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

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95 AMERICIUM 241<br />

GAMMA<br />

FISSICN PRODUCT MASS VI ELD SPECTRUM ( CONTINUED)<br />

722051 HoOKASHITA JAE<br />

0: FISSION YIELD OF SM-152, AND SM-153 WANTEDo<br />

<strong>DATA</strong> WANTED FOR THERMAL NEUTRONS. FAST REACTOR<br />

NEUTRONS(80-800 KEV). FISSION SPECTRUM NEUTRONS<br />

AND HIGH ENERGY NEUTRONS(1 A-15 ME V)o<br />

0: FOR BURN UP CALCULATION FROM DESTRUCTIVE AND<br />

NON-DESTRUCTIVE CALCULATIONSo<br />

M: NEW REOUESTo<br />

STATUS-<br />

K UR<br />

MILLER* - SJA 27 281(1568)o<br />

-STATUS<br />

SRE<br />

CCP<br />

AE<br />

CCP<br />

S GA<br />

HAR<br />

GRE<br />

CRC<br />

GEV<br />

ANL<br />

HILLER - KT 12 <strong>46</strong>5(19701<br />

GRECHUSHKINA - TABLES SHOWING THE COMPOSITION OF PROMPT FISSION PRODUCTS FROM U-235, U-238, AND<br />

PU—239 FISSICN, ATOM1ZDAT, MOSCOW(1964),<br />

FORSYTH* - 70 KARLSRUHE VCLol Po521,<br />

G USE V - PROTECTION AGAINST GAMMA RADIATION FROM FISSION PRODUCTS, ATOMIZDAT, MOSCOW( 1 968)c<br />

LAMMER* - 73 PARIS PAPER 13, EVALUATION<br />

CROUCH - 73 PARIS PAPER 94, EVALUATION,<br />

DEVILLERS+ - 73 PARIS PAPER 63, EVALUATION;<br />

WALKER - 73 PARIS PAPER 34, EVALUATION,<br />

MEEK + - NE00-12154, EVALUATION,<br />

GLENDENIN+ - WORK IN PROGRESSo<br />

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

722540<br />

1 4o 0 MEV YcNAITO JAE<br />

A: ACCURACY REQUIRED AT THERMAL IS 3 PERCENT, 10<br />

PERCENT ABOVE,<br />

0: FOR BURN UP CALCULATION OF A PU LOADED THERMAL<br />

REACTOR,<br />

M: NEW REQUESTC<br />

-STATUS<br />

GA<br />

GEL<br />

S GA<br />

HAR<br />

SRL<br />

CARLSON+ - NP/A 141 577( 1970). <strong>DATA</strong> THERMAL TO 20 KEVc<br />

ROHR+ - EANCCI El-157 ( 1973). IN PROGRESS 5 EV TO 2 KEV.;<br />

EDER* - 73 PARIS PAPER 12, COMPILATION,<br />

CABELL* - AERE-R-6761(1971), THERMAL,<br />

BAUMANN+ - NSE 32 265(19681. 8 PERCENT AT THERMALo<br />

9 2 URANIUM 236 NEUTRON DELAYED NEUTRONS EMITTED PER FISSION<br />

701032 3,00 MEV 10,OX Ro Bo WALTON<br />

Q: ALSO FOR 14 MEV, NEUTRONS,<br />

0: BACKGROUND CORRECTION IN U- 235 SPENT FUEL ASSAYo<br />

92 URANIUM 236 ENERGY SPECTRUM OF FISSION NEUTRONS<br />

201031 lOoOX USA Rc B;WALTON LAS<br />

0: ONE ENERGY ABOVE FISSION THRESHOLD,<br />

0: BACKGROUND CORRECTIONS IN U-235 SPENT FUEL ASSAYo<br />

92 URANIUM 238 NEUTRON DELAYED NEUTRONS EMITTED PER FISSION<br />

201035 So 00 MEV 14o 0 MEV<br />

A Ro Be WALTON LAS<br />

o: <strong>DATA</strong> DESIRED FOR EXTRAPOLATION TO IS MEVo<br />

CALCULATIONS OF MODERATING ASSEMBLIES FOR U ASSAYo<br />

STATUS<br />

A 1<br />

HFA<br />

IAE<br />

LAS<br />

ANL<br />

ALD<br />

TUTTLEo - NSE 56 37(1975), REVIEW WITH RECOMMENCED VALUESc<br />

SHALEV+ - NSE 51 52(1973), FAST REACTOR SPECTRUMc<br />

MANERO+ - REA 10 637(1972), REVIEW Ool TO 15 MEV,<br />

EVANS* - USNOC-3 127(1972), REVISED <strong>DATA</strong> AT 3o1 AND IS MEV,<br />

COXo ANL/NDM-=(1974)o MEASUREMENT AND EVALUATION, 2 TO 15 MEV,<br />

MCTAGGART - EAN<strong>DC</strong>(UK)-151(1973) , FAST REACTOR SPEC MEASUREMENT IN PROGRESS,<br />

92 URANIUM 238 NEUTRON FISSION PRODUCT MASS YIELD SPECTRUM<br />

222.052 1 o 0 X HoOKASHITA JAE<br />

FISSION YIELD OF RU-106. XE-133. SM-152, SM-153.<br />

CE 141, CE—144. ND-143, ND-144. ND-145, ND-1<strong>46</strong>,<br />

NO—147. ND-148, ND-150 AND CS-137 WANTEOo<br />

<strong>DATA</strong> WANTED FOR FISSION SPECTRUM NEUTRONS AND<br />

HIGH ENERGY NEUTR0NS(14 - 15 MEVIo<br />

FOR BURN UP CALCULATION FROM DESTRUCTIVE AND<br />

NON-DESTRUCTIVE MEASUREMENTo<br />

NEW REQUESTo<br />

SAFEGUARDS LIST PAGE IV o 8

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