ENTRY 41684 20210608 41954168400000001 SUBENT 41684001 20210608 41954168400100001 BIB 12 78 4168400100002 TITLE Investigation of Inelastic Neutron Scattering on 4168400100003 27Al Nuclei 4168400100004 AUTHOR (N.A.Fedorov,T.Yu.Tretyakova,V.M.Bystritsky, 4168400100005 Yu.N.Kopach,I.N.Ruskov,V.R.Skoy,D.N.Grozdanov, 4168400100006 N.I.Zamyatin,W.Dongming,F.A.Aliev,K.Hramco,A.Kumar, 4168400100007 A.Gandhi,S.Dabylova,D.I.Yurkov,Yu.N.Barmakov) 4168400100008 INSTITUTE (4ZZZDUB) N.A.Fedorov,T.Yu.Tretyakova,V.M.Bystritsky, 4168400100009 Yu.N.Kopach,I.N.Ruskov,V.R.Skoy,D.N.Grozdanov, 4168400100010 N.I.Zamyatin,W.Dongming,F.A.Aliev,K.Hramco,S.Dabylova 4168400100011 (4RUSMOS) N.A.Fedorov, T.Yu.Tretyakova 4168400100012 (3BULBLA) I.N.Ruskov,D.N.Grozdanov 4168400100013 (3CPRCPR) Xian Jiao Tong University, Xian, China 4168400100014 W.Dongming 4168400100015 (4AZRAZR) Inst.of Geology and Geophysics of Azerbaijan 4168400100016 National Academy of Sciences, Baku, Azerbaijan 4168400100017 F.A.Aliev 4168400100018 (4MLDMLD) Inst. of Chemistry of the Academy of Sciences4168400100019 of Moldova, Chisinau, Republic of Moldova 4168400100020 K.Hramco 4168400100021 (3INDBHU) A.Kumar,A.Gandhi 4168400100022 (4RUSRUS) All-Russia Research Institute of Automatics 4168400100023 (VNIIA), Moscow, 127055, Russia. 4168400100024 D.I.Yurkov,Yu.N.Barmakov 4168400100025 REFERENCE (J,PAN,82,343,2019) 4168400100026 #doi:10.1134/s1063778819040094 4168400100027 Engl.translation of: 4168400100028 (J,YF,82,297,2019) Issue 4. 4168400100029 #doi:10.1134/S0044002719040093 4168400100030 FACILITY (NGEN,4ZZZDUB) TANGRA setup on the basis of ING-27 4168400100031 neutron generator. 4168400100032 INC-SOURCE (D-T) Deuterons up to 80-100 keV on tritium target. 4168400100033 INC-SPECT Maximum intensity of the neutron flux in 4PI geometry 4168400100034 5.E+7 n/sec . 4168400100035 SAMPLE Distance neutron source - sample 169 mm. 4168400100036 4 cm x 4 cm x 14 cm size. 4168400100037 METHOD (COINC,TOF) Alpha-gamma coincidence. Neutron-gamma 4168400100038 separation by time-of-flight. 4168400100039 DETECTOR (SI) 64-pixel silicon alpha detector, pixel size 4168400100040 6x6 mm2, located at 100 mm distance from the tritium 4168400100041 target . For detection of 3.5 MeV alphas from 4168400100042 d+t -> n+alpha reaction. 4168400100043 (BGO) 18 scintillation detectors based on BGO crystals 4168400100044 of 76 mm diameter, 65 mm thickness; arranged in 4168400100045 horizontal plane along a circle of 750 mm radius with 4168400100046 a step of 14 degrees of angle. For gamma detection. 