ENTRY V0029 20110131 V028V002900000001 SUBENT V0029001 20110131 V028V002900100001 BIB 9 303 V002900100002 TITLE A simultaneous evaluation of some important cross- V002900100003 sections at 14.70 MeV - Al27(n,a), Fe56(n,p), V002900100004 Cu63(n,2n), Cu65(n,2n), Au197(n,2n), Nb93(n,2n), V002900100005 S32(n,p) and h1(n,n) V002900100006 AUTHOR (J.G.Hayes, T.B.Ryves) V002900100007 INSTITUTE (2UK NPL) V002900100008 REFERENCE (J,ANE,8,469,1981) V002900100009 MONITOR The results are normalized to the associated particle V002900100010 measurements. V002900100011 METHOD Method of weighted least-squares was used in the V002900100012 evaluation. V002900100013 ** Principal points of this evaluation V002900100014 (1.) Simultaneous evaluations, in which a group of V002900100015 cross-sections are considered, together with their V002900100016 correlation. V002900100017 (2.) Ratio of cross sections is employed to avoid the V002900100018 absolute measurement of neutron fluence rate. V002900100019 All activation cross-sections are in fact measured asV002900100020 ratios relative to some monitor (standard) cross- V002900100021 sections. All results were firstly adjusted to a V002900100022 neutron energy of 14.70 MeV. V002900100023 (3.) The cross-sections are determined in a known V002900100024 neutron fluence which may be determined either by a V002900100025 proton recoil telescope, or by a plastic scintillatorV002900100026 or by the associated particle technique (in case of V002900100027 D-T neutron source). The associated particle V002900100028 technique is absolute. V002900100029 (4.) The mathematical treatment follows that of Hayes V002900100030 and Axton, Metrologia 6(1969)21. V002900100031 ** Results V002900100032 The results are mostly in agreement within the errors V002900100033 with several other evaluation. V002900100034 The ENDF/B-V ratio of the 2 most commonly used V002900100035 standard cross-sections, Al-27(n,a) and Fe-56(n,p), V002900100036 was 7.5% higher than the ratio of this results. V002900100037 ** Selection of papers V002900100038 About 70 from more than 100 original papers on V002900100039 activation cross section measurement around 14 MeV V002900100040 have been included in the evaluation(except H(n,n)H).V002900100041 Nearly all papers prior to 1960 were arbitrarily V002900100042 excluded. The following tables shows the out-lines V002900100043 of the data selection, correlation and the results. V002900100044 (All reference abbreviations are explained in each V002900100045 subentries.) V002900100046 The cross-section data are given as follows, V002900100047 ------------------------------------------------------ V002900100048 Reaction Code T(1/2) Assumed shape V002900100049 No. (14.1-14.9 MeV) V002900100050 ------------------------------------------------------ V002900100051 Al27(n,a)Na24 2 15.03H Vonach+(1970) V002900100052 Fe56(n,p)Mn56 3 2.579H -13.3MB/(MEV) V002900100053 Cu63(n,2n)Cu62 4 9.74M Simons+(1970) V002900100054 Cu65(n,2n)Cu64 5 12.701H Mannhart+(1975) V002900100055 Au197(n,2n)Au196 6 6.183D flat V002900100056 Nb93(n,2n)Nb92m 7 10.15D flat V002900100057 S32(n,p)P32 8 14.28D -48MB/(MEV). V002900100058 H1(n,n)H1 9 --- Gammel (1963) V002900100059 Associated ----- V002900100060 particle V002900100061 ------------------------------------------------------ V002900100062 ** The cross-section ratios used in this evaluation V002900100063 (Detail of reference-name