IAEA-NDS ENDF Download System, v-2008-07-22 0 0 0 0 6.315300+4 1.516070+2 1 0 0 11359 1451 1 0.000000+0 0.000000+0 0 0 0 01359 1451 2 0.000000+0 0.000000+0 0 0 239 811359 1451 3 63-Eu-153 BNL EVAL-FEB78 S.MUGHABGHAB 1359 1451 4 DIST-OCT80 910813 1359 1451 5 THIS MATERIAL DEALS WITH THE EVALUATION OF NEUTRON AND GAMMA-RAY 1359 1451 6 PRODUCTION CROSS SECTIONS OF THE ISOTOPE EU-153.THE EMPHASIS IS 1359 1451 7 PLACED ON THE LOW ENERGY REGION BECAUSE OF THE IMPORTANCE OF 1359 1451 8 EUROPIUM IN CONTROL RODS IN NUCLEAR REACTORS.THE RADIATIVE 1359 1451 9 CAPTURE CROSS SECTION IS UPDATED TO INCORPORATE RECENT AVAILABLE1359 1451 10 DATA. ALSO, THE (N,P),(N,A),AND (N,2N) CROSS SECTIONS ARE 1359 1451 11 RENORMALIZED TO RECENT MEASUREMENTS 1359 1451 12 FILE = 2 RESONANCE PARAMETERS 1359 1451 13 -------------------------------- 1359 1451 14 RESONANCE PARAMETERS RECOMMENDED IN BNL-325(1973) (REF.1) WERE 1359 1451 15 ADOPTED IN THIS EVALUATION. SPIN ASSIGNMENT OF ONE RESONANCE AT 1359 1451 16 2.457 EV IS DETERMINED. FOR THE OTHER RESONANCES, SPIN 1359 1451 17 ASSIGNMENTS WERE MADE RANDOMLY IN ORDER TO SATISFY SPIN INDEPEND-1359 1451 18 ENCE OF STRENGTH FUNCTION AND THE 2J+1 LAW OF LEVEL DENSITY. 1359 1451 19 RECENT DATA ON THE MEASUREMENT OF THE THERMAL CROSS SECTION OF EU1359 1451 20 -153 BROUGHT OUT THE PROBLEMS WITH THE ACCURATE DETERMINATION OF 1359 1451 21 THIS CROSS SECTION.(REF2-6).THESE PROBLEMS ARE RELATED TO THE 1359 1451 22 LACK OF VERY ACCURATE KNOWLEDGE OF EU-151 CONTENT IN EU-153 1359 1451 23 SAMPLES AND PREVIOUS INACCURATE VALUE OF HALF LIFE OF EU-154. 1359 1451 24 (16YEARS). THE HALF LIFE OF EU-154 IS PRESENTLY KNOWN AS 8.2-+0.31359 1451 25 YEARS. AFTER CORRECTING THE DATA FOR EU-151 IMPURITY AND HALF1359 1451 26 LIFE OF EU-154,A WEIGHTED AVERAGE VALUE 300 B IS DERIVED 1359 1451 27 FOR THE THERMAL CROSS SECTION OF EU-153. 1359 1451 28 THE POSITIVE ENERGY RESONANCES CONTRIBUTE 58B TO THE THERMAL 1359 1451 29 CROSS-SECTION. THE DIFFERENCE IS ACCOUNTED FOR BY A NEGATIVE 1359 1451 30 ENERGY RESONANCE.WITH A SPIN OF J=2 AS DERIVED FROM THERMAL 1359 1451 31 SPECTRA MEASUREMENT(REF.7) 1359 1451 32 THE THERMAL CROSS SECTIONS ARE: 1359 1451 33 CAPTURE = 299.85B 1359 1451 34 SCATTERING = 6.75B 1359 1451 35 TOTAL = 306.60B 1359 1451 36 THE CAPTURE RESONANCE INTEGRAL = 1448. B 1359 1451 37 THE UNRESOLVE ENERGY REGION FROM 97.22EV TO 10 KEV IS REPRESENTED1359 1451 38 BY AVERAGE RESONANCE PARAMETERS AS RECOMMENDED IN REF.1: 1359 1451 39 S(0) =2.50 E-04 1359 1451 40 GAMMA WIDTH=95.8 MV 1359 1451 41 AVERAGE SPACING=1.37 EV 1359 1451 42 S(1) =6.0 E-05 1359 1451 43 FILE=3 (NEUTRON CROSS SECTIONS) 1359 1451 44 ------------------------------- 1359 1451 45 4.1 TOTAL CROSS SECTION (MT = 1) 1359 1451 46 SEVERAL MEASUREMENTS OF THE TOTAL CROSS SECTION IN THE LOW ENERGY1359 1451 47 RANGE WERE EVALUATED AND REPRESENTED AS RESOLVED RESONANCE 1359 1451 48 PARAMETERS. IN THE INTERMEDIATE ENERGY RANGE BETWEEN 0.8 KEV - 24 1359 