4168400100047 Energy resolution of BGO gamma-detectors ~10.4% at 4168400100048 Egamma=662 keV. 4168400100049 Similar measurement was done by HPGe-detectors of 4168400100050 ~3.4% energy resolution for Egamma=662 keV. 4168400100051 ADD-RES . Table 1 of J. Phys.At.Nucl.,82,343,2019 4168400100052 measured gamma-transitions with initial and final 4168400100053 levels energy,spin,parity; all energies in keV: 4168400100054 Egamma Reaction E-LVL-ini E-LVL-fin 4168400100055 472. Al-27(n,a)Na-24 472.(1+) 0.(4+) 4168400100056 792. Al-27(n,n')Al-27 3004.(9/2+) 2211.(7/2+) 4168400100057 844. Al-27(n,n')Al-27 844.(1/2+) 0.(5/2+) 4168400100058 874. Al-27(n,a)Na-24 1346.(1+) 472.(1+) 4168400100059 985. Al-27(n,p)Mg-27 985.(3/2+) 0.(1/2+) 4168400100060 1014. Al-27(n,n')Al-27 1014.(3/2+) 0.(5/2+) 4168400100061 1506. Al-27(n,n')Al-27 4510.(11/2+) )) 3004.(9/2+) 4168400100062 1698. Al-27(n,p)Mg-27 1698.(5/2+) 0.(1/2+) 4168400100063 1720. Al-27(n,n')Al-27 2735.(5/2+) 1014.(3/2+) 4168400100064 1809. Al-27(n,d)Mg-26 1809.(2+) 0.(0+) 4168400100065 1940. Al-27(n,p)Mg-27 1940.(5/2+) 0.(1/2+) 4168400100066 2063. Al-27(n,p)Mg-27 3761.(5/2-,7/2-) 1699.(5/2+) 4168400100067 2211. Al-27(n,n')Al-27 2211.(7/2+) 0.(1/2+) 4168400100068 2298. Al-27(n,n')Al-27 4510.(11/2+) 2211.(7/2+) 4168400100069 2506. Al-27(n,p)Mg-27 3491.(3/2+,5/2+) 985.(3/2+) 4168400100070 3004. Al-27(n,n')Al-27 3004.(9/2+) 0.(1/2+) 4168400100071 3203. Al-27(n,n')Al-27 4054.(1/2-) 844.(1/2+) 4168400100072 4580. Al-27(n,n')Al-27 4580.(7/2+) 0.(5/2+) 4168400100073 . Model calculation of Legendre coefficients - see 4168400100074 Table 2 of J.Phys.At.Nucl.,v.82,p.343,2019 4168400100075 HISTORY (20200609C) M.M. 4168400100076 Request for the data of Fig.4a-e was sent 09 Jun.2020 4168400100077 to A.N.Fedorov. 4168400100078 (20200619R) Data were received from N.A.Fedorov 4168400100079 (20210608A) Subents 002,003 were corrected 4168400100080 ENDBIB 78 0 4168400100081 COMMON 1 3 4168400100082 EN 4168400100083 MEV 4168400100084 14.1 4168400100085 ENDCOMMON 3 0 4168400100086 ENDSUBENT 85 0 4168400199999 SUBENT 41684002 20210608 41954168400200001 BIB 4 8 4168400200002 REACTION (13-AL-27(N,INL)13-AL-27,PAR,DA,G,LEG/RS) 4168400200003 ERR-ANALYS (DATA-ERR) Type of uncertainty is not explained in the 4168400200004 article. 4168400200005 STATUS (TABLE) Table 2 of J.Phys.At.Nucl.,v.82,p.343,2019 4168400200006 HISTORY (20210608A) SF8: LEG/RSD -> LEG/RS 4168400200007 Formula used to derive Legendre coefficients 4168400200008 W(THETA)=1+a2*P2(cos(THETA))+a4*P4(cos(THETA)) 4168400200009 was deleted according to comment of N.Otsuka (NDS,IAEA)4168400200010 ENDBIB 8 0 4168400200011 NOCOMMON 0 0 4168400200012 DATA 4 7 4168400200013 E NUMBER DATA DATA-ERR 4168400200014 KEV NO-DIM NO-DIM NO-DIM 4168400200015 845. 