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INDC(SEC)-46/U+R+F+SIN DC INTERNATIONAL NUCLEAR DATA ...

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92 URANIUM 235 NEUTRON D E L A Y E D N E U T R O N S E M I T T E D P E R F I S S I (CONTINUED)<br />

O N<br />

92 URANIUM 236 NEUTRON FISSION CROSS <strong>SEC</strong>TION<br />

o£2LS£ 1 5o 0 MEV Ac MICHAUDON BRC<br />

0: EVALUATION MAY BE SUF=ICIENTo<br />

652380 4o OC MEV 10C 0 MEV HcGERWIN<br />

212062 5 00c EV 15o 0 MEV J c Yc EARRE CAD<br />

0: WANTED RELATIVE TO U-235 FISSION CROSS <strong>SEC</strong>TIONo<br />

0: FOR FAST REACTOR CALCULATIONSc<br />

215013 100c 5o 00 MEV<br />

MoNcNIKOL AEV<br />

FEI<br />

0:<br />

M:<br />

RATIO WANTED RELATIVE TO U-235o<br />

AVERAGE CS IN FISSION NEUTRON SPECTRUM OF CF-252<br />

TIMES NU-BAR OF CF-252 WOULD BE VERY USEFUL<br />

(REQUIRED ACCURACY 1 PERCENT >c<br />

SEE GENERAL COMMENTS IN THE IN TROOUC TI ONo<br />

SUBSTANTIAL MODIFICATIONSo<br />

STA TUS<br />

LAS CRAMER* - LA-4 4 20 ( 1970). CATA 35 EV TO 2o9 MEVc<br />

ORL RCSLER+ - LSNOC-1 148(1972), WORK IN PROGRESS 500 KEV TO 8 MEVc<br />

GEL THEOBALD* - cANCC(E)-157 (1573), IN PROGRESS IN SUBTHRESHOLD REGIONc<br />

92 URANIUM 236 NEUTRON NEUTRONS EMITTED PER FISSION (NU BAR)<br />

212C62 5C0o 1 5O 0 MEV JoYcEARRE<br />

A: ACCURACY RELATIVE TO NU CF-252o<br />

o: FOR FAST REACTOR CALCULATIONSo<br />

214014<br />

5o 00 MEV CCP McNcNIKOLAEV FEI<br />

0: SEE GENERAL COMMENTS IN THE INTRODUCTION<br />

STATUS<br />

GA CARLSON* - NP/A 141 577( 1570), <strong>DATA</strong> THERMAL TO 20 KEV.-<br />

GEL ROHR+ - EAN<strong>DC</strong>(E)-157 (1973). IN PROGRESS 5 EV TO 2 KEVo<br />

SGA EDER+ - 73 PARIS PAPER 12. COMPILATICNo<br />

HAR CABELL* - AERE-R-6761 ( 1 971 >c THEHMALo<br />

SRL BAUMANN+ - NSE 32 265(1968). 8 PERCENT AT THERMALo<br />

STATUS-<br />

IAE MANERO* - REA 10 637(1972). REVIEW,<br />

92 URANIUM 236 NEUTRON RESONANCE PARAMETERS<br />

214011 1 Co 0 EV 5o00 KEV 2 CCP McNoNIKOLAEV FEI<br />

Q: NEUTRON AND CAPTURE WIDTHS WANTED FOR EVALUATION<br />

OF SELFSHIEL DING IN RESOLVED RESONANCE REGIONc<br />

A: OBSERVATION OF AT LEAST 50 PERCENT OF P-WAVE<br />

RESONANCES IN THE ENERGY INTERVAL TO 1 KEV IS<br />

OESIREOo<br />

0: SEE GENERAL COMMENTS IN THE INTRODUCTION<br />

STATISTICAL ANALYSIS OF MEASURED<br />

RESONANCE PARAMETERS WANTED©<br />

AVERAGE S AND P WAVE RESONANCE PARAMETERS SHOULD<br />

BS DERIVED,<br />

M: SUBSTANTIAL MODIFICATIONSo<br />

STATUS<br />

STATUS<br />

GEL CAFRARO* - 72 EUDAPEST 200. 39 RESCNANCESo<br />

GEL THEOBALD* - EANOC(E)-157 (1973), IN PROGRESSc<br />

92 URANIUM 237 NEUTRON CAPTUREE CRoSS licTION<br />

242380 1o 00 KEV 3,00 MEV 20o OX 1 FR AoMICHAUDON BRC<br />

0: EVALUATION MAY BE SUFFICIENTc<br />

92 URANIUM 237 NEUTRON FISSION CROSS <strong>SEC</strong>TION<br />

242025 lo 00 KEV 15o 0 MEV 20o0X 1 FR Ac MICHAUDON BRC<br />

O: EVALUATION MAY BE SUFFICIENTo<br />

STATUS<br />

STATUS<br />

USA USN<strong>DC</strong>o TECHNICALLY VERY DIFFICULT OR IMPOSSIBLE AT PRESENTo<br />

LAS MC NALLY* - PR/C 9 717(1974), <strong>DATA</strong> 43 TO 1000 EV AND Oo1 TO 2 MEV FROM <strong>NUCLEAR</strong> EXPLOSION(POMMARD)<br />

92 URANIUM 238 NEUTRON TOTAL CROSS <strong>SEC</strong>TION<br />

212065 5C0o EV 15o0 MEV loOX 2 FR JoYoBARRE CAD<br />

0: FOR FAST REACTOR CALCULATIONSo<br />

FISSION LIST PAGE 1 lo 83

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