1451 49 KEV, THE TOTAL CROSS SECTION OF NATURAL EUROPIUM WAS MEASURED BY 1359 1451 50 EGELSTAFF(3). COMPARED TO THE RECENT MEASUREMENTS BY RAHN (9) FOR 1359 1451 51 EU-153 (ENERGY RANGE OF 0.06KEV TO 3 KEV). EGELSTAFF'S DATA IS 1359 1451 52 ABOUT 30% TOO SMALL. THE SMOOTH TOTAL CROSS SECTION CALCULATED 1359 1451 53 USING THE UNRESOLVED RESONANCE PARAMETER AGREES WITH RAHN'S DATA 1359 1451 54 WITHIN 10%. ALTHOUGH RAHN'S TOTAL CROSS SECTION DATA SHOW THE 1359 1451 55 RESONANCE SHAPE AND THE AVERAGE VALUES OVER SEVERAL RESONANCES 1359 1451 56 FLUCTUATE, THE DATA WERE REPRESENTED AS UNRESOLVED RESONANCE 1359 1451 57 PARAMETERS, SO THAT SELF SHIELDING AND THE DOPPLER EFFECT COULD BE1359 1451 58 CALCULATED. BECAUSE OF NO DATA BETWEEN 30 KEV TO 2.3 MEV, THE 1359 1451 59 TOTAL CROSS SECTION WAS CALCULATED BY THE OPTICAL MODEL USING 1359 1451 60 MOSTLY BESCHETTI AND GREENLESS' OPTICAL PARAMETERS (10). 1359 1451 61 BETWEEN 2.3 MEV TO 15 MEV, THE DATA OBTAINED BY FOSTER ET AL (11)1359 1451 62 FOR NATURAL EUROPIUM WERE TAKEN. ABOVE THIS ENERGY RANGE, THE 1359 1451 63 TOTAL CROSS SECTION WAS EVALUATED FROM A COMPARISON BETWEEN THE 1359 1451 64 OPTICAL MODEL CALCULATION AND FOSTER'S DATA. 1359 1451 65 4.2 ELASTIC SCATTERING CROSS SECTION (MT = 2) 1359 1451 66 THE ELASTIC SCATTERING CROSS SECTIONS IN THE ENERGY HIGHER THAN 1359 1451 67 THE UNRESOLVED RESONANCE ENERGY WERE OBTAINED BY SUBSTRUCTING THE 1359 1451 68 NON-ELASTIC CROSS SECTION FROM THE EVALUATED TOTAL CROSS SECTION. 1359 1451 69 4.3 NONELASTIC SCATTERING CROSS SECTION (MT = 3) 1359 1451 70 THE NONELASTIC SCATTERING CROSS SECTION WAS CALCULATED BY SUMMING1359 1451 71 UP ALL CROSS SECTIONS EXCEPT THE ELASTIC SCATTERING CROSS SECTION.1359 1451 72 4.4 INELASTIC SCATTERING CROSS SECTION (MT = 4, 51, 52 .... 91) 1359 1451 73 THE INELASTIC SCATTERING CROSS SECTIONS WERE GIVEN AS TOTAL (MT =1359 1451 74 4), DISCRETE LEVEL EXCITATION CROSS SECTION (MT = 51 ...) OF THE 1359 1451 75 FIRST 11LEVELS AND CONTINUUM LEVEL EXCITATION CROSS SECTION (MT = 1359 1451 76 91). THE LEVEL SCHEME FOR THESE DISCRETE LEVELS IS TAKEN FROM (7),1359 1451 77 (REF.12-18) 1359 1451 78 THE INDIVIDUAL LEVEL EXCITATION CROSS SECTIONS WERE CALCULATED 1359 1451 79 USING THE CODE COMNUC-3 (14,15) FOR THE NEUTRON ENERGIES UP TO 3 1359 1451 80 MEV. THE INELASTIC SCATTERING CROSS SECTION FOR DISCRETE LEVEL 1359 1451 81 EXCITATION ABOVE 3 MEV WAS NEGLECTED AND THE INELASTIC SCATTERING 1359 1451 82 CROSS SECTION FOR CONTINUUM LEVEL EXCITATION WAS CALCULATED 1359 1451 83 BY THE CASCADE CALCULATION OF GROGI-3 (21,22). THE LEVEL DENSITY 1359 1451 84 PARAMETERS FOR THE CONTINUUM OF LEVELS WERE TAKEN FROM THE COOK 1359 1451 85 DATA (23) FOR DEFORMED NUCLEI USING THE GILBERT-CAMERON FORMULA. 1359 1451 86 (REF.24). 1359 1451 87 (N,P) AND (N,N'P) CROSS SECTIONS (MT=103,28) 1359 1451 88 -------------------------------------------- 1359 1451 89 EXPERIMENTAL DATA ARE AVAILABLE ONLY FOR A NEUTRON ENERGY 14.7 1359 1451 90 MEV.