2. 0.015 0.2 4168400200016 845. 4. 0.05 0.2 4168400200017 1015. 2. 0.06 0.03 4168400200018 2215. 2. 0.14 0.02 4168400200019 2215. 4. 0.02 0.03 4168400200020 3005. 2. 0.11 0.03 4168400200021 3005. 4. -0.09 0.04 4168400200022 ENDDATA 9 0 4168400200023 ENDSUBENT 22 0 4168400299999 SUBENT 41684003 20210608 41954168400300001 BIB 4 8 4168400300002 REACTION (13-AL-27(N,X)12-MG-26,PAR,DA,G,LEG/RS) 4168400300003 ERR-ANALYS (DATA-ERR) Type of uncertainty is not explained in the 4168400300004 article. 4168400300005 STATUS (TABLE) Table 2 of J.Phys.At.Nucl.,v.82,p.343,2019 4168400300006 HISTORY (20210608A) SF8: LEG/RSD -> LEG/RS 4168400300007 Formula used to derive Legendre coefficients 4168400300008 W(THETA)=1+a2*P2(cos(THETA))+a4*P4(cos(THETA)) 4168400300009 was deleted according to comment of N.Otsuka (NDS,IAEA)4168400300010 ENDBIB 8 0 4168400300011 NOCOMMON 0 0 4168400300012 DATA 4 2 4168400300013 E NUMBER DATA DATA-ERR 4168400300014 KEV NO-DIM NO-DIM NO-DIM 4168400300015 1805. 2. 0.09 0.03 4168400300016 1805. 4. 0.02 0.03 4168400300017 ENDDATA 4 0 4168400300018 ENDSUBENT 17 0 4168400399999 SUBENT 41684004 20200609 41884168400400001 BIB 5 11 4168400400002 REACTION (13-AL-27(N,INL)13-AL-27,PAR,DA,G,REL) 4168400400003 See ANALYSIS for REL explanation. 4168400400004 ANALYSIS Angular distribution was defined as number of counts 4168400400005 at specified angle to number of counts average for all 4168400400006 angles. 4168400400007 FLAG (1.) Measurement by symmetrically placed detectors. 4168400400008 (2.) Measurement by symmetrically placed detectors. 4168400400009 ERR-ANALYS (ERR-S) Statistical uncertainty (information from the 4168400400010 author) 4168400400011 STATUS (TABLE) From author. 4168400400012 Fig.6 a,b,d,e of J.Phys.At.Nucl.,v.82,p.343,2019 4168400400013 ENDBIB 11 0 4168400400014 NOCOMMON 0 0 4168400400015 DATA 5 216 4168400400016 E COS DATA ERR-S FLAG 4168400400017 KEV NO-DIM ARB-UNITS ARB-UNITS NO-DIM 4168400400018 845. -0.64 1.44 0.38 4168400400019 845. -0.61 1.42 0.18 4168400400020 845. -0.60 0.92 0.23 4168400400021 845. -0.56 1.19 0.22 1. 4168400400022 845. -0.56 1.02 0.25 2. 4168400400023 845. -0.51 1.17 0.26 4168400400024 845. -0.45 1.07 0.25 4168400400025 845. -0.39 1.11 0.19 1. 4168400400026 845. -0.39 1.03 0.25 2. 4168400400027 845. -0.35 0.97 0.17 4168400400028 845. -0.34 1.18 0.17 4168400400029 845. -0.30 0.88 0.14 4168400400030 845. -0.23 1.54 0.21 4168400400031 845. -0.17 1.10 0.28 4168400400032 845. -0.16 1.19 0.23 4168400400033 845. -0.11 1.23 0.14 1. 