is given in each subentry, V002900100064 code no.of reaction cross-section is above-mentioned. V002900100065 Ratios relative to monitor (standard) cross-sections V002900100066 References (percent uncertainties in parentheses) V002900100067 -------------------------------------------------------V002900100068 Code No 1 2 3 4 5 6 7 8 9 Note V002900100069 -------------------------------------------------------V002900100070 57AL1 - - - - - - 220 - S V002900100071 (5) V002900100072 78AN1 S - - - 19.72 - - - - V002900100073 (6.9) V002900100074 64AR1 104 - - - - - - - S (A) V002900100075 (2.3) V002900100076 69BA2 S 0.936 - - - - - - - (A,I)V002900100077 (3) V002900100078 69BA1 S 0.943 - 8.12 17.5 - 1.767 - - V002900100079 (4) (6) (5) (5) V002900100080 75BA1 S - - - 19.16 - - - - V002900100081 (2.9) V002900100082 62BO1 - S 5.58 10.23 - - - - - V002900100083 61PO1 (7.7) (7.6) V002900100084 70BO1 - - - - - 0.742 - S - V002900100085 (5.9) V002900100086 69BO1 111.6 - - - - - - - S V002900100087 (4) V002900100088 63BU1 0.524 0.494 - 4.81 - 2.01 S - - V002900100089 63SA1 (4.2) (4) (3) (4.2) V002900100090 64SA1 V002900100091 65SA1 V002900100092 74SA1 V002900100093 69CR1 121 - 603 1033 - - - - S V002900100094 (5) (4.6) (5.6) V002900100095 68CU1 0.125 0.112 - S - - - - - V002900100096 (9) (7) V002900100097 60DE1 - - 0.846 - - - - S - V002900100098 (5) V002900100099 68DI1 S - - - 20.81 - - - - V002900100100 (3.9) V002900100101 62GA1 0.172 0.158 - - - - - S - V002900100102 (10) (9.3) V002900100103 62GL1 - - S - - 0.901 - - - V002900100104 (8.5) V002900100105 62GL2 - - S 1.87 - - - - - (A) V002900100106 (2) V002900100107 65GR1 - - 554 - - - - - S (B) V002900100108 (2.2) V002900100109 79LU1 116.3 - - - - - - - S V002900100110 (2.6) V002900100111 66HE1 1.074 S - - - - 2.29 - - (C) V002900100112 63HE1 (2) (6) V002900100113 78HU1 S - - - - 4.43 - - - V002900100114 (7.7) V002900100115 70HU1 - S - - - 4.25 - - - V002900100116 (6.7) V002900100117 76HU1 - 108.8 - - - - - - S (D) V002900100118 (0.79) V002900100119 64LE1 - - 564 - - - - - S (E) V002900100120 (10) V002900100121 69LE1 - 0.1046 - S - - 0.229 - - V002900100122 (3) (13) V002900100123 65LI1 - 0.1689 - - - - - S - (D) V002900100124 74LI1 (0.93) V002900100125 75LI1 V002900100126 65PA1 0.1845 - 0.976 1.61 3.01 0.655 - S - (F) V002900100127 65LI1 (5.7) (6.9) (6.9) (5.4) (4.8) V002900100128 65PA2 V002900100129 70PA1 V002900100130 75PA1 V002900100131 74MA1 - - - S 2.17 - - - - V002900100132 (7) V002900100133 67MI1 0.235 - S - - - - - - V002900100134 (7.7) V002900100135 72MO1 S - 4.06 8.75 - - - - - (E) V002900100136 (3.5) (3) V002900100137 65NA1 - S - 8.98 - - - - - V002900100138 (8) V002900100139 72NE1 S - - - 18.93 4.06 - - - V002900100140 78NE1 (4.6) (2.8) V002900100141 64BO1 112.0 105.0 511 1036 - - 215 - S V002900100142 67PA1(3.6) (4.8) (3) (3.5) (2.8) V002900100143 61PR1 116.4 - - 989 2380 - - - S (G) V002900100144 61BA1 (5) (6.3) (8.9) V002900100145 72QU1 S - - 8.12 18.73 4.23 - - - (K) V002900100146 71QU1 (4.1) (10.3)(7.5) V002900100147 66RI1 S - - - - 3.97 - - - V002900100148 (5) V002900100149 73RO1 1.069 S - 9.80 - - 1.985 6.04 - (B,H)V002900100150 73RO2(0.63) (1.7) (1.2) (0.63) V002900100151 78RY1 1.040 S 5.01 8.89 19.83 4.14 - 6.15 - V002900100152 78RY2(0.77) (1.2) (1.1) (3) (2.4) (0.77) V002900100153 81RY1 V002900100154 81RY2 V002900100155 61SA1 - - 549 - - - - - S V002900100156 (4.5) V002900100157 71SA1 112.7 - - - - - - - S