(REFS.25-28). THE ENDF/B IV EVALUATION, BASED ON SEMI- 1359 1451 91 EMPIRICAL STATISCAL MODEL CODE THRESH (REF.29),IS RENORMALIZED 1359 1451 92 TO A VALUE OF 5.6 MB AT 14.7 MEV. 1359 1451 93 NO CROSS SECTION MEASUREMENTS FOR (N,N'P) REACTION ARE AVAILABLE 1359 1451 94 THIS CROSS SECTION WAS CALCULATED BY USING GROGI-3 CODE 1359 1451 95 (N,ALPHA) AND (N,N'ALPHA) CROSS SECTIONS (MT=107,22) 1359 1451 96 ---------------------------------------------------- 1359 1451 97 TWO DISCRAPENT VALUES AT 14.7 MEV ARE AVAILABLE,2.2-+0.3 MB 1359 1451 98 AND 9-+2 MB(REFS.26,30). IN THIS EVALUATION, A VALUE OF 9 MB. 1359 1451 99 IS ADOPTED AT 14.7 MEV. THIS CHOICE IS BASED ON SYSTEMATICS, 1359 1451 100 WHICH INDICATE THAT (N,ALPHA) REACTION HAS A MAXIMUM OF ABOUT 1359 1451 101 9 MB AT ATOMIC WEIGHT= 155,AND ON OBTAINING AN ESTIMATE FROM THE 1359 1451 102 DOUBLE DIFFERENTIAL DATA OF REF.31 AT NEUTRON ENERGY OF 18.15 1359 1451 103 MEV. THEREFORE THE (N,ALPHA) EVALUATION OF ENDF/B IV WHICH IS 1359 1451 104 BASED ON THRESH CALCULATIONS IS RENORMALIZED TO 9MB AT 14.7 1359 1451 105 MEV.THE THERMAL CROSS SECTION IS SET EQUAL TO 1 MICRO BARN,REF.321359 1451 106 SINCE NO EXPERIMENTAL DATA IS AVAILABLE FOR (N,N'ALPHA) 1359 1451 107 REACTION,THE CROSS SECTION WAS CALCULATED USING GROGI-3 CODE 1359 1451 108 (N,2N),(N,3N) CROSS SECTIONS (MT=16)(MT=17) 1359 1451 109 -------------------------------------------- 1359 1451 110 SEVERAL 14.7 MEV CROSS SECTIONS IN WHICH THE RESIDUAL NUCLEUS 1359 1451 111 GOES TO THE METASTABLE STATE EU-152-M1 WITH 9.3 H AND EU-152-M2 1359 1451 112 WITH 96 MIN HALF L.FE HAVE BEEN MEASURED.REF.33-35,26. QAIM,REF361359 1451 113 MEASURED RECENTLY,THE CROSS SECTION LEADING TO THE 12.4 Y GROUND 1359 1451 114 STATE OF EU-152,AS WELL AS THE CROSS SECTIONS TO THE TWO META- 1359 1451 115 STABLE STATES. THE TOTAL (N,2N) CROSS SECTION (REF.36) IS 2047-+ 1359 1451 116 171 B. THE GROGI-3 CALCULATIONS OF ENDF/B IV ARE NORMALIZED TO 1359 1451 117 THIS VALUE AT 14.7 MEV. 1359 1451 118 FOR (N,3N) REACTION,NO EXPERIMENTAL RESULTS ARE AVAILABLE.AS A 1359 1451 119 RESULT,THE VALUES CALCULATED BY GROGI-3 WERE ADOPTED. 1359 1451 120 (N,D),(N,T)AND (N,HE-3) REACTION CROSS SECTIONS (MT=104,105,107) 1359 1451 121 -----------------------------------------------------------------1359 1451 122 SINCE NO EXPERIMENTAL DATA ARE AVAILABLE FOR THESE REACTIONS, 1359 1451 123 THE VALUES CALCULATED BY GROGI-3 FOR ENDF/B IV WERE ADOPTED. 1359 1451 124 THE RADIATIVE CAPTURE CROSS SECTION (MT=102) 1359 1451 125 -------------------------------------------- 1359 1451 126 THE RADIATIVE CAPTURE CROSS SECTION IN THE ENERGY RANGE 10-5 TO 1359 1451 127 97.7 EV IS REPRESENTED BY THE RESONANCE PARAMETERS. BETWEEN 97.7 1359 1451 128 EV AND 10 KEV IT IS DESCRIBED BY AVERAGE RESONANCE PARAMETERS 1359 1451 129 ADOPTED FROM REF.1. IN THE HIGHER ENERGY REGION,10 KEV TO 360 KEV1359 1451 130 THE EVALUATION IS BASED ON EXPERIMENTAL DATA OF REF.2,37-39. 