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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28 NICKEL 56 NEUTRCN N.NF<br />
652136 1 So 0 MEV lOoOX 2 FR #0M ICHAUDON BRC<br />
Q: PRODUCTION OF CO-57 (270 DAY) THROUGH<br />
SIGMA(N.NP)+SIGMA(N,D)o<br />
0: ACTIVATION OETECTORc<br />
CIRCUIT ACT I VATIONo<br />
DISAGREEMENT BETWEEN JERONYMO(SACLAY) AND OTHERSo<br />
28 NICKEL 58 NEUTRCN N.ALPHA<br />
652.135 14o 0 MEV 2 GER Be GOEL KFK<br />
A: ACCURACY REQUIRED TO BETTER THAN 20o PERCENTo<br />
0: VERIFICATION OF EVAPORATION THEORY CALCULATIONSo<br />
STATUS<br />
STATUS<br />
N<strong>DC</strong> SCHETT+ - EAN<strong>DC</strong>-S5 (1974) , CCMPILATICN OF EXPERIMENTAL <strong>DATA</strong> AVAILABLE AS OF JANUARY 1974c<br />
28 NICKEL 58 NEUTRON RESONANCE PARAMETERS<br />
241.056 100c KEV lOoOX 2 USA FoGoPEREY ORL<br />
PoBohEMMIG<br />
AEC<br />
Co Ec TILL<br />
ANL<br />
O: ENERGY REQUESTED IS A MAXIMUM VALUE ONLYo<br />
NEUTRON WIDTH. GAMMA WIDTH. SPIN AND PARITY<br />
WANTEOo<br />
M: NEW REQUESTc<br />
STATUS<br />
STATUS<br />
ORL HALPERINo - MEASUREMENTS PLANNED FOR 1975o<br />
28 NICKEL 59 _ NEUTRCN _ N,ALPHA<br />
242523 2Eo3 MV 500o EV 20o0X 2 BLC NoMAENE MOL<br />
A: EVEN AN ACCURACY OF 50 PERCENT WOULD BE USEFULo<br />
0: EVALUATION OF HE PRODUCTION IN STEEL IN HIGH FLUX<br />
REACTORS THROUGH THE REACTION CHAIN<br />
N1-58(N . GAMMA>NI-59(N,ALPHA)FE-56o<br />
STATUS<br />
STATUS<br />
MOL MAENE - ThEORETICAL EVALUATION OF THERMAL CROSS <strong>SEC</strong>TION BY KIROUAC (NSE <strong>46</strong> 427) YIELDS 30 BARNS.<br />
TO BE COMPARED WITH A VALUE OF 11 EARNS DEDUCED BY WEITMAN FROM ANOMALOUS HELIUM PRODUCTION<br />
RATE IN STEEL IRRADIATED IN A FILE SPECTRUMo<br />
28 NICKEL 60 _ NEUTRON _ N,P<br />
652132 15c 0 MEV lOoOX 2 FR Ao MICHAUDON BRC<br />
Q: PRODUCTION OF C0-60 (5c 3 YEAR) o<br />
0: ACTIVATION OETECTORo<br />
28 NICKEL 60 _ NEUTRCN N.ALPHA<br />
6S2l3£ 14o 0 MEV 2 GER BoGOEL KFK<br />
A: ACCURACY REQUIRED TO BETTER THAN 20o PERCENTo<br />
0: VERIFICATION OF EVAPORATION THEORY CALCULATIONSo<br />
28^NICKEL 60 NEUTRON _ RESONANCE PARAMETERS<br />
131S5S lOOo KEV lOoOX 2 USA FoGoPEREY ORL<br />
PoBohEMMIG<br />
AEC<br />
CoEcTILL<br />
ANL<br />
Q: ENERGY REQUESTED IS A MAXIMUM VALUE ONLYo<br />
NEUTRON WIDTH. GAMMA WIDTH, SPIN AND PARITY<br />
WANTEDo<br />
M: NEW REQUESTc<br />
STATUS<br />
STATUS<br />
ORL HALPERIN* - MEASUREMENTS PLANNED FOR 1975o<br />
28 NICKEL 61 NEUTRCN RESCNANCE'PARAMETERS<br />
651125 lo 00 KEV 600o KEV 9,OX 1 USA ROEHRLICH KAP<br />
Q: NEUTRON *IDTh NEEDEDo<br />
241062 1 OOo KEV lOoOX 3 USA FoGoPEREY ORL<br />
PoBohEMMIG<br />
AEC<br />
CoEoTILL<br />
ANL<br />
Q: ENERGY REQUESTED IS A MAXIMUM VALUE ONLYc<br />
NEUTRON WIDTH, GAMMA WIDTH, SPIN AND PARITY<br />
WANTEOo<br />
M: NEW REQUESTo<br />
FISSION LIST PAGE 26