ENTRY C2174 20150826 C153C217400000001 SUBENT C2174001 20150826 C153C217400100001 BIB 10 22 C217400100002 TITLE Elastic and Inelastic Scattering of Protons from C217400100003 120Sn for Ep = 20.6, 25.2, 30.6 and 36.2 MeV: C217400100004 Tabulated Differential Cross Sections C217400100005 AUTHOR (F.E.Bertrand,T.A.Love,N.Baron,F.G.Perey,J.K.Dickens) C217400100006 REFERENCE (R,ORNL-4252,1968) C217400100007 INSTITUTE (1USAORL) C217400100008 FACILITY (CYCLO,1USAORL) Oak Ridge Isochronous Cyclotron. C217400100009 SAMPLE (50-SN-120,ENR=0.99) The 120Sn target was nominally C217400100010 4.5 mg/cm2 and >99% enriched. C217400100011 DETECTOR (GELI) A cooled Ge(Li) planer detector. C217400100012 PART-DET (P) C217400100013 METHOD (PHD) Protons scattered from the l20Sn target were C217400100014 detected using a Ge(Li) detector mounted so that the C217400100015 protons entered the side of the detector and were C217400100016 stopped in the depleted region. The total energy C217400100017 resolution (FWHM) was ~0.1% for each incident energy C217400100018 used. Pulses from the detector were amplified, C217400100019 converted to digital form, transferred to memory of a C217400100020 PDP-8 computer, and the resulting spectra were stored C217400100021 on magnetic tape. Peak areas were extracted using a C217400100022 peak-stripping routine written for a PDP-7 computer. C217400100023 HISTORY (20150826C) BP C217400100024 ENDBIB 22 0 C217400100025 NOCOMMON 0 0 C217400100026 ENDSUBENT 25 0 C217400199999 SUBENT C2174002 20150826 C153C217400200001 BIB 3 10 C217400200002 REACTION (50-SN-120(P,EL)50-SN-120,,DA) C217400200003 ERR-ANALYS (ERR-T) For elastic scattering the errors due to C217400200004 counting statistics were small, and the major C217400200005 contribution to delta sigma was the estimate of C217400200006 uncertainties associated with our knowledge of the C217400200007 variation of the target thickness in the region C217400200008 struck by the beam. C217400200009 (ERR-1,2.,4.) In the region struck by the beam, the C217400200010 variation in target thickness amounted to 3 +- 1%. C217400200011 STATUS (TABLE) Table 1 of R,ORNL-4252,1968. C217400200012 ENDBIB 10 0 C217400200013 COMMON 1 3 C217400200014 EN C217400200015 MEV C217400200016 20.6 C217400200017 ENDCOMMON 3 0 C217400200018 DATA 3 19 C217400200019 ANG-CM DATA-CM ERR-T C217400200020 ADEG MB/SR MB/SR C217400200021 15.100 22086.000 2686.000 C217400200022 20.200 6841.000 370.000 C217400200023 25.200 2916.000 150.000 C217400200024 30.200 1189.000 62.000 C217400200025 35.300 433.000 22.000 C217400200026 40.300 161.700 8.300 C217400200027 45.300 94.200 4.800 C217400200028 50.400 79.400 4.000 C217400200029 55.400 10.800 3.600 C217400200030 60.400 58.500 3.000 C217400200031 65.400 40.900 2.100 C217400200032 70.500 23.800 1.200 C217400200033 75.500 10.210 0.550 C217400200034 80.500 5.110 0.280 C217400200035 85.500 4.910 0.270 C217400200036 90.500 7.490 0.390 C217400200037 95.500 8.280 0.440 C217400200038 100.500 7.460 0.400 C217400200039 110.500 2.940 0.170 C217400200040 ENDDATA 21 0 C217400200041 ENDSUBENT 40 0 C217400299999 SUBENT C2174003 20150826 