V002900100158 (8) V002900100159 70SC1 S - - - - - 2.018 - - V002900100160 (5.3) V002900100161 74SH1 - 111.5 - - - - - - S (D) V002900100162 77RA1 (1.2) V002900100163 62ST1 1.039 S - - - - - - - (J) V002900100164 (2.7) V002900100165 79SW1 113.5 - - - - - - - S V002900100166 (1.6) V002900100167 77TE1 - 110.8 - - - - - - S (D) V002900100168 77KU1 (1.05) V002900100169 81TH1 - - - - - - - 658.5 S V002900100170 (1.4) V002900100171 66VA1 S - - - - 4.05 - - - V002900100172 (5) V002900100173 70VO1 112.0 - - - - - - - S V002900100174 (0.6) V002900100175 68VO1 S 0.897 - 8.17 19.3 - - - - V002900100176 75MA1 (1.7) (0.84) (1.6) V002900100177 60WE1 - - S 2.02 - - - - - V002900100178 (8.4) V002900100179 81WI1 111.1 - - - - - - - S V002900100180 (0.9) V002900100181 -------------------------------------------------------V002900100182 Notes V002900100183 A. H result excluded. V002900100184 B. E(n)=14.70 MeV, not as quoted in the paper V002900100185 C. Associated particle result excluded. V002900100186 D. See Ryves and Axton.Proc.Knoxville Conf.(1979)980.V002900100187 E. half-life not given. V002900100188 F. Fe result superseded. V002900100189 G. Uncertainty not given. V002900100190 H. H result corrected for use of relativistic V002900100191 kinematics. Fe result corrected for foil counting,V002900100192 1+K=1.016. V002900100193 I. S result excluded. V002900100194 J. Nb result excluded. V002900100195 K. Cu-63 result excluded,because rel to Al(n,p) by V002900100196 S.M.Qaim (priv.comm.1981). V002900100197 For H(n,w)H from proton recoil telescope measurements V002900100198 before 1973, a correction of 2.8% was made (see V002900100199 Thomas and Axton,Nucl.Instrum.Meth.174(1980)321). V002900100200 Cu-62 half-life was corrected to 9.74m. Cu-64 branch- V002900100201 ing ratios of I(beta+)=17.9%. and I(beta-)=37.1% V002900100202 were used, except for Ryves et al.,Metrologia 14 V002900100203 (1978)127. Nb and Au corrections have been discussed V002900100204 by Philis et al.,CEA-R-4676(1976),CEA-R-4826(1977). V002900100205 ** Following activation measurements (since 1960) are V002900100206 excluded from evaluation. (Detail of references is V002900100207 given in each subentry. Reaction (monitor) code is V002900100208 same as before. V002900100209 -------------------------------------------------------V002900100210 Reference Measured Standard Unc. Comments V002900100211 reac. (MONIT) (%) V002900100212 -------------------------------------------------------V002900100213 Basu+(1966) 6 Q 8. Few details V002900100214 Bormann+(1963) 4 1 Q Graphical result V002900100215 Bormann+(1969) 3,4 PL 7. Cu63 result high V002900100216 Bramlitt+(1962) 6 1 18. Large error V002900100217 Carter(1966) 6 Q Q No details V002900100218 Cevolani+(1962) 3 9 7. Cu62 half-life 10.1m V002900100219 Chatterjee+(1967) 3 PL 10. Few details V002900100220 Chittenden+(1961) 2 1,3 10. Result high V002900100221 Cross+(1962) 2 1 10. Result low V002900100222 Csikai+(1963) 1 LN Q ------- V002900100223 Depraz+(1960) 1,2,4 3 8-12. Results divergent V002900100224 Dressler+(1978) 1 2 5. Ratio high V002900100225 Dyer+(1972) 2 SINP 9. E(n) low: Q V002900100226 Ferguson+(1960) 3 LINT 9. Result low V002900100227 Garg(1979) 2 3 10. Result high V002900100228 Hankla+(1972) 5 1,2 8. E(n) above Au(n,3n) V002900100229 threshold 14.8 MeV:QV002900100230 Jeronymo+(1963) 1 PL 10. Large error V002900100231 Lebowitz+(1970) 1 FN2N 18. ------- V002900100232 Levkovskii(1964) 