4168400400034 845. -0.11 1.17 0.25 2. 4168400400035 845. -0.05 0.96 0.16 4168400400036 845. 0.00 1.12 0.25 4168400400037 845. 0.06 1.08 0.16 4168400400038 845. 0.07 1.30 0.18 4168400400039 845. 0.13 1.06 0.17 4168400400040 845. 0.14 1.11 0.15 4168400400041 845. 0.20 0.85 0.15 4168400400042 845. 0.24 1.00 0.29 4168400400043 845. 0.30 1.17 0.14 1. 4168400400044 845. 0.30 0.40 0.09 2. 4168400400045 845. 0.35 1.17 0.16 4168400400046 845. 0.37 1.17 0.14 4168400400047 845. 0.43 1.15 0.16 4168400400048 845. 0.45 0.84 0.19 4168400400049 845. 0.52 0.52 0.12 4168400400050 845. 0.53 1.33 0.17 4168400400051 845. 0.58 0.96 0.14 1. 4168400400052 845. 0.58 0.94 0.11 2. 4168400400053 845. 0.63 0.97 0.15 4168400400054 845. 0.65 1.24 0.24 4168400400055 845. 0.70 1.06 0.14 1. 4168400400056 845. 0.70 0.68 0.18 2. 4168400400057 845. 0.75 0.91 0.19 1. 4168400400058 845. 0.75 1.20 0.21 2. 4168400400059 845. 0.80 1.20 0.19 4168400400060 845. 0.81 0.97 0.18 4168400400061 845. 0.85 1.03 0.13 1. 4168400400062 845. 0.85 1.11 0.21 2. 4168400400063 845. 0.88 0.92 0.22 1. 4168400400064 845. 0.88 1.29 0.18 2. 4168400400065 845. 0.91 0.88 0.17 4168400400066 845. 0.93 1.06 0.22 4168400400067 845. 0.94 1.02 0.15 1. 4168400400068 845. 0.94 1.22 0.18 2. 4168400400069 845. 0.96 1.02 0.15 4168400400070 845. 0.97 0.97 0.11 4168400400071 845. 0.98 0.72 0.23 4168400400072 1015. -0.65 1.13 0.18 4168400400073 1015. -0.61 1.14 0.11 4168400400074 1015. -0.60 0.83 0.14 4168400400075 1015. -0.56 0.98 0.12 1. 4168400400076 1015. -0.56 1.12 0.13 2. 4168400400077 1015. -0.52 1.23 0.15 4168400400078 1015. -0.45 0.95 0.14 4168400400079 1015. -0.39 1.07 0.11 1. 4168400400080 1015. -0.39 0.85 0.14 2. 4168400400081 1015. -0.35 1.03 0.10 1. 4168400400082 1015. -0.35 0.89 0.09 2. 4168400400083 1015. -0.29 0.90 0.10 4168400400084 1015. -0.24 1.17 0.14 4168400400085 1015. -0.18 0.96 0.14 4168400400086 1015. -0.16 1.06 0.11 4168400400087 1015. -0.11 1.04 0.12 4168400400088 1015. -0.10 0.82 0.07 4168400400089 1015. -0.06 0.92 0.10 4168400400090 1015. 0.00 0.99 0.15 4168400400091 1015. 0.06 0.97 0.11 4168400400092 1015. 0.07 0.89 0.08 4168400400093 1015. 0.13 0.83 0.10 1. 4168400400094 1015. 0.13 1.19 0.09 2. 4168400400095 1015. 0.20 0.87 0.10 4168400400096 1015. 0.24 0.81 0.13 4168400400097 1015. 0.30 0.78 0.09 4168400400098 1015. 0.31 1.31 0.10 4168400400099 1015. 0.36 1.14 0.10 4168400400100 1015. 0.38 0.99 0.09 4168400400101 1015. 0.43 1.23 0.14 4168400400102 1015. 0.45 1.35 0.20 4168400400103 1015. 0.52 0.93 0.09 1. 4168400400104 1015. 0.52 1.10 0.11 2. 4168400400105 1015. 0.58 0.84 0.07 1. 4168400400106 1015. 0.58 1.21 0.10 2. 4168400400107 1015. 