C153C217400300001 BIB 3 11 C217400300002 REACTION (50-SN-120(P,EL)50-SN-120,,DA) C217400300003 ERR-ANALYS (ERR-T) For elastic scattering the errors due to C217400300004 counting statistics were small, and the major C217400300005 contribution to delta sigma was the estimate of C217400300006 uncertainties associated with our knowledge of the C217400300007 variation of the target thickness in the region C217400300008 struck by the beam. In the region struck by the beam, C217400300009 the variation in target thickness amounted to 3 +- 1%. C217400300010 (ERR-1,2.,4.) In the region struck by the beam, the C217400300011 variation in target thickness amounted to 3 +- 1%. C217400300012 STATUS (TABLE) Table 1 of R,ORNL-4252,1968. C217400300013 ENDBIB 11 0 C217400300014 COMMON 1 3 C217400300015 EN C217400300016 MEV C217400300017 25.2 C217400300018 ENDCOMMON 3 0 C217400300019 DATA 3 20 C217400300020 ANG-CM DATA-CM ERR-T C217400300021 ADEG MB/SR MB/SR C217400300022 15.100 12598.000 868.000 C217400300023 20.200 4075.000 244.000 C217400300024 25.200 1593.000 94.000 C217400300025 30.200 621.000 31.000 C217400300026 35.300 255.000 13.000 C217400300027 40.300 108.500 5.500 C217400300028 45.300 46.700 2.400 C217400300029 50.400 34.300 1.800 C217400300030 55.400 41.000 2.100 C217400300031 60.400 41.900 2.100 C217400300032 65.400 27.000 1.400 C217400300033 70.500 10.890 0.560 C217400300034 75.500 2.940 0.170 C217400300035 80.500 3.370 0.120 C217400300036 85.500 6.890 0.360 C217400300037 90.500 8.000 0.410 C217400300038 95.500 5.920 0.320 C217400300039 100.500 3.120 0.170 C217400300040 105.500 1.138 0.078 C217400300041 110.500 0.730 0.046 C217400300042 ENDDATA 22 0 C217400300043 ENDSUBENT 42 0 C217400399999 SUBENT C2174004 20150826 C153C217400400001 BIB 3 11 C217400400002 REACTION (50-SN-120(P,EL)50-SN-120,,DA) C217400400003 ERR-ANALYS (ERR-T) For elastic scattering the errors due to C217400400004 counting statistics were small, and the major C217400400005 contribution to delta sigma was the estimate of C217400400006 uncertainties associated with our knowledge of the C217400400007 variation of the target thickness in the region C217400400008 struck by the beam. In the region struck by the beam, C217400400009 the variation in target thickness amounted to 3 +- 1%. C217400400010 (ERR-1,2.,4.) In the region struck by the beam, the C217400400011 variation in target thickness amounted to 3 +- 1%. C217400400012 STATUS (TABLE) Table 1 of R,ORNL-4252,1968. C217400400013 ENDBIB 11 0 C217400400014 COMMON 1 3 C217400400015 EN C217400400016 MEV C217400400017 30.6 C217400400018 ENDCOMMON 3 0 C217400400019 DATA 3 14 C217400400020 ANG-CM DATA-CM ERR-T C217400400021 ADEG MB/SR MB/SR C217400400022 15.100 7407.000 398.000 C217400400023 25.200 723.000 36.000 C217400400024 30.200 384.000 19.000 C217400400025 35.300 218.000 11.000 C217400400026 40.300 13.000 3.100 C217400400027 45.300 13.800 0.710 C217400400028 50.400 27.100 1.400 C217400400029 60.400 35.500 1.800 C217400400030 65.400 13.640 0.690 C217400400031 75.500 4.250 0.220 C217400400032 82.500 8.930 0.460 C217400400033 90.500 4.160 0.250 C217400400034 105.500 