INDC(SEC)-46/U+R+F+SIN DC INTERNATIONAL NUCLEAR DATA ...
INDC(SEC)-46/U+R+F+SIN DC INTERNATIONAL NUCLEAR DATA ...
INDC(SEC)-46/U+R+F+SIN DC INTERNATIONAL NUCLEAR DATA ...
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92 URANIUM 235 NEUTRON ENERGY CIFFcRENTIAL INELASTIC CROSS <strong>SEC</strong>TION (CONTINUEDI<br />
STATUS<br />
STATUS<br />
GEL KNITTER* - ZP 257 108(1972). <strong>DATA</strong> 1=5 TO 2o3 MEVc<br />
LRL KAMMERDIENER - UCRL-51232 (1972), <strong>DATA</strong> AT 14 MEVo<br />
ALD SATCHELOR+ - A taRE/0-55/69, <strong>DATA</strong> 2 TO 4 MEV;<br />
ANL GUENTHER+ - USNCC-11 25(1974), EXPERIMENTAL AND THEORETICAL WORK IN PROGRESS TO 4 MEVc<br />
92 URANIUM 235 ' NEUTRON DOUBLE DIFFERENTIAL INELASTIC CROSS <strong>SEC</strong>TION<br />
652052 1 3o 0 KEV lOoC MEV lOoOX 1 JAP He MATSUNOBU SAE<br />
O: CROSS <strong>SEC</strong>TIONS FOR EXCITATION OF INDIVIDUAL LEVELS<br />
ALSO WANTEDo<br />
A: ENERGY RESOLUTION 1 TO 2 PERCENT DESIREDo<br />
O: FOR FAST REACTORSo<br />
FOR EVALUATION OF <strong>NUCLEAR</strong> <strong>DATA</strong>o<br />
NO EXPERIMENTAL <strong>DATA</strong> ABOVE 7o5 MEVc<br />
M: SUBSTANTIAL MODIFICATIONSo<br />
653052 3 OOo KEV 1 Oo 0 MEV lOoOX 1 BAN MoMc ISLAM RAM<br />
O: FOR FAST REACTORSc<br />
.742071 1 5o 0 MEV 20 o 0 X 2 FR AoMICHAUDON BRC<br />
0: FOR CRITICAL ASSEMBLIESc<br />
92URANILM235 _ NEUTRCN TOTAL SCATTERING_CROSS <strong>SEC</strong>TJON_<br />
752026 1o 00 KEV 1Oo 0 MEV 2o OX 1 JAP He MATSUNOBU SAE<br />
A: ENERGY RESOLUTION - 1 TO 2 PERCENTo<br />
o: EVALUATION OF U-235 <strong>NUCLEAR</strong> <strong>DATA</strong> AND FOR REACTOR<br />
DESIGN CALCULATIONSo<br />
THE EXPERIMENTAL <strong>DATA</strong> ARE VERY POORo<br />
NO EXPERIMENTAL <strong>DATA</strong> FROM 5o5 MEV TO 10 MEVo<br />
M: NEW REOUESTc<br />
92 URANIUM 235 NEUTRCN DIFFERENTIAL TOTAL SCATTERING CROSS <strong>SEC</strong>TION<br />
252027 1o 00 KEV 1Oo 0 MEV 1 JAP He MATSUNOBU SAE<br />
A: ACCURACY REQUIRED - 2 TO 5 PERCENTo<br />
ENERGY RESOLUTION - 1 TO 2 PERCENTo<br />
o: EVALUATION OF U-235 <strong>NUCLEAR</strong> <strong>DATA</strong> AND FOR REACTOR<br />
DESIGN CALCULATIONSo<br />
THE EXPERIMENTAL <strong>DATA</strong> ARE VERY POORo<br />
NO EXPERIMENTAL <strong>DATA</strong> FROM 5o 5 MEV TO 10 MEVo<br />
Ml NEW REQUEST.;<br />
92 URANIUM 235 NEUTRON NCN-ELASTIC CROSS <strong>SEC</strong>TION<br />
652561 1 So 0 MEV 5 FoWELLER KFK<br />
A: ACCURACY 10 PERCENT REQUIRED TO lo 5 MEV AND 20<br />
PERCENT ABOVEc<br />
ENERGY RESOLUTION ABOUT 100 KEVo<br />
655051 1 00c KEV lOoO MEV lOoOX BAN MoMoISLAM RAM<br />
O: FOR FAST REACTORSc<br />
92 URANIUM 235 NEUTRON CAPTURE CROSS <strong>SEC</strong>TION<br />
662055 1o 00 KEV 1 Oo 0 MEV JAP Sc KATSURA GI<br />
HoMATSUNOBU<br />
JAE<br />
SAE<br />
0: ALPHA ALSO WANTEOo<br />
A: REQUIRED ACCURACY -<br />
RESOLUT ION - 1 TO 2<br />
O: FOR FAST REACTORSc<br />
<strong>NUCLEAR</strong> <strong>DATA</strong> EVALUATIONc<br />
5 TO 10 PEPCENTo<br />
PERCENTo<br />
NO EXPERIMENTAL <strong>DATA</strong> ABOVE 2<br />
M: SUBSTANTIAL MODIFICATIONSo<br />
652576 1 Oo 0 KEV lOoO MEV<br />
A: ACCURACY TO OBTAIN 1 PERCENT IN ALPHAo<br />
o: ANALYSIS OF CRITICAL EXPERIMENTSo<br />
653060 3Oo 0 KEV BAN MoMoISLAM RAM<br />
0: FOR FAST REACTORSc<br />
241112 1o 00 MV lo 00 EV A NoSTEEN BET<br />
Q: SHAPE ESPECIALLY IMPORTANT AT LOW ENERGYo<br />
M: NEW REQUESTO<br />
242005 200o EV SOOo KEV SWD HoHAEGGBLOM AE<br />
O: FAST REACTOR CALCULATIONSo<br />
242028 3o 00 MEV FR AoMICHAUDON BRC<br />
0: FOR CRITICAL ASSEMBLIESc<br />
FISSION LIST PAGE IIo 69
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