7 Q 18. Summary account V002900100233 Liskien+(1965) 2 TL 6. Superseded Liskien'79V002900100234 Lu Wen-Deh+(1970) 6 2 5. Result high V002900100235 McCrary+(1960) 3,4 Q 10. Result high, V002900100236 see Bychkov+(1980) V002900100237 Molla+(1977) 2 1,ASNN 7. Result low V002900100238 Rayburn(1961) 4 3 8. Cu64 half-life 13.6m V002900100239 Schmitt+(1961) 1 UNF 7. ------- V002900100240 Singh(1970) 2 Q Q Summary. Result high V002900100241 Strain+(1965) 4 1,3 Q ------- V002900100242 Strohal+(1962) 6 2 6. Result low V002900100243 Tewes+(1960) 1,5,6 TL 20. Large error V002900100244 Vonach+(1959) 6 1 15. Large error V002900100245 -------------------------------------------------------V002900100246 Notes V002900100247 Q. Question or questionable V002900100248 PL Plastic counter V002900100249 TL Telescope V002900100250 LN Long counter V002900100251 SINP Si28(n,p) V002900100252 LINT Li6(n,t) V002900100253 FN2N F(n,2n) V002900100254 ASNN As(n,2n) V002900100255 UNF U238(n,f) V002900100256 ** The distribution of ratio measurements in the V002900100257 evaluation is given as follows, (the code of reaction V002900100258 cross-section is same as before.) V002900100259 -------------------------------------------------------V002900100260 x-section 1 2 3 4 5 6 7 8 9 V002900100261 -------------------------------------------------------V002900100262 1 7. 2. 5. 7. 5. 3. 2. 10.V002900100263 2 2. 5. 1. 2. 3. 4. 4.V002900100264 3 2. 0. 1. 0. 2. 5.V002900100265 4 1. 0. 2. 1. 3.V002900100266 5 0. 0. 1. 1.V002900100267 6 1. 2. 0.V002900100268 7 0. 2.V002900100269 8 1.V002900100270 9 - V002900100271 -------------------------------------------------------V002900100272 ** The results of this evaluation at 14.70 MeV and the V002900100273 variance-covariance matrix for the results are as V002900100274 follows, (variances given in (%)**2 .) V002900100275 -------------------------------------------------------V002900100276 Reaction Code x-sec Unc.(%) V002900100277 No. (MB) Least-sq. Syst. Total V002900100278 -------------------------------------------------------V002900100279 Al27(n,a)Na24 1 113.3 0.6 0.6 V002900100280 Fe56(n,p)Mn56 2 108.1 0.6 0.6 V002900100281 Cu63(n,2n)Cu62 3 544. 1.3 0.2 1.3 V002900100282 Cu65(n,2n)Cu64 4 986. 1.2 +1.0 +1.6 V002900100283 -2.5 -2.8 V002900100284 Au197(n,2n)Au196 5 2164. 1.7 0.1 1.7 V002900100285 Nb93(n,2n)Nb92m 6 449. 1.9 1.9 V002900100286 S32(n,p)P32 7 215. 1.4 1.4 V002900100287 H1(n,n)H1 8 653. 0.8 1.0 1.3 V002900100288 -------------------------------------------------------V002900100289 Variance-covariance matrix V002900100290 -------------------------------------------------------V002900100291 Al27(n,a)Na24 0.32 0.19 0.16 0.19 0.30 0.26 0.21 0.19V002900100292 Fe56(n,p)Mn56 0.36 0.24 0.27 0.22 0.26 0.27 0.31V002900100293 Cu63(n,2n)Cu62 1.65 0.86 0.18 0.25 0.34 0.27V002900100294 Cu65(n,2n)Cu64 1.60 0.22 0.32 0.39 0.26V002900100295 Au197(n,2n)Au196 2.82 0.50 0.23 0.21V002900100296 Nb93(n,2n)Nb92m 3.60 0.31 0.26V002900100297 S32(n,p)P32 2.12 0.23V002900100298 H1(n,n)H1 0.64V002900100299 -------------------------------------------------------V002900100300 ERR-ANALYS 1 sigma uncertainties are given. V002900100301 STATUS (TABLE) Table 6 of J,ANE,8,469,1981 V002900100302 HISTORY (19820129C) KO. V002900100303 (19871116A) DG. Superseded by EXFOR V0043 V002900100304 (20110131U) On. Upper to lower cases, 4 digits year V002900100305 ENDBIB 303 0 V002900100306 COMMON 1 3 