1.417 0.080 C217400400035 110.500 2.100 0.110 C217400400036 ENDDATA 16 0 C217400400037 ENDSUBENT 36 0 C217400499999 SUBENT C2174005 20150826 C153C217400500001 BIB 3 11 C217400500002 REACTION (50-SN-120(P,EL)50-SN-120,,DA) C217400500003 ERR-ANALYS (ERR-T) For elastic scattering the errors due to C217400500004 counting statistics were small, and the major C217400500005 contribution to delta sigma was the estimate of C217400500006 uncertainties associated with our knowledge of the C217400500007 variation of the target thickness in the region C217400500008 struck by the beam. In the region struck by the beam, C217400500009 the variation in target thickness amounted to 3 +- 1%. C217400500010 (ERR-1,2.,4.) In the region struck by the beam, the C217400500011 variation in target thickness amounted to 3 +- 1%. C217400500012 STATUS (TABLE) Table 1 of R,ORNL-4252,1968. C217400500013 ENDBIB 11 0 C217400500014 COMMON 1 3 C217400500015 EN C217400500016 MEV C217400500017 36.2 C217400500018 ENDCOMMON 3 0 C217400500019 DATA 3 23 C217400500020 ANG-CM DATA-CM ERR-T C217400500021 ADEG MB/SR MB/SR C217400500022 15.100 6511.000 353.000 C217400500023 20.200 1258.000 64.000 C217400500024 25.200 407.000 21.000 C217400500025 30.200 371.000 19.000 C217400500026 35.300 220.000 11.000 C217400500027 39.300 71.700 3.600 C217400500028 42.300 16.560 0.880 C217400500029 45.300 8.930 0.470 C217400500030 47.400 19.900 1.000 C217400500031 50.400 39.800 2.000 C217400500032 55.400 46.100 2.400 C217400500033 60.400 22.500 1.200 C217400500034 65.400 4.940 0.270 C217400500035 67.900 3.240 0.190 C217400500036 70.500 4.700 0.250 C217400500037 75.500 8.860 0.460 C217400500038 80.500 7.800 0.410 C217400500039 85.500 4.000 0.210 C217400500040 90.500 1.586 0.088 C217400500041 95.500 1.672 0.076 C217400500042 100.500 1.794 0.099 C217400500043 105.500 1.708 0.096 C217400500044 110.500 1.133 0.065 C217400500045 ENDDATA 25 0 C217400500046 ENDSUBENT 45 0 C217400599999 SUBENT C2174006 20150826 C153C217400600001 BIB 4 11 C217400600002 REACTION (50-SN-120(P,INL)50-SN-120,PAR,DA) C217400600003 ERR-ANALYS (ERR-T) For inelastic scattering, in addition to the C217400600004 target for nonuniformity, the major contributions to C217400600005 delta sigma include counting statistics and the C217400600006 estimation of the error associated with subtraction C217400600007 of the background. In the region struck by the beam, C217400600008 the variation in target thickness amounted to 3 +- 1%. C217400600009 (ERR-1,2.,4.) In the region struck by the beam, the C217400600010 variation in target thickness amounted to 3 +- 1%. C217400600011 LEVEL-PROP (50-SN-120,E-LVL=1.17,SPIN=2.,PARITY=+1.) C217400600012 STATUS (TABLE) Table 2 of R,ORNL-4252,1968. C217400600013 ENDBIB 11 0 C217400600014 COMMON 2 3 C217400600015 EN Q-VAL C217400600016 MEV MEV C217400600017 20.6 -1.17 C217400600018 ENDCOMMON 3 0 C217400600019 DATA 3 18 C217400600020 ANG-CM DATA-CM ERR-T C217400600021 ADEG MB/SR MB/SR C217400600022 20.200 4.780 0.690 C217400600023 25.200 5.220 0.520 C217400600024 30.200 5.010 0.500 C217400600025 35.300 3.070 0.300 C217400600026 40.300 1.920 0.190 