1359 1451 131 ABOVE 360 KEV,THE EVALUATION IS BASED ON COMNUC CALCULATIONS(REF.1359 1451 132 20) AND NORMALIZED TO A VALUE OF 1MB AT 14.7MEV. 1359 1451 133 AFTER THE COMPLETION OF THIS EVALUATION,THE CAPTURE CROSS 1359 1451 134 SECTION WAS AVERAGED OVER A 620-POINT CFRMF SPECTRUM. THE VALUE 1359 1451 135 THUS OBTAINED IS 1.585 B,WHICH IS IN EXCELLENT AGREEMENT WITH 1359 1451 136 AN EXPERIMENTAL VALUE OF 1.51 -+0.12 B. (REF.40) 1359 1451 137 FILE=4(ANGULAR DISTRIBUTION OF SECONDARY NEUTRNS) 1359 1451 138 ------------------------------------------------- 1359 1451 139 NO EXPERIMENTAL DATA WERE AVAILABLE, SO THE VALUES CALCULATED BY 1359 1451 140 ABACUS-2(41) USING THE OPTICAL MODEL WAS ADOPTED AS THE 1359 1451 141 EVALUATED DATA. THE LEGENDRE COEFFICIENTS, CALCULATED BY CHAD 1359 1451 142 (42) WERE GIVEN IN FILE 4. 1359 1451 143 5.2 INELASTICALLY SCATTERED NEUTRONS (N,2N),(N,3N),(N,N'P), 1359 1451 144 AND(N,N'ALPHA) REACTION (MT=51...,91,MT=16,17,22,23) 1359 1451 145 NEUTRONS FROM THESE REACTIONS WERE ASSUMED TO BE ISOTOPIC IN THE 1359 1451 146 CENTER OF MASS SYSTEM. 1359 1451 147 FILE =5(ENERGY DISTRIBUTION OF SECONDARY NEUTRONS) 1359 1451 148 -------------------------------------------------- 1359 1451 149 6.1 (N,2N),(N,3N) AND (N,N') REACTIONS (MT=16,17, AND 91) 1359 1451 150 THE EFFECTIVE TEMPERATURE OF THESE MAXWELLIANS WERE OBTAINED BY 1359 1451 151 THE WEISKOPF FORMULA (43). 1359 1451 152 FILE=12 (MULTIPLICITIES AND TRANSITION PROBABILITY ARRAY) 1359 1451 153 --------------------------------------------------------- 1359 1451 154 7.1 RADIATIVE CAPTURE GAMMA-RAY MULTIPLICITY 1359 1451 155 GROSHEV'S AND SHERA'S DATA (44,45) USED AS EVALUATED DATA FOR 1359 1451 156 RADIATIVE CAPTURE REACTION (MT = 102) BETWEEN .00001 EV TO 1 MEV 1359 1451 157 NEUTRON ENERGY. 1359 1451 158 THERE IS NO EXPERIMENTAL DATA FOR NEUTRON ENERGIES LARGER THAN 1359 1451 159 1 MEV. SO THE GAMMA RAY PRODUCTION CROSS SECTIONS FOR ALL 1359 1451 160 REACTIONS WERE CALCULATED BY THE GROGI-3 CODE. 1359 1451 161 7.2 TRANSITION PROBABILITY ARRAY FOR GAMMA RAY DUE TO INELASTIC 1359 1451 162 NEUTRON SCATTERING 1359 1451 163 THE EVALUATED TRANSITION PROBABILITIES WERE CALCULATED FROM REF 1359 1451 164 (12,14,16,46). MOST DATA WERE TAKEN FROM (16). 1359 1451 165 FILE=14(ANGULAR DISTRIBUTION OF GAMMA RAYS) 1359 1451 166 ------------------------------------------- 1359 1451 167 ALL GAMMA RAY PRODUCED BY NEUTRON CAPTURE, INELASTIC AND NON 1359 1451 168 ELASTIC SCATTERING ARE ASSUMED TO BE ISOTOPIC. 