IAEA-NDS ENDF Download System, v-2008-07-22 0 0 0 0 5.010000+3 9.926900+0 0 0 0 26425 1451 1 0.000000+0 0.000000+0 0 0 0 06425 1451 2 0.000000+0 0.000000+0 0 0 83 46425 1451 3 5-B - 10 LASL EVAL-JAN79 L.STEWART, G.HALE, P.YOUNG 6425 1451 4 DIST-MAR84 REVO 840217 6425 1451 5 6425 1451 6 ************************************************************** 6425 1451 7 6425 1451 8 CROSS SECTIONS CHANGED BELOW 1.5 AND ABOVE 9 FROM 6425 1451 9 VERSION IV 6425 1451 10 6425 1451 11 DATA ABOVE 9 MEV NOT CONSISTENT WITH VERSION V DUE TO 6425 1451 12 THE ADDITION OF THE N,2NP 2ALPHA CROSS SECTION WHICH 6425 1451 13 IS ZERO IN VERSION V. 6425 1451 14 6425 1451 15 TOTAL HE-4 PRODUCTION CROSS SECTION (MT=207) SUM OF 6425 1451 16 6425 1451 17 MT=107 WHICH IS THE SUM OF MT=780 AND 781 6425 1451 18 MT=51-85 WHICH HAVE LR=22, DECAY BY (N,N ALPHA) 6425 1451 19 6425 1451 20 PLUS TWICE THE SUM OF 6425 1451 21 6425 1451 22 MT=113 (N,T, 2ALPHA) 6425 1451 23 MT=51-85 WHICH HAVE LR=35, DECAY BY (N,ND 2ALPHA) 6425 1451 24 MT=N,2N. A NEW EVALUATION BASED ON THE (N,2N) 14-MEV 6425 1451 25 MEASUREMENTS OF MATHER AND PAIN (REF.1), 6425 1451 26 ASSUMING ALL REACTIONS (N,2N 2ALPHA). 6425 1451 27 6425 1451 28 MF=2 SCATTERING RADIUS - 4.0238-13 CM IN MT=151 6425 1451 29 6425 1451 30 MF=3 MT=207, TOTAL HE-4 PRODUCTION FROM. 6425 1451 31 6425 1451 32 MT=107 SUM OF MT=780 AND 781 6425 1451 33 6425 1451 34 CALCULATED FROM R-MATRIX THEORY (REF. 2) 6425 1451 35 USING DATA ON TOTAL AND ELASTIC IN ADDITION TO 6425 1451 36 EXPERIMENTS ON N,ALPHA BELOW 1 MEV. 6425 1451 37 6425 1451 38 MT=780 (N,ALPHA ZERO) 6425 1451 39 0-1 MEV. R-MATRIX CALCULATIONS, EXP. DATA INCLUDED 6425 1451 40 FROM REF.3 AND REF.4. ANGULAR DISTRIBUTIONS FOR 6425 1451 41 THE INVERSE REACTION OF REF.5 ALSO INCLUDED. 6425 1451 42 1-20 MEV. BASED ON DATA FROM REF4 EXTRAPOLATED FROM 6425 1451 43 8-20 MEV AFTER RENORMALIZATION USING FACTOR OF 1.4. 6425 1451 44 6425 1451 45 MT=781 6425 1451 46 0-1 MEV. R-MATRIX CALCULATIONS. DATA FROM REF.6 IN- 6425 1451 47 CLUDED. ABSOLUTE DIF. DATA FROM REF.7 ALSO USED 6425 1451 48 IN THE ANALYSIS. 6425 1451 49 1-20 MEV. SMOOTH CURVE THROUGH MEASUREMENTS OF REF.46425 1451 50 AND REF.8, WITH SMOOTH EXTRAPOLATION FROM 15 TO 6425 1451 51 20 MEV. REF.4 DATA RENORMALIZED BY FACTOR 1.4. 