C217400600027 45.400 1.010 0.100 C217400600028 50.400 1.210 0.120 C217400600029 55.400 1.230 0.120 C217400600030 60.400 1.530 0.150 C217400600031 65.400 1.410 0.140 C217400600032 70.500 0.932 0.093 C217400600033 75.500 0.599 0.059 C217400600034 80.500 0.392 0.039 C217400600035 85.500 0.311 0.033 C217400600036 90.500 0.371 0.037 C217400600037 95.500 0.370 0.039 C217400600038 100.500 0.312 0.034 C217400600039 110.500 0.300 0.032 C217400600040 ENDDATA 20 0 C217400600041 ENDSUBENT 40 0 C217400699999 SUBENT C2174007 20150826 C153C217400700001 BIB 4 11 C217400700002 REACTION (50-SN-120(P,INL)50-SN-120,PAR,DA) C217400700003 ERR-ANALYS (ERR-T) For inelastic scattering, in addition to the C217400700004 target for nonuniformity, the major contributions to C217400700005 delta sigma include counting statistics and the C217400700006 estimation of the error associated with subtraction C217400700007 of the background. In the region struck by the beam, C217400700008 the variation in target thickness amounted to 3 +- 1%. C217400700009 (ERR-1,2.,4.) In the region struck by the beam, the C217400700010 variation in target thickness amounted to 3 +- 1%. C217400700011 LEVEL-PROP (50-SN-120,E-LVL=1.17,SPIN=2.,PARITY=+1.) C217400700012 STATUS (TABLE) Table 2 of R,ORNL-4252,1968. C217400700013 ENDBIB 11 0 C217400700014 COMMON 2 3 C217400700015 EN Q-VAL C217400700016 MEV MEV C217400700017 25.2 -1.17 C217400700018 ENDCOMMON 3 0 C217400700019 DATA 3 16 C217400700020 ANG-CM DATA-CM ERR-T C217400700021 ADEG MB/SR MB/SR C217400700022 20.200 5.860 0.820 C217400700023 25.200 6.500 0.820 C217400700024 30.200 5.380 0.400 C217400700025 35.300 2.700 0.200 C217400700026 40.300 1.500 0.110 C217400700027 45.300 1.046 0.078 C217400700028 50.400 1.319 0.098 C217400700029 55.400 1.480 0.110 C217400700030 60.400 1.125 0.064 C217400700031 65.400 0.804 0.064 C217400700032 70.500 0.687 0.051 C217400700033 75.500 0.555 0.050 C217400700034 80.500 0.405 0.043 C217400700035 100.500 0.293 0.030 C217400700036 105.500 0.336 0.034 C217400700037 110.500 0.304 0.026 C217400700038 ENDDATA 18 0 C217400700039 ENDSUBENT 38 0 C217400799999 SUBENT C2174008 20150826 C153C217400800001 BIB 4 11 C217400800002 REACTION (50-SN-120(P,INL)50-SN-120,PAR,DA) C217400800003 ERR-ANALYS (ERR-T) For inelastic scattering, in addition to the C217400800004 target for nonuniformity, the major contributions to C217400800005 delta sigma include counting statistics and the C217400800006 estimation of the error associated with subtraction C217400800007 of the background. In the region struck by the beam, C217400800008 the variation in target thickness amounted to 3 +- 1%. C217400800009 (ERR-1,2.,4.) In the region struck by the beam, the C217400800010 variation in target thickness amounted to 3 +- 1%. C217400800011 LEVEL-PROP (50-SN-120,E-LVL=1.17,SPIN=2.,PARITY=+1.) C217400800012 STATUS (TABLE) Table 2 of R,ORNL-4252,1968. C217400800013 ENDBIB 11 0 C217400800014 COMMON 2 3 C217400800015 EN Q-VAL C217400800016 MEV MEV C217400800017 30.6 -1.17 C217400800018 ENDCOMMON 3 0 C217400800019 DATA 3 14 C217400800020 ANG-CM DATA-CM ERR-T C217400800021 ADEG MB/SR MB/SR C217400800022 