1359 1451 169 FILE=15(ENERGY DISTRIBUTION OF SECONDARY GAMMA RAYS) 1359 1451 170 --------------------------------------------------- 1359 1451 171 FOR THERMAL NEUTRON CAPTURE THEY ARE EXPRESSED BY HYSTOGRAM TYPE 1359 1451 172 SPECTRUM WITH 0.25 MEV BIN ENERGY WIDTH. FOR ABOVE 1 MEV NEUTRON 1359 1451 173 ENERGY, THEY ARE TABULATED WITH 0.5 MEV BIN. 1359 1451 174 REFERENCES 1359 1451 175 ----------- 1359 1451 176 1) S.F.MUGHABGHAB AND D.I.GARBER,BNL-325 THIRD EDITION VOL-1,19731359 1451 177 2) M.C.MOXON,D.A.J.ENDACOTT,AND J.E.JOLLY,ANNALS NUCL.ENER.3,399 1359 1451 178 (1976) 1359 1451 179 3) J.I.WIDDER,NUCL. SC. ENG.,60,53(1976) 1359 1451 180 4) J.I. KIM,E.M.GRYNTAKIS,H.J.BORN,RADIOCHIMICA ACTA,22,20,(1975)1359 1451 181 5) V.P. VERTEBNY ET.AL,PROC. 1ST NEUTRON PHYSICS CONF,KIEVE,PART 1359 1451 182 2,239,(1973) 1359 1451 183 6) V.F. RAZBUDEJ,A.F.FEDOROVA,A.V.MURAVITSKIJ,INDC(CCP)-100/U, 1359 1451 184 23(1977) 1359 1451 185 7) W.STOFFL,D.RABENSTEIN,K.SCHRECKENBACH,AND T.VON EGIDY,Z.PHYSIK1359 1451 186 A282,97 (1977) 1359 1451 187 8) P.A.EGELSTAFF.SCISRS DATA NO. 60952 (1955). 1359 1451 188 9) F.J.RAHN, PRIVATE COMMUNICATION (1973). 1359 1451 189 10)F.D.BECCHETTI AND G.W.GREENLEES. PHYS. REV. 182, 1190 (1969). 1359 1451 190 11)D.G.FOSTER JR. 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NATURFORSCHUNG 16A, 927 (1961). 1359 1451 242 1 451 323 11359 1451 243 2 151 87 01359 1451 244 3 1 71 11359 1451 245 3 2 71 11359 1451 246 3 3 53 11359 1451 247 3 4 40 01359 1451 248 3 16 8 01359 1451 249 3 17 6 01359 1451 250 3 22 14 11359 1451 251 3 28 13 01359 1451 252 3 51 22 01359 1451 253 3 52 21 01359 1451 254 3 53 20 01359 1451 255 3 54 18 01359 1451 256 3 55 17 01359 1451 257 3 56 17 01359 1451 258 3 57 13 01359 1451 259 3 58 13 01359 1451 260 3 59 12 01359 1451 261 3 60 11 01359 1451 262 3 61 10 01359 1451 263 3 91 15 01359 1451 264 3 102 21 11359 1451 265 3 103 14 01359 1451 266 3 104 12 01359 1451 267 3 105 10 01359 1451 268 3 106 5 01359 1451 269 3 107 14 01359 1451 270 3 251 25 01359 1451 271 3 252 25 01359 1451 272 3 253 25 01359 1451 273 4 2 392 01359 1451 274 4 16 10 01359 1451 275 4 17 10 01359 1451 276 4 22 10 01359 1451 277 4 28 10 01359 1451 278 4 51 10 01359 1451 279 4 52 10 01359 1451 280 4 53 10 01359 1451 281 4 54 10 01359 1451 282 4 55 10 01359 1451 283 4 56 10 01359 1451 284 4 57 10 01359 1451 285 4 58 10 01359 1451 286 4 59 10 01359 1451 287 4 60 10 01359 1451 288 4 61 10 01359 1451 289 4 91 10 01359 1451 290 5 16 7 01359 1451 291 5 17 7 01359 1451 292 5 22 7 01359 1451 293 5 28 7 01359 1451 294 5 91 7 01359 1451 295 12 3 11 01359 1451 296 12 51 3 01359 1451 297 12 52 3 01359 1451 298 12 53 3 01359 1451 299 12 54 3 01359 1451 300 12 55 4 01359 1451 301 12 56 3 01359 1451 302 12 57 3 01359 1451 303 12 58 4 01359 1451 304 12 59 3 01359 1451 305 12 60 3 01359 1451 306 12 61 3 01359 1451 307 12 102 5 01359 1451 308 14 3 1 01359 1451 309 14 51 1 01359 1451 310 14 52 1 01359 1451 311 14 53 1 01359 1451 312 14 54 1 01359 1451 313 14 55 1 01359 1451 314 14 56 1 01359 1451 315 14 57 1 01359 1451 316 14 58 1 01359 1451 317 14 59 1 01359 1451 318 14 60 1 01359 1451 319 14 61 1 01359 1451 320 14 102 1 01359 1451 321 15 3 235 01359 1451 322 15 102 34 01359 1451 323 0.000000+0 0.000000+0 0 0 0 01359 1 0 324 0.000000+0 0.000000+0 0 0 0 01359 0 0 325 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2.13650-15 135915 3 1888 