0.64 0.99 0.11 4168400400108 1015. 0.65 1.14 0.17 4168400400109 1015. 0.70 1.08 0.07 1. 4168400400110 1015. 0.70 0.92 0.12 2. 4168400400111 1015. 0.75 0.96 0.11 4168400400112 1015. 0.76 1.15 0.11 4168400400113 1015. 0.80 0.98 0.12 4168400400114 1015. 0.81 0.98 0.12 4168400400115 1015. 0.85 1.07 0.09 1. 4168400400116 1015. 0.85 0.79 0.09 2. 4168400400117 1015. 0.88 0.97 0.11 1. 4168400400118 1015. 0.88 1.10 0.09 2. 4168400400119 1015. 0.91 1.03 0.10 4168400400120 1015. 0.92 0.81 0.14 4168400400121 1015. 0.95 1.06 0.09 1. 4168400400122 1015. 0.95 1.02 0.11 2. 4168400400123 1015. 0.96 1.13 0.06 1. 4168400400124 1015. 0.96 1.18 0.09 2. 4168400400125 1015. 0.98 0.71 0.12 4168400400126 2215. -0.65 1.07 0.14 4168400400127 2215. -0.61 1.08 0.09 4168400400128 2215. -0.60 0.86 0.08 4168400400129 2215. -0.56 0.95 0.05 1. 4168400400130 2215. -0.56 1.02 0.08 2. 4168400400131 2215. -0.51 1.01 0.08 4168400400132 2215. -0.46 0.88 0.15 4168400400133 2215. -0.39 0.95 0.07 1. 4168400400134 2215. -0.39 0.91 0.07 2. 4168400400135 2215. -0.35 0.90 0.07 1. 4168400400136 2215. -0.35 0.99 0.11 2. 4168400400137 2215. -0.29 0.99 0.06 4168400400138 2215. -0.23 0.98 0.11 4168400400139 2215. -0.18 0.87 0.09 1. 4168400400140 2215. -0.18 1.07 0.11 2. 4168400400141 2215. -0.12 0.88 0.07 4168400400142 2215. -0.11 0.86 0.09 4168400400143 2215. -0.06 0.88 0.10 4168400400144 2215. 0.00 1.01 0.10 4168400400145 2215. 0.07 1.10 0.11 4168400400146 2215. 0.08 0.97 0.11 4168400400147 2215. 0.13 0.92 0.10 1. 4168400400148 2215. 0.13 0.90 0.09 2. 4168400400149 2215. 0.20 0.91 0.09 4168400400150 2215. 0.23 1.03 0.11 4168400400151 2215. 0.30 1.04 0.06 4168400400152 2215. 0.31 0.95 0.12 4168400400153 2215. 0.36 1.03 0.08 4168400400154 2215. 0.37 0.97 0.08 4168400400155 2215. 0.43 1.00 0.07 4168400400156 2215. 0.45 0.87 0.09 4168400400157 2215. 0.52 0.86 0.07 1. 4168400400158 2215. 0.52 0.91 0.09 2. 4168400400159 2215. 0.57 0.94 0.12 4168400400160 2215. 0.58 0.95 0.05 4168400400161 2215. 0.63 1.09 0.09 4168400400162 2215. 0.65 1.03 0.12 4168400400163 2215. 0.70 1.05 0.06 4168400400164 2215. 0.71 1.05 0.11 4168400400165 2215. 0.76 1.15 0.10 1. 4168400400166 2215. 0.76 1.12 0.12 2. 4168400400167 2215. 0.80 1.08 0.11 4168400400168 2215. 0.81 1.20 0.09 4168400400169 2215. 0.85 1.09 0.10 1. 4168400400170 2215. 0.85 1.13 0.14 2. 4168400400171 2215. 0.88 1.08 0.04 4168400400172 2215. 0.89 1.15 0.09 4168400400173 2215. 0.91 1.04 0.06 4168400400174 2215. 0.92 1.26 0.16 4168400400175 2215. 0.94 1.19 0.07 4168400400176 2215. 0.95 1.18 0.08 4168400400177 2215. 0.96 1.18 0.05 1. 4168400400178 2215. 0.96 1.13 0.08 2. 4168400400179 2215. 