 0. 84.9 73.9 0.48 0.13 D602900800055 0. 84.9 76.5 0.92 0.31 D602900800056 0. 84.9 79.0 0.12 6.E-02 D602900800057 0. 84.9 84.1 6.E-02 4.E-02 D602900800058 0. 84.9 89.1 2.E-02 2.E-02 D602900800059 0.9 62.9 104.1 0.32 0.16 D602900800060 0.9 62.9 113.9 0.4 0.12 D602900800061 0.9 62.9 123.7 0.54 0.16 D602900800062 0.9 62.9 133.3 0.57 0.17 D602900800063 0.9 62.9 142.9 0.67 0.17 D602900800064 0.9 64.9 91.1 0.18 9.E-02 D602900800065 0.9 64.9 91.1 0.14 8.E-02 D602900800066 0.9 64.9 101.1 0.49 0.14 D602900800067 0.9 64.9 109.0 0.63 0.15 D602900800068 0.9 64.9 118.8 0.7 0.15 D602900800069 0.9 64.9 123.7 0.53 0.13 D602900800070 0.9 64.9 138.1 0.46 9.E-02 D602900800071 0.9 64.9 142.9 0.42 8.E-02 D602900800072 0.9 64.9 147.6 0.52 0.1 D602900800073 0.9 64.9 152.4 0.41 9.E-02 D602900800074 0.9 64.9 161.8 0.35 8.E-02 D602900800075 0.9 84.9 48.1 1.06 0.34 D602900800076 0.9 84.9 53.4 1.7 0.38 D602900800077 0.9 84.9 55.9 3.32 0.52 D602900800078 0.9 84.9 58.5 2.9 0.51 D602900800079 0.9 84.9 61.1 3. 0.47 D602900800080 0.9 84.9 63.7 2.96 0.36 D602900800081 0.9 84.9 66.3 2.07 0.38 D602900800082 0.9 84.9 71.4 1.09 0.26 D602900800083 0.9 84.9 73.9 0.78 0.17 D602900800084 0.9 84.9 76.5 0.46 0.16 D602900800085 0.9 84.9 79.0 0.35 0.1 D602900800086 0.9 84.9 84.1 0.11 6.E-02 D602900800087 0.9 84.9 89.1 7.E-02 4.E-02 D602900800088 1.61 62.9 104.1 8.E-02 8.E-02 D602900800089 1.61 62.9 113.9 0.11 8.E-02 D602900800090 1.61 62.9 123.7 0.2 9.E-02 D602900800091 1.61 62.9 133.3 0.36 0.14 D602900800092 1.61 62.9 142.9 8.E-02 6.E-02 D602900800093 1.61 64.9 101.2 0.45 0.13 D602900800094 1.61 64.9 109.0 0.48 0.13 D602900800095 1.61 64.9 123.7 0.38 0.11 D602900800096 1.61 64.9 128.5 0.23 8.E-02 D602900800097 1.61 64.9 133.3 0.35 0.1 D602900800098 1.61 64.9 138.1 0.1 4.E-02 D602900800099 1.61 64.9 142.9 8.E-02 4.E-02 D602900800100 1.61 64.9 147.6 8.E-02 4.E-02 D602900800101 1.61 64.9 152.4 4.E-02 3.E-02 D602900800102 1.61 84.9 48.1 0.81 0.27 D602900800103 1.61 84.9 53.4 1.61 0.37 D602900800104 1.61 84.9 55.9 0.73 0.24 D602900800105 1.61 84.9 58.5 0.79 0.26 D602900800106 1.61 84.9 61.1 1.24 0.31 D602900800107 1.61 84.9 63.7 0.73 0.18 D602900800108 1.61 84.9 66.3 0.69 0.22 D602900800109 1.61 84.9 71.4 0.45 0.15 D602900800110 1.61 84.9 73.9 0.37 5.E-02 D602900800111 1.61 84.9 76.5 0.17 0.1 D602900800112 1.61 84.9 79.0 0.32 0.1 D602900800113 1.61 84.9 89.1 0.1 5.E-02 D602900800114 ENDDATA 86 0 D602900800115 ENDSUBENT 114 0 D602900899999 ENDENTRY 8 0 D602999999999