0.000000+0 1.100000+7 0 0 1 26135915 3 1889 26 1 135915 3 1890 0.000000+0 4.014800-7 5.000000+5 5.220300-7 1.000000+6 4.013800-7135915 3 1891 1.500000+6 2.891100-7 2.000000+6 1.811800-7 2.500000+6 1.029900-7135915 3 1892 3.000000+6 5.393100-8 3.500000+6 2.646900-8 4.000000+6 1.226400-8135915 3 1893 4.500000+6 5.397800-9 5.000000+6 2.266700-9 5.500000+6 9.14050-10135915 3 1894 6.000000+6 3.58290-10 6.500000+6 1.38570-10 7.000000+6 5.31460-11135915 3 1895 7.500000+6 2.01530-11 8.000000+6 7.70440-12 8.500000+6 2.91410-12135915 3 1896 9.000000+6 1.15720-12 9.500000+6 5.35570-13 1.000000+7 2.54530-13135915 3 1897 1.050000+7 1.23860-13 1.100000+7 5.85310-14 1.150000+7 2.65950-14135915 3 1898 1.200000+7 1.15750-14 1.250000+7 4.80040-15 135915 3 1899 0.000000+0 1.200000+7 0 0 1 26135915 3 1900 26 1 135915 3 1901 0.000000+0 4.575100-7 5.000000+5 5.533300-7 1.000000+6 3.917000-7135915 3 1902 1.500000+6 2.578600-7 2.000000+6 1.539600-7 2.500000+6 8.918500-8135915 3 1903 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3.61870-11 8.000000+6 1.49600-11 8.500000+6 6.33610-12135915 3 1918 9.000000+6 2.77040-12 9.500000+6 1.24410-12 1.000000+7 5.70290-13135915 3 1919 1.050000+7 2.65800-13 1.100000+7 1.27060-13 1.150000+7 6.28280-14135915 3 1920 1.200000+7 3.06120-14 1.250000+7 1.46260-14 135915 3 1921 0.000000+0 1.400000+7 0 0 1 26135915 3 1922 26 1 135915 3 1923 0.000000+0 4.998000-7 5.000000+5 5.892200-7 1.000000+6 4.083700-7135915 3 1924 1.500000+6 2.495800-7 2.000000+6 1.313900-7 2.500000+6 6.426900-8135915 3 1925 3.000000+6 2.983100-8 3.500000+6 1.385600-8 4.000000+6 6.775100-9135915 3 1926 4.500000+6 3.492200-9 5.000000+6 1.774900-9 5.500000+6 8.73040-10135915 3 1927 6.000000+6 4.15080-10 6.500000+6 1.90880-10 7.000000+6 8.51120-11135915 3 1928 7.500000+6 3.70260-11 8.000000+6 1.59480-11 8.500000+6 6.91020-12135915 3 1929 9.000000+6 3.07460-12 9.500000+6 1.41720-12 1.000000+7 6.74290-13135915 3 1930 1.050000+7 3.28040-13 1.100000+7 1.61580-13 1.150000+7 7.99790-14135915 3 1931 1.200000+7 3.96960-14 1.250000+7 1.97350-14 135915 3 1932 0.000000+0 1.500000+7 0 0 1 26135915 3 1933 26 1 135915 3 1934 0.000000+0 4.769100-7 5.000000+5 5.857000-7 1.000000+6 4.227600-7135915 3 1935 1.500000+6 2.608200-7 2.000000+6 1.367000-7 2.500000+6 6.542300-8135915 3 1936 3.000000+6 2.910600-8 3.500000+6 1.248900-8 4.000000+6 5.355400-9135915 3 1937 4.500000+6 2.400300-9 5.000000+6 1.161600-9 5.500000+6 5.94420-10135915 3 1938 6.000000+6 3.00360-10 6.500000+6 1.47440-10 7.000000+6 7.03630-11135915 3 1939 7.500000+6 3.27740-11 8.000000+6 1.50170-11 8.500000+6 6.83070-12135915 3 1940 9.000000+6 3.12850-12 9.500000+6 1.46380-12 1.000000+7 7.07160-13135915 3 1941 1.050000+7 3.52280-13 1.100000+7 1.79080-13 1.150000+7 9.18230-14135915 3 1942 1.200000+7 4.70260-14 1.250000+7 2.38990-14 135915 3 1943 0.000000+0 1.600000+7 0 0 1 26135915 3 1944 26 1 135915 3 1945 0.000000+0 4.431100-7 5.000000+5 5.713800-7 1.000000+6 4.345300-7135915 