0.98 0.84 0.10 4168400400180 3005. -0.65 1.45 0.20 4168400400181 3005. -0.61 1.08 0.09 1. 4168400400182 3005. -0.61 1.08 0.14 2. 4168400400183 3005. -0.56 1.05 0.12 1. 4168400400184 3005. -0.56 1.25 0.19 2. 4168400400185 3005. -0.51 0.95 0.10 4168400400186 3005. -0.45 1.07 0.10 4168400400187 3005. -0.40 0.86 0.10 1. 4168400400188 3005. -0.40 0.93 0.09 2. 4168400400189 3005. -0.35 0.98 0.13 4168400400190 3005. -0.34 0.92 0.09 4168400400191 3005. -0.30 0.67 0.14 4168400400192 3005. -0.23 1.23 0.19 4168400400193 3005. -0.17 1.03 0.12 1. 4168400400194 3005. -0.17 0.90 0.13 2. 4168400400195 3005. -0.12 0.87 0.10 4168400400196 3005. -0.11 1.03 0.09 4168400400197 3005. -0.06 1.14 0.11 4168400400198 3005. 0.00 0.95 0.08 4168400400199 3005. 0.07 1.05 0.11 1. 4168400400200 3005. 0.07 1.08 0.17 2. 4168400400201 3005. 0.12 0.87 0.12 4168400400202 3005. 0.13 0.81 0.08 4168400400203 3005. 0.20 1.00 0.11 4168400400204 3005. 0.23 1.02 0.14 4168400400205 3005. 0.30 0.77 0.12 4168400400206 3005. 0.31 0.91 0.08 4168400400207 3005. 0.35 1.04 0.07 4168400400208 3005. 0.37 0.94 0.14 4168400400209 3005. 0.43 0.84 0.09 4168400400210 3005. 0.44 0.96 0.10 4168400400211 3005. 0.50 0.90 0.07 4168400400212 3005. 0.53 0.97 0.17 4168400400213 3005. 0.58 1.08 0.09 1. 4168400400214 3005. 0.58 0.88 0.13 2. 4168400400215 3005. 0.63 0.99 0.09 4168400400216 3005. 0.65 1.03 0.09 4168400400217 3005. 0.70 1.10 0.12 4168400400218 3005. 0.71 1.04 0.12 4168400400219 3005. 0.75 1.09 0.13 4168400400220 3005. 0.76 1.11 0.06 4168400400221 3005. 0.80 1.11 0.08 4168400400222 3005. 0.81 1.03 0.12 4168400400223 3005. 0.84 1.10 0.09 4168400400224 3005. 0.85 1.12 0.16 4168400400225 3005. 0.88 1.17 0.12 1. 4168400400226 3005. 0.88 1.11 0.09 2. 4168400400227 3005. 0.91 1.08 0.12 4168400400228 3005. 0.92 1.08 0.12 4168400400229 3005. 0.94 1.22 0.10 4168400400230 3005. 0.95 1.10 0.10 4168400400231 3005. 0.96 1.07 0.10 1. 4168400400232 3005. 0.96 1.23 0.08 2. 4168400400233 3005. 0.98 0.76 0.06 4168400400234 ENDDATA 218 0 4168400400235 ENDSUBENT 234 0 4168400499999 SUBENT 41684005 20200609 41884168400500001 BIB 5 11 4168400500002 REACTION (13-AL-27(N,X)12-MG-26,PAR,DA,G,REL) 4168400500003 See ANALYSIS for REL explanation. 4168400500004 ANALYSIS Angular distribution was defined as number of counts 4168400500005 at specified angle to number of counts average for all 4168400500006 angles. 4168400500007 FLAG (1.) Measurement by symmetrically placed detectors. 4168400500008 (2.) Measurement by symmetrically placed detectors. 4168400500009 ERR-ANALYS (ERR-S) Statistical uncertainty (information from the 4168400500010 author) 4168400500011 STATUS (TABLE) From author. 