6425 1451 52 6425 1451 53 MT=51-85 (N,NPRIME) 6425 1451 54 USING ALL AVAILABLE INFORMATION ON LEVEL SCHEMES AND 6425 1451 55 GAMMA RAY MEASUREMENTS, MANY LEVELS WERE ASSUMED TO 6425 1451 56 DECAY BY PARTICLE EMISSION, EITHER (N,N ALPHA) OR 6425 1451 57 (N,ND 2ALPHA). LR FLAGS WERE USED. 6425 1451 58 6425 1451 59 MT= N,2N EVALUATED AS DESCRIBED ABOVE 6425 1451 60 6425 1451 61 MT=113 (N,T 2 ALPHA) 6425 1451 62 0-2.3 MEV, BASED ON SINGLE-LEVEL FIT TO RESONANCE 6425 1451 63 MEASURED AT 2 MEV IN REF. 4, ASSUMING L=0 INCOMING 6425 1451 64 NEUTRONS AND L=2 OUTGOING TRITONS. 6425 1451 65 2.3-20 MEV, SMOOTH CURVE THROUGH MEASUREMENTS OF REF. 6425 1451 66 9 AND REF. 10, FOLLOWING THE GENERAL SHAPE OF REF. 4 6425 1451 67 FROM 4-9 MEV. 6425 1451 68 6425 1451 69 ************************************************************ 6425 1451 70 6425 1451 71 1. D.S. MATHER AND L.F. PAIN, AWRE REPORT 047/69 (1969). 6425 1451 72 2. G.M. HALE, PROC. INT. SPECIALISTS SYM. ON NEUTRON STAN- 6425 1451 73 DARDS AND APPLICATIONS, NBS-SP 493, GAITHERSBURG, MD (1977) 6425 1451 74 3. R.L. MACKLIN AND J.H. GIBBONS, PHYS.REV. 165, 1147 (1968). 6425 1451 75 4. E.A. DAVIS ET AL., NUCL.PHYS. 27, 448 (1961). 6425 1451 76 5. L.VAN DER ZWAN AND K.W. GEIGER, NUCL. PHYS. A180, 615 (1972)6425 1451 77 6. R.A. SCHRACK ET AL., PROC.ICINN(ERDA-CONF-760715-P2), 1345 6425 1451 78 (1976). 6425 1451 79 7. R.M. SEALOCK AND J.C. OVERLEY, PHYS.REV.C13, 2149 (1976). 6425 1451 80 8. D.O. NELLIS ET AL., PHYS.REV.C1, 847 (1970). 6425 1451 81 9. G.M. FRYE AND J.H. GAMMEL, PHYS.REV. 103, 328 (1956). 6425 1451 82 10. M.E. WYMAN ET AL., PHYS.REV. 112, 1264 (1958). 6425 1451 83 6425 1451 84 ************************************************************ 6425 1451 85 6425 1451 86 1 451 90 26425 1451 87 2 151 4 16425 1451 88 3 207 61 16425 1451 89 33 207 18 26425 1451 90 0.000000+0 0.000000+0 0 0 0 06425 1 0 91 0.000000+0 0.000000+0 0 0 0 06425 0 0 92 5.010000+3 9.926900+0 0 0 1 06425 2151 93 5.010000+3 1.000000+0 0 0 1 06425 2151 94 1.000000-5 1.000000+4 0 0 0 06425 2151 95 3.000000+0 4.023800-1 0 0 0 06425 2151 96 0.000000+0 0.000000+0 0 0 0 06425 2 0 97 0.000000+0 0.000000+0 0 0 0 06425 0 0 98 5.010000+3 9.926900+0 0 0 0 06425 3207 99 0.000000+0 2.790000+6 0 0 2 1726425 3207 100 23 5 172 2 6425 3207 101 1.000000-5 1.930000+5 1.000000-2 6.102700+3 2.530000-2 3.836600+36425 3207 102 1.000000-1 1.929600+3 1.000000+0 6.099200+2 1.000000+1 1.926100+26425 3207 103 1.000000+2 6.065700+1 1.000000+3 1.896400+1 1.000000+4 5.873900+06425 3207 104 2.000000+4 4.143500+0 3.000000+4 3.391600+0 4.000000+4 2.950500+06425 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