3 1946 1.500000+6 2.766400-7 2.000000+6 1.481600-7 2.500000+6 7.149700-8135915 3 1947 3.000000+6 3.173700-8 3.500000+6 1.337400-8 4.000000+6 5.494600-9135915 3 1948 4.500000+6 2.264900-9 5.000000+6 9.62190-10 5.500000+6 4.33960-10135915 3 1949 6.000000+6 2.11550-10 6.500000+6 1.08550-10 7.000000+6 5.51230-11135915 3 1950 7.500000+6 2.73740-11 8.000000+6 1.33520-11 8.500000+6 6.43390-12135915 3 1951 9.000000+6 3.08870-12 9.500000+6 1.49200-12 1.000000+7 7.32490-13135915 3 1952 1.050000+7 3.68140-13 1.100000+7 1.89580-13 1.150000+7 9.92990-14135915 3 1953 1.200000+7 5.23150-14 1.250000+7 2.74620-14 135915 3 1954 0.000000+0 1.700000+7 0 0 1 26135915 3 1955 26 1 135915 3 1956 0.000000+0 4.127100-7 5.000000+5 5.534300-7 1.000000+6 4.403300-7135915 3 1957 1.500000+6 2.905400-7 2.000000+6 1.610200-7 2.500000+6 7.981000-8135915 3 1958 3.000000+6 3.610100-8 3.500000+6 1.535700-8 4.000000+6 6.300500-9135915 3 1959 4.500000+6 2.553200-9 5.000000+6 1.042300-9 5.500000+6 4.36500-10135915 3 1960 6.000000+6 1.90880-10 6.500000+6 8.91320-11 7.000000+6 4.54130-11135915 3 1961 7.500000+6 2.36930-11 8.000000+6 1.22250-11 8.500000+6 6.21960-12135915 3 1962 9.000000+6 3.13640-12 9.500000+6 1.57800-12 1.000000+7 7.97670-13135915 3 1963 1.050000+7 4.07820-13 1.100000+7 2.11760-13 1.150000+7 1.11740-13135915 3 1964 1.200000+7 5.96970-14 1.250000+7 3.20350-14 135915 3 1965 0.000000+0 1.800000+7 0 0 1 26135915 3 1966 26 1 135915 3 1967 0.000000+0 3.910900-7 5.000000+5 5.372700-7 1.000000+6 4.414600-7135915 3 1968 1.500000+6 2.997800-7 2.000000+6 1.714800-7 2.500000+6 8.767900-8135915 3 1969 3.000000+6 4.085200-8 3.500000+6 1.779500-8 4.000000+6 7.412800-9135915 3 1970 4.500000+6 3.025300-9 5.000000+6 1.234300-9 5.500000+6 5.11820-10135915 3 1971 6.000000+6 2.18370-10 6.500000+6 9.68990-11 7.000000+6 4.66760-11135915 3 1972 7.500000+6 2.38100-11 8.000000+6 1.26260-11 8.500000+6 6.71980-12135915 3 1973 9.000000+6 3.54510-12 9.500000+6 1.85720-12 1.000000+7 9.71050-13135915 3 1974 1.050000+7 5.09190-13 1.100000+7 2.68900-13 1.150000+7 1.43370-13135915 3 1975 1.200000+7 7.71820-14 1.250000+7 4.18530-14 135915 3 1976 0.000000+0 1.900000+7 0 0 1 26135915 3 1977 26 1 135915 3 1978 0.000000+0 3.750600-7 5.000000+5 5.237700-7 1.000000+6 4.402500-7135915 3 1979 1.500000+6 3.057400-7 2.000000+6 1.795700-7 2.500000+6 9.452200-8135915 3 1980 3.000000+6 4.548100-8 3.500000+6 2.047500-8 4.000000+6 8.789500-9135915 3 1981 4.500000+6 3.673500-9 5.000000+6 1.524300-9 5.500000+6 6.40010-10135915 3 1982 6.000000+6 2.76180-10 6.500000+6 1.23640-10 7.000000+6 5.91340-11135915 3 1983 7.500000+6 2.97840-11 8.000000+6 1.57540-11 8.500000+6 8.49840-12135915 3 1984 9.000000+6 4.62090-12 9.500000+6 2.50960-12 1.000000+7 1.35650-12135915 3 1985 1.050000+7 7.31480-13 1.100000+7 3.94910-13 1.150000+7 2.14020-13135915 3 1986 1.200000+7 1.16600-13 1.250000+7 6.38470-14 135915 3 1987 0.000000+0 2.000000+7 0 0 1 26135915 3 1988 26 1 135915 3 1989 0.000000+0 