15.100 5.540 0.550 C217400800023 25.200 6.670 0.660 C217400800024 30.200 4.310 0.430 C217400800025 35.300 2.440 0.240 C217400800026 40.300 1.590 0.150 C217400800027 45.300 1.600 0.150 C217400800028 50.400 1.470 0.140 C217400800029 60.400 0.700 0.070 C217400800030 65.400 0.840 0.083 C217400800031 75.500 0.576 0.057 C217400800032 82.500 0.276 0.027 C217400800033 90.500 0.336 0.033 C217400800034 105.500 0.196 0.019 C217400800035 110.500 0.148 0.014 C217400800036 ENDDATA 16 0 C217400800037 ENDSUBENT 36 0 C217400899999 SUBENT C2174009 20150826 C153C217400900001 BIB 4 11 C217400900002 REACTION (50-SN-120(P,INL)50-SN-120,PAR,DA) C217400900003 ERR-ANALYS (ERR-T) For inelastic scattering, in addition to the C217400900004 target for nonuniformity, the major contributions to C217400900005 delta sigma include counting statistics and the C217400900006 estimation of the error associated with subtraction C217400900007 of the background. In the region struck by the beam, C217400900008 the variation in target thickness amounted to 3 +- 1%. C217400900009 (ERR-1,2.,4.) In the region struck by the beam, the C217400900010 variation in target thickness amounted to 3 +- 1%. C217400900011 LEVEL-PROP (50-SN-120,E-LVL=1.17,SPIN=2.,PARITY=+1.) C217400900012 STATUS (TABLE) Table 2 of R,ORNL-4252,1968. C217400900013 ENDBIB 11 0 C217400900014 COMMON 2 3 C217400900015 EN Q-VAL C217400900016 MEV MEV C217400900017 36.2 -1.17 C217400900018 ENDCOMMON 3 0 C217400900019 DATA 3 23 C217400900020 ANG-CM DATA-CM ERR-T C217400900021 ADEG MB/SR MB/SR C217400900022 15.100 5.500 0.520 C217400900023 20.200 6.970 0.520 C217400900024 25.200 6.720 0.500 C217400900025 30.200 3.440 0.250 C217400900026 35.300 2.040 0.150 C217400900027 39.300 2.370 0.170 C217400900028 42.300 2.360 0.170 C217400900029 45.300 1.970 0.140 C217400900030 47.400 1.700 0.120 C217400900031 50.400 1.101 0.082 C217400900032 55.400 0.701 0.058 C217400900033 60.400 0.776 0.072 C217400900034 65.400 0.956 0.071 C217400900035 68.000 0.897 0.070 C217400900036 70.500 0.690 0.051 C217400900037 75.500 0.365 0.030 C217400900038 80.500 0.269 0.030 C217400900039 85.500 0.299 0.024 C217400900040 90.500 0.390 0.029 C217400900041 95.500 0.263 0.019 C217400900042 100.500 0.155 0.014 C217400900043 105.500 0.104 0.012 C217400900044 110.500 0.105 0.011 C217400900045 ENDDATA 25 0 C217400900046 ENDSUBENT 45 0 C217400999999 SUBENT C2174010 20150826 C153C217401000001 BIB 4 21 C217401000002 REACTION (50-SN-120(P,INL)50-SN-120,PAR,DA) C217401000003 ERR-ANALYS (ERR-T) For inelastic scattering, in addition to the C217401000004 target for nonuniformity, the major contributions to C217401000005 delta sigma include counting statistics and the C217401000006 estimation of the error associated with subtraction C217401000007 of the background. In the region struck by the beam, C217401000008 the variation in target thickness amounted to 3 +-1%. C217401000009 An additional uncertainty for the Ex = 2.35-MeV C217401000010 data was associated with the unknown contributions of C217401000011 partially resolved proton groups corresponding to C217401000012 excitation of levels in 120Sn with