4168400500012 Fig.6 c of J.Phys.At.Nucl.,v.82,p.343,2019 4168400500013 ENDBIB 11 0 4168400500014 COMMON 1 3 4168400500015 E 4168400500016 KEV 4168400500017 1805. 4168400500018 ENDCOMMON 3 0 4168400500019 DATA 4 72 4168400500020 COS DATA ERR-S FLAG 4168400500021 NO-DIM ARB-UNITS ARB-UNITS NO-DIM 4168400500022 -0.65 0.96 0.08 4168400500023 -0.63 0.54 0.27 4168400500024 -0.61 0.91 0.07 1. 4168400500025 -0.61 1.02 0.09 2. 4168400500026 -0.56 0.91 0.05 1. 4168400500027 -0.56 0.95 0.08 2. 4168400500028 -0.53 1.16 0.31 4168400500029 -0.51 0.98 0.07 4168400500030 -0.46 0.95 0.08 4168400500031 -0.43 1.14 0.26 4168400500032 -0.40 0.84 0.08 4168400500033 -0.39 1.08 0.05 4168400500034 -0.35 0.95 0.08 1. 4168400500035 -0.35 0.94 0.06 2. 4168400500036 -0.32 1.36 0.24 4168400500037 -0.29 0.91 0.07 4168400500038 -0.23 1.11 0.08 4168400500039 -0.20 0.79 0.34 4168400500040 -0.18 1.01 0.08 4168400500041 -0.17 0.91 0.06 4168400500042 -0.11 0.99 0.07 1. 4168400500043 -0.11 1.02 0.06 2. 4168400500044 -0.08 0.68 0.34 4168400500045 -0.05 0.94 0.06 4168400500046 0.00 1.07 0.09 4168400500047 0.04 1.35 0.66 4168400500048 0.07 0.97 0.06 4168400500049 0.08 0.94 0.07 4168400500050 0.13 1.00 0.08 1. 4168400500051 0.13 0.88 0.06 2. 4168400500052 0.16 1.04 0.27 4168400500053 0.20 0.96 0.06 4168400500054 0.23 0.88 0.07 4168400500055 0.27 1.07 0.39 4168400500056 0.30 1.06 0.06 1. 4168400500057 0.30 0.94 0.07 2. 4168400500058 0.36 1.12 0.06 4168400500059 0.37 0.94 0.05 4168400500060 0.38 0.78 0.26 4168400500061 0.43 1.02 0.07 4168400500062 0.47 1.02 0.08 4168400500063 0.50 0.65 0.29 4168400500064 0.52 0.94 0.08 1. 4168400500065 0.52 0.88 0.07 2. 4168400500066 0.58 0.97 0.07 1. 4168400500067 0.58 0.94 0.06 2. 4168400500068 0.60 1.00 0.24 4168400500069 0.63 0.96 0.07 4168400500070 0.65 1.08 0.08 4168400500071 0.68 1.45 0.42 4168400500072 0.70 1.07 0.07 1. 4168400500073 0.70 0.94 0.08 2. 4168400500074 0.74 1.06 0.07 4168400500075 0.76 1.14 0.09 4168400500076 0.77 0.94 0.18 4168400500077 0.80 1.09 0.07 4168400500078 0.81 1.16 0.08 4168400500079 0.84 0.72 0.22 1. 4168400500080 0.84 1.09 0.07 2. 4168400500081 0.85 1.14 0.08 4168400500082 0.88 1.01 0.08 1. 4168400500083 0.88 1.08 0.06 2. 4168400500084 0.90 1.27 0.20 4168400500085 0.92 1.06 0.08 4168400500086 0.93 1.10 0.08 4168400500087 0.94 1.09 0.07 1. 4168400500088 0.94 1.16 0.33 2. 4168400500089 0.95 1.07 0.07 4168400500090 0.96 1.12 0.07 1. 4168400500091 0.96 1.21 0.06 2. 4168400500092 0.97 0.96 0.32 4168400500093 0.98 0.83 0.07 4168400500094 ENDDATA 74 0 4168400500095 ENDSUBENT 94 0 4168400599999 ENDENTRY 5 0 4168499999999