3.609800-7 5.000000+5 5.110700-7 1.000000+6 4.376400-7135915 3 1990 1.500000+6 3.100000-7 2.000000+6 1.866100-7 2.500000+6 1.011100-7135915 3 1991 3.000000+6 5.035100-8 3.500000+6 2.356600-8 4.000000+6 1.054500-8135915 3 1992 4.500000+6 4.588400-9 5.000000+6 1.971700-9 5.500000+6 8.50850-10135915 3 1993 6.000000+6 3.75240-10 6.500000+6 1.71590-10 7.000000+6 8.32250-11135915 3 1994 7.500000+6 4.23980-11 8.000000+6 2.26060-11 8.500000+6 1.23180-11135915 3 1995 9.000000+6 6.79350-12 9.500000+6 3.76710-12 1.000000+7 2.09130-12135915 3 1996 1.050000+7 1.15880-12 1.100000+7 6.40650-13 1.150000+7 3.54070-13135915 3 1997 1.200000+7 1.95950-13 1.250000+7 1.08690-13 135915 3 1998 0.000000+0 0.000000+0 0 0 0 0135915 0 1999 6.315300+4 1.516070+2 0 0 1 0135915102 2000 0.000000+0 0.000000+0 0 1 1 3135915102 2001 3 1 135915102 2002 1.000000-5 1.000000+0 1.000000+6 1.000000+0 2.000000+7 1.000000+0135915102 2003 0.000000+0 0.000000+0 0 0 1 4135915102 2004 4 1 135915102 2005 0.000000+0 1.000000-5 0 0 1 27135915102 2006 27 1 135915102 2007 0.000000+0 3.832000-7 2.500000+5 3.529900-7 5.000000+5 3.176400-7135915102 2008 7.500000+5 3.705800-7 1.000000+6 3.235700-7 1.250000+6 2.959800-7135915102 2009 1.500000+6 2.850600-7 1.750000+6 2.823400-7 2.000000+6 2.600500-7135915102 2010 2.250000+6 2.215300-7 2.500000+6 1.815100-7 2.750000+6 1.427100-7135915102 2011 3.000000+6 1.058800-7 3.250000+6 8.263400-8 3.500000+6 6.572100-8135915102 2012 3.750000+6 5.126100-8 4.000000+6 3.690200-8 4.250000+6 2.571400-8135915102 2013 4.500000+6 2.074700-8 4.750000+6 1.628900-7 5.000000+6 2.227200-9135915102 2014 5.250000+6 6.438900-9 5.500000+6 8.409100-9 5.750000+6 6.438700-9135915102 2015 6.000000+6 6.139100-9 6.250000+6 1.878710-9 6.444000+6 0.000000+0135915102 2016 0.000000+0 0.999999+6 0 0 1 27135915102 2017 27 1 135915102 2018 0.000000+0 3.832000-7 2.500000+5 3.529900-7 5.000000+5 3.176400-7135915102 2019 7.500000+5 3.705800-7 1.000000+6 3.235700-7 1.250000+6 2.959800-7135915102 2020 1.500000+6 2.850600-7 1.750000+6 2.823400-7 2.000000+6 2.600500-7135915102 2021 2.250000+6 2.215300-7 2.500000+6 1.815100-7 2.750000+6 1.427100-7135915102 2022 3.000000+6 1.058800-7 3.250000+6 8.263400-8 3.500000+6 6.572100-8135915102 2023 3.750000+6 5.126100-8 4.000000+6 3.690200-8 4.250000+6 2.571400-8135915102 2024 4.500000+6 2.074700-8 4.750000+6 1.628900-7 5.000000+6 2.227200-9135915102 2025 5.250000+6 6.438900-9 5.500000+6 8.409100-9 5.750000+6 6.438700-9135915102 2026 6.000000+6 6.139100-9 6.250000+6 1.473400-9 6.500000+6 0.000000+0135915102 2027 0.000000+0 1.000000+6 0 0 1 2135915102 2028 2 1 135915102 2029 0.000000+0 1.000000-6 1.000000+6 0.000000+0 135915102 2030 0.000000+0 2.000000+7 0 0 1 2135915102 2031 2 1 135915102 2032 0.000000+0 1.000000-6 1.000000+6 0.000000+0 135915102 2033 0.000000+0 0.000000+0 0 0 0 0135915 0 2034 0.000000+0 0.000000+0 0 0 0 01359 0 0 2035 0.000000+0 0.000000+0 0 0 0 0 0 0 0 2036 0.000000+0 0.000000+0 0 0 0 0 -1 0 0 0