Ex between 2.3 and C217401000013 2.4 MeV. We assumed that the reaction of interest C217401000014 dominated the resulting peak seen in the pulse-height C217401000015 spectrum. Analysis of the data using this assumption C217401000016 indicated that the contribution from the unresolved C217401000017 levels was <30%. The largest uncertainties occur at C217401000018 the minima of the angular distributions. C217401000019 (ERR-1,2.,4.) Target Thickness. C217401000020 (ERR-2,,30.) Unresolved levels. C217401000021 LEVEL-PROP (50-SN-120,E-LVL=2.35,SPIN=3.,PARITY=-1.) C217401000022 STATUS (TABLE) Table 3 of R,ORNL-4252,1968. C217401000023 ENDBIB 21 0 C217401000024 COMMON 2 3 C217401000025 EN Q-VAL C217401000026 MEV MEV C217401000027 20.6 -2.35 C217401000028 ENDCOMMON 3 0 C217401000029 DATA 3 18 C217401000030 ANG-CM DATA-CM ERR-T C217401000031 ADEG MB/SR MB/SR C217401000032 20.200 1.620 0.290 C217401000033 25.200 1.630 0.240 C217401000034 30.600 2.560 0.380 C217401000035 35.300 3.110 0.460 C217401000036 40.300 2.820 0.420 C217401000037 45.400 2.200 0.320 C217401000038 50.400 1.620 0.240 C217401000039 55.400 1.100 0.160 C217401000040 60.400 0.920 0.130 C217401000041 65.500 1.120 0.160 C217401000042 70.500 1.190 0.170 C217401000043 75.500 1.370 0.200 C217401000044 80.500 1.020 0.150 C217401000045 85.500 0.890 0.130 C217401000046 90.500 0.680 0.100 C217401000047 95.500 0.418 0.062 C217401000048 100.500 0.327 0.049 C217401000049 110.500 0.325 0.048 C217401000050 ENDDATA 20 0 C217401000051 ENDSUBENT 50 0 C217401099999 SUBENT C2174011 20150826 C153C217401100001 BIB 4 21 C217401100002 REACTION (50-SN-120(P,INL)50-SN-120,PAR,DA) C217401100003 ERR-ANALYS (ERR-T) For inelastic scattering, in addition to the C217401100004 target for nonuniformity, the major contributions to C217401100005 delta sigma include counting statistics and the C217401100006 estimation of the error associated with subtraction C217401100007 of the background. In the region struck by the beam, C217401100008 the variation in target thickness amounted to 3 +-1%. C217401100009 An additional uncertainty for the Ex = 2.35-MeV C217401100010 data was associated with the unknown contributions of C217401100011 partially resolved proton groups corresponding to C217401100012 excitation of levels in 120Sn with Ex between 2.3 and C217401100013 2.4 MeV. We assumed that the reaction of interest C217401100014 dominated the resulting peak seen in the pulse-height C217401100015 spectrum. Analysis of the data using this assumption C217401100016 indicated that the contribution from the unresolved C217401100017 levels was <30%. The largest uncertainties occur at C217401100018 the minima of the angular distributions. C217401100019 (ERR-1,2.,4.) Target Thickness. C217401100020 (ERR-2,,30.) Unresolved levels. C217401100021 LEVEL-PROP (50-SN-120,E-LVL=2.35,SPIN=3.,PARITY=-1.) C217401100022 STATUS (TABLE) Table 3 of R,ORNL-4252,1968. C217401100023 ENDBIB 21 0 C217401100024 COMMON 2 3 C217401100025 EN Q-VAL C217401100026 MEV MEV C217401100027 25.2 -2.35 C217401100028 ENDCOMMON 3 0 C217401100029 DATA 3 17 C217401100030 ANG-CM DATA-CM ERR-T C217401100031 ADEG MB/SR MB/SR C217401100032 30.300 2.960 0.440 C217401100033 35.300 6.250 0.480 C217401100034 40.300 3.050 0.450 C217401100035 45.400 2.130 0.310 C217401100036 50.400 1.580 0.230 C217401100037 55.400 1.050 0.150 C217401100038 60.400 0.910 0.130 C217401100039 65.500 1.040 0.150 C217401100040 70.500 1.100 0.160 C217401100041 75.500 0.990 0.140 C217401100042 80.500 0.700 0.100 C217401100043 85.500 0.528 0.079 C217401100044 90.500 0.396 0.059 C217401100045 95.500 0.339 0.050 C217401100046 100.500 0.293 0.043 C217401100047 105.500 0.300 0.045 C217401100048 110.500 0.270 0.040 C217401100049 ENDDATA 19 0 C217401100050 ENDSUBENT 49 0 C217401199999 SUBENT C2174012 20150826 C153C217401200001 BIB 4 21 C217401200002 REACTION (50-SN-120(P,INL)50-SN-120,PAR,DA) C217401200003 ERR-ANALYS (ERR-T) For inelastic scattering, in addition to the C217401200004 target for nonuniformity, the major contributions to C217401200005 delta sigma include counting statistics and the C217401200006 estimation of the error associated with subtraction C217401200007 of the background. In the region struck by the beam, C217401200008 the variation in target thickness amounted to 3 +-1%. C217401200009 An additional uncertainty for the Ex = 2.35-MeV C217401200010 data was associated with the unknown contributions of C217401200011 partially resolved proton groups corresponding to C217401200012 excitation of levels in 120Sn with Ex between 2.3 and C217401200013 2.4 MeV. We assumed that the reaction of interest C217401200014 dominated the resulting peak seen in the pulse-height C217401200015 spectrum. Analysis of the data using this assumption C217401200016 indicated that the contribution from the unresolved C217401200017 levels was <30%. The largest uncertainties occur at C217401200018 the minima of the angular distributions. C217401200019 (ERR-1,2.,4.) Target Thickness. C217401200020 (ERR-2,,30.) Unresolved levels. C217401200021 LEVEL-PROP (50-SN-120,E-LVL=2.35,SPIN=3.,PARITY=-1.) C217401200022 STATUS (TABLE) Table 3 of R,ORNL-4252,1968. C217401200023 ENDBIB 21 0 C217401200024 COMMON 2 3 C217401200025 EN Q-VAL C217401200026 MEV MEV C217401200027 36.2 -2.35 C217401200028 ENDCOMMON 3 0 C217401200029 DATA 3 23 C217401200030 ANG-CM DATA-CM ERR-T C217401200031 ADEG MB/SR MB/SR C217401200032 15.100 5.370 0.800 C217401200033 20.200 5.760 0.860 C217401200034 25.200 6.060 0.900 C217401200035 30.200 5.830 0.870 C217401200036 35.300 5.080 0.760 C217401200037 39.300 3.890 0.560 C217401200038 42.300 3.260 0.480 C217401200039 45.400 2.890 0.430 C217401200040 47.400 2.570 0.380 C217401200041 50.400 2.510 0.370 C217401200042 55.400 2.000 0.300 C217401200043 60.400 1.240 0.180 C217401200044 65.500 1.200 0.180 C217401200045 68.000 1.120 0.160 C217401200046 70.500 1.170 0.170 C217401200047 75.500 0.720 0.100 C217401200048 80.500 0.560 0.083 C217401200049 85.500 0.381 0.057 C217401200050 90.500 0.395 0.059 C217401200051 95.500 0.319 0.047 C217401200052 100.500 0.293 0.043 C217401200053 105.500 0.199 0.029 C217401200054 110.500 0.167 0.025 C217401200055 ENDDATA 25 0 C217401200056 ENDSUBENT 55 0 C217401299999 ENDENTRY 12 0 C217499999999