V002900100307 EN V002900100308 MEV V002900100309 14.70 V002900100310 ENDCOMMON 3 0 V002900100311 ENDSUBENT 310 0 V002900199999 SUBENT V0029002 20110131 V028V002900200001 BIB 5 42 V002900200002 REACTION (13-AL-27(N,A)11-NA-24,,SIG,,,EVAL) V002900200003 REL-REF (E,80078002,P.M.Aron+,J,AE,16,370,1964) =78AR1V002900200004 (E,21250002,P.Boschung+,J,HPA,42,252,196904) =69BO1V002900200005 (E,11457007,J.Butler+,J,CJP,41,372,1963) =63BU1V002900200006 (E,20930005,D.Crumpton+,J,JIN,31,1,196901) =69CR1V002900200007 (E,20890003,P.Cuzzocrea+,J,NC/B,54,53,196803) =68CU1V002900200008 (E,11494003,F.Gabbard+,J,PR,128,1276,1962) =62GA1V002900200009 (E,30523001,Lu Han-Lin+,J,PHE,3,(1),88,197901) =79LU1V002900200010 in the text,the author's name is inversely taken. V002900200011 (E,21372002,J.D.Hemmingway+,J,PRS/A,292,180,1966)=66HE1V002900200012 (E,20378003,A.Paulsen+,J,JNE/AB,19,907,196511) =65PA1V002900200013 (E,21345002,B.Minetti+,J,ZP,199,275,196701) =67MI1V002900200014 (E,20888002,G.C.Bonazzola+,J,NP,51,337,196402) =64BO1V002900200015 (E,11462002,B.P.Bayhurst+,J,JIN,23,173,1961) =61BA1V002900200016 in the Ref.of the text 61BA1 is dropped. V002900200017 (E,20798002,J.C.Robertson+,J,JNE,27,139,197303) =73RO1V002900200018 (E,,J.C.Robertson+,J,JNE,27,531,1973) =73RO2V002900200019 (E,20867006,T.B.Ryves+,J,JP/G,4,(11),1783,1978) =78RY2V002900200020 (E,10186002,G.N.Salaita,J,NP/A,170,193,197107) =71SA1V002900200021 (E,30008029,P.Strohal+,J,NP,30,49,196202) =62ST1V002900200022 (E,20986009,M.T.Swinhoe,C,79KNOX,246,197910) =79SW1V002900200023 and report AERE-PR/NP26,P.39(1979) V002900200024 (E,20111001,H.Vonach+,J,ZP,237,155,197009) =70VO1V002900200025 (E,,G.Winkler+,W,WINKLER,1981) Check req'd =81WI1V002900200026 * Following activation measurements are excluded V002900200027 from the evaluation, the reasons of which are V002900200028 mentioned in subentry .001. Marked with N. V002900200029 (N,30118004,J.Csikai+,J,NP,46,141,196307) V002900200030 (N,21419004,M.J.Depraz+,J,JPR,21,377,196005) V002900200031 (N,30479002,U.Garuska+,P,INR-1773/I/PL/A,16,1978) V002900200032 and J.Dresler et al.,77GAUSSIG Conf.,ZFK-376,51(1978) V002900200033 (N,20922002,J.M.Jeronymo+,J,NP,47,157,1963) V002900200034 (N,10116002,J.Lebowitz+,J,NC/A,65,675,1970) V002900200035 (N,11530003,H.W.Schmitt+,J,PR,121,827,1961) V002900200036 (N,11504003,H.A.Tewes+,R,UCRL-6028-T,196006) V002900200037 COMMENT Other evaluations are V002900200038 ENDF/B-V 116.8 mb V002900200039 Spaepen(1969),Tech.Rep.IAEA-107 114. mb V002900200040 Tagesen,Vonach(1981),Phys.Data,13,No.3,113.1+/-0.5 mb V002900200041 The ENDF value is 3% higher than this work. V002900200042 STATUS (SPSDD,V0043002) Superseded by EXFOR V0043.002 V002900200043 HISTORY (20110131U) On. Upper to lower cases, 4 digits year V002900200044 ENDBIB 42 0 V002900200045 NOCOMMON 0 0 V002900200046 NODATA 0 0 V002900200047 ENDSUBENT 46 0 V002900299999 SUBENT V0029003 20110131 V028V002900300001 BIB 5 42 V002900300002 REACTION (26-FE-56(N,P)25-MN-56,,SIG,,,EVAL) V002900300003 REL-REF (E,10022010,R.C.Barrall+,R,AFWL-TR-68-134,1969) =69BA2V002900300004 (E,10031005,R.C.Barrall+,J,NP/A,138,387,196912) =69BA1V002900300005 (E,11701001,D.C.Santry+,J,CJP,42,1030,1964) =64SA1V002900300006 (E,20890004,P.Cuzzocrea+,J,NC/B,54,53,196803) =68CU1V002900300007 (E,11494009,F.Gabbard+,J,PR,128,1276,1962) =62GA1V002900300008 (E,,V.D.Huynh,R,BIPM-76/2,1976) =76HU1V002900300009 (E,40223010,V.Levkovskii+,J,SNP,8,4,196901) =69LE1V002900300010 (E,20377002,H.Liskien+,J,JNE,19,73,196502) =65LI1V002900300011 H.Liskien,A.Paulsen,int.rep.CBNM-VG-1(1974) =74LI1V002900300012 H.Liskien,A.Paulsen,int.rep.CBNM-VG-6(1975) =75LI1V002900300013 (E,20888004,G.C.Bonazzola+,J,NP,51,337,196402) =64BO1V002900300014 (E,,Z.A.Ramendik+,J,SJA,42,152,197708) =77RA1V002900300015 V.T.Shchebolev et al.,Metrologie 8(1974)61 =74SH1V002900300016 (E,20993002,K.Kudo,J,NIM,141,325,197703) =77KU1V002900300017 E.Teranishi et al. Bull.Electrotec.Lab.41(77)693=77TE1V002900300018 (E,20815001,H.Vonach+,C,68WASH,2,885,196803) =68VO1V002900300019 * Following activation measurements are excluded V002900300020 from the evaluation, the reasons of which are V002900300021 mentioned in subentry .001. Marked with N. V002900300022 (N,11718005,D.M.Chittenden+,J,PR,122,860,1961) V002900300023 (N,11696001,W.G.Cross+,P,EANDC(CAN)-16,1,1963) V002900300024 and report PR-P-53,7(1962) Chalk River. V002900300025 (N,21419006,M.J.Depraz+,J,JPR,21,377,1960) V002900300026 (N,10289002,N.C.Dyer+,J,JIN,34,1119,197204) V002900300027 in the text (Table2), it is miscoded as 1, which is toV002900300028 be 2. V002900300029 (N,30531006,K.C.Garg+,J,IPA,17,385,197906) V002900300030 (N,20377002,H.Liskien+,J,JNE,19,73,196502) V002900300031 (N,20554006,S.M.Qaim+,C,71CANT,,121,1971) V002900300032 and N.Molla,S.M.Qaim,Nucl.Phys,A283(1977)269. V002900300033 (N,10309004,J.J.Singh,J,ANS,15,147,197206) V002900300034 in the text (Table 2), Singh(1970) should be read as V002900300035 Singh (1972). V002900300036 COMMENT Other evaluations are, V002900300037 ENDF/B-V 103.6 mb V002900300038 Bychkov+(1980),Report INDC(CCP)-146 108. mb V002900300039 Zolotarev+(1980),Report INDC(CCP)-147 109.45 mb V002900300040 Ryves,Axton(1979),79KNOX Conf,P.980, 109.2+/-1.0 mb V002900300041 The ENDF value is 4% lower than this work. V002900300042 STATUS (SPSDD,V0043003) Superseded by EXFOR V0043.003 V002900300043 HISTORY (20110131U) On. Upper to lower cases, 4 digits year V002900300044 ENDBIB 42 0 V002900300045 NOCOMMON 0 0 V002900300046 NODATA 0 0 V002900300047 ENDSUBENT 46 0 V002900399999 SUBENT V0029004 20110131 V028V002900400001 BIB 5 30 V002900400002 REACTION (29-CU-63(N,2N)29-CU-62,,SIG,,,EVAL) V002900400003 REL-REF (E,21339006,M.Bormann+,J,ZP,166,477,196202) =62BO1V002900400004 (E,21352008,H.Pollehn+,J,ZN/A,16,227,1961) =61PO1V002900400005 (E,20930002,D.Crumpton+,J,JIN,31,1,196901) =69CR1V002900400006 (E,11411003,A.J.de Jejuren+,J,PR,120,901,1960) =60DE1V002900400007 (E,20106001,B.Grimeland,J,PR/B,137,878,196502) =65GR1V002900400008 (E,21401002,J.Letessir+,J,CR,259,4620,196412) =64LE1V002900400009 (E,20377004,H.Liskien+,J,JNE,19,73,196502) =65LI1V002900400010 H.Liskien,A.Paulsen,int.rep.CBNM-VG-1(1974) =74LI1V002900400011 H.Liskien,A.Paulsen,int.rep.CBNM-VG-6(1975) =75LI1V002900400012 (E,21509003,R.Mogharrab+,J,AKE,19,107,197204) =72MO1V002900400013 (E,,A.Pasquarelli,J,NP/A,93,218,196703) =67PA1V002900400014 (E,20772001,T.B.Ryves+,J,MET,14,(3),127,197806) =78RY1V002900400015 (E,20329003,M.Sakisaka+,J,JPJ,16,1869,196110) =61SA1V002900400016 * Following activation measurements are excluded V002900400017 from the evaluation, the reasons of which are V002900400018 mentioned in subentry .001. Marked with N. V002900400019 (N,20835004,M.Bormann+,J,NP/A,130,195,1969) V002900400020 (N,21266007,M.Cevolani+,J,NC,26,1328,1962) V002900400021 (N,30061003,Chatterjee+,P,BARC-305,30,1967) V002900400022 (N,11356004,J.M.Fergusson+,J,PR,118,228,1960) V002900400023 (N,11268004,J.H.McCrary+,J,BAP,5,246(HA5),1960) V002900400024 COMMENT Other evaluations are, V002900400025 UKNDL 616. mbV002900400026 JENDL 527. mbV002900400027 Body,Csikai(1973), Atom.Energy Rev.11,153, 558+/-11 mbV002900400028 Bychkov+(1980),Report INDC(CCP)-146 557. mbV002900400029 Tagesen+(1979),Phys.Data,13,1 543+/-5 mbV002900400030 STATUS (SPSDD,V0043004) Superseded by EXFOR V0043.004 V002900400031 HISTORY (20110131U) On. Upper to lower cases, 4 digits year V002900400032 ENDBIB 30 0 V002900400033 NOCOMMON 0 0 V002900400034 NODATA 0 0 V002900400035 ENDSUBENT 34 0 V002900499999 SUBENT V0029005 20110131 V028V002900500001 BIB 5 41 V002900500002 REACTION (29-CU-65(N,2N)29-CU-64,,SIG,,,EVAL) V002900500003 REL-REF (E,10022015,R.C.Barrall+,R,AFWL-TR-68-134,1969) =69BA1V002900500004 (E,21352009,H.Pollehn+,J,ZN/A,16,227,1961) =61PO1V002900500005 (E,11776001,D.C.Santry+,J,CJP,44,1183,1965) =65SA1V002900500006 (E,20930003,D.Crumpton+,J,JIN,31,1,196901) =69CR1V002900500007 (E,31107001,R.N.Glover+,J,NP,29,309,1962) =62GL2V002900500008 (E,20386003,A.Paulsen+,J,NUK,7,117,196503) =65PA2V002900500009 H.Liskien,A.Paulsen,Int.Rep.CBNM-VG-1(1974) =74LI1V002900500010 H.Liskien,A.Paulsen,Int.Rep.CBNM-VG-6(1975) =75LI1V002900500011 (E,21509004,R.Mogharrab+,J,AKE,19,107,197204) =72MO1V002900500012 (E,20198001,W.Nagel,T,NAGEL,196612) =65NA1V002900500013 and W.Nagel and A.H.W.Aten, Physica,31(1965)1091 V002900500014 (E,20888006,G.C.Bonazzola+,J,NP,51,337,196402) =64BO1V002900500015 (E,11645007,R.J.Prestwood+,J,PR,121,1438,196103) =60PR1V002900500016 (E,20536009,S.M.Qaim,J,NP/A,185,614,197205) =72QU1V002900500017 (E,20799015,J.C.Robertson+,J,JNE,27,531,197308) =73RO2V002900500018 (E,20772001,T.B.Ryves+,J,MET,14,(3),127,197806) =78RY1V002900500019 (E,20815001,H.Vonach+,C,68WASH,2,885,196803) =68VO1V002900500020 (E,20611001,W.Mannhart+,J,ZP/A,272,279,197503) =75MA1V002900500021 (E,31039005,E.Weigold,J,AUJ,13,186,1960) =60WE1V002900500022 * Following activation measurements are excluded V002900500023 from the evaluation, the reasons of which are V002900500024 mentioned in subentry .001. Marked with N. V002900500025 (N,21343004,M.Bormann+,J,ZP,174,1,1963) V002900500026 (N,20835005,M.Bormann+,J,NP/A,130,195,1969) V002900500027 (N,21419007,M.J.Depraz+,J,JPR,21,377,196005) V002900500028 (N,11268005,J.H.McCrary+,J,BAP,5,246(HA5),1960) V002900500029 (N,11328013,L.A.Rayburn,J,PR,122,168,1961) V002900500030 (N,11263026,J.E.Strain+,R,ORNL-3672,1965) V002900500031 COMMENT Other evaluations are, V002900500032 ENDF/B-V 926. mb V002900500033 UKNDL 989. mb V002900500034 JENDL 951. mb V002900500035 Body,Csikai(1973),Atom.Energy Rev.11,153, 971+/-5 mb V002900500036 Bychkov+(1980),Report INDC(CCP)-146 997. mb V002900500037 For the Cu-65(n,2n) cross-section, there is a current V002900500038 large uncertainty due to the Cu-64 decay-scheme V002900500039 branching, which must be clarified before a reliable V002900500040 result can be determined. V002900500041 STATUS (SPSDD,V0043005) Superseded by EXFOR V0043.005 V002900500042 HISTORY (20110131U) On. Upper to lower cases, 4 digits year V002900500043 ENDBIB 41 0 V002900500044 NOCOMMON 0 0 V002900500045 NODATA 0 0 V002900500046 ENDSUBENT 45 0 V002900599999 SUBENT V0029006 20110131 V028V002900600001 BIB 5 28 V002900600002 REACTION (79-AU-197(N,2N)79-AU-196,,SIG,,,EVAL) V002900600003 REL-REF (E,20842005,P.Andersson+,R,LUNF-D6-3021,197811) =78AN1V002900600004 (E,10022022,R.C.Barall+,R,AFWL-TR-68-134,1969) =69BA1V002900600005 (E,10536054,B.P.Bayhurst+,J,PR/C,12,451,197508) =75BA1V002900600006 (E,20802017,W.Dilg+,J,NP/A,118,9,196809) =68DI1V002900600007 (E,20486005,A.Paulsen+,J,AKE,26,34,197508) =75PA1V002900600008 H.Liskien,A.Paulsen,INT.REP.CBNM-VG-1(1974) =74LI1V002900600009 H.Liskien,A.Paulsen,INT.REP.CBNM-VG-6(1975) =75LI1V002900600010 (E,40136020,G.N.Maslov+,R,YK-9,50,1972) =74MA1V002900600011 and report INDC(CCP)-42/U,P.10(1974). Engl.TranslationV002900600012 (E,10312009,D.R.Nethaway,J,NP/A,190,635,1972) =72NE1V002900600013 (E,11645026,R.J.Prestwood+,J,PR,121,1438,196103) =61PR1V002900600014 (E,20536031,S.M.Qaim,J,NP/A,185,614,197205) =72QU1V002900600015 (E,,T.B.Ryves+,J,JP/G,7,(2),115,1981) =81RY1V002900600016 (E,20815001,H.Vonach+,C,68WASH,2,885,196803) =68VO1V002900600017 * Following activation measurements are excluded V002900600018 from the evaluation, the reasons of which are V002900600019 mentioned in subentry .001. Marked with N. V002900600020 (N,10244008,A.K.Hankla+,J,NP/A,180,157,1972) V002900600021 (N,11504017,H.A.Tewes+,R,UCRL-6028-T,196006) V002900600022 COMMENT The results of other evaluations are, V002900600023 ENDF/B-V 2202.mbV002900600024 Philis,Bersillon(1977),report CEA-R-4826, 2238+224 mbV002900600025 -336 mbV002900600026 Body,Csikai(1973),Atom.Energy Rev.11,153, 2109+/-110mbV002900600027 Bychkov et al.(1980),report INDC(CCP)-146,2274. mbV002900600028 STATUS (SPSDD,V0043006) Superseded by EXFOR V0043.006 V002900600029 HISTORY (20110131U) On. Upper to lower cases, 4 digits year V002900600030 ENDBIB 28 0 V002900600031 NOCOMMON 0 0 V002900600032 NODATA 0 0 V002900600033 ENDSUBENT 32 0 V002900699999 SUBENT V0029007 20110131 V028V002900700001 BIB 5 29 V002900700002 REACTION (41-NB-93(N,2N)41-NB-92-M,,SIG,,,EVAL) V002900700003 REL-REF (E,20830002,M.Borman+,J,NP/A,157,481,197011) =70BO1V002900700004 (E,10420003,D.C.Santry+,P,PR-CMA-27,14,197401) =74SA1V002900700005 (E,80238003,V.L.Glagolev+,J,ZET,40,743,1961) =62GL1V002900700006 and JETP,13(1961)520, English translation. V002900700007 (E,10836003,C.G.Hudson+,J,ANE,5,589,1978) =78HU1V002900700008 (E,10088019,I.Husain+,J,PR/C,1,1233,197004) =70HU1V002900700009 (E,20393002,A.Paulsen+,J,ZP,238,23,197009) =70PA1V002900700010 (E,10709001,D.R.Nethaway+,J,JIN,40,1285,1978) =78NE1V002900700011 (E,20554011,S.M.Qaim+,C,71CANT,,121,197109) =71QU1V002900700012 (E,20033012,R.Rieder+,J,APA,23,42,196605) =66RI1V002900700013 (E,,T.B.Ryves+,J,JP/G,7,(4),529,1981) =81RY1V002900700014 (E,20347005,D.G.Vallis,R,AWRE-O-76/66,196612) =66VA1V002900700015 * Following activation measurements are excluded V002900700016 from the evaluation, the reasons of which are V002900700017 mentioned in subentry .001. Marked with N. V002900700018 (N,,D.Basu+,C,66BOMBAY,,209,196602) V002900700019 (N,11590001,E.T.Bramlitt+,J,PR,131,2649,1963) V002900700020 (N,,P.Carter,C,66WASH,,682,196603) V002900700021 (N,10497005,W.D.Lu+,J,PR/C,1,350,197001) V002900700022 (N,30008014,P.Strohal+,J,NP,30,49,196202) V002900700023 (N,11504010,H.A.Tewes+,R,UCRL-6028-T,196006) V002900700024 (N,20087006,H.Vonach+,J,OSA,96,120,195903) V002900700025 In the text (Table 2), it is miscoded as 7, which is V002900700026 to be 6. V002900700027 COMMENT The result of other evaluation is, V002900700028 Philis et al.,(1975), Report CEA-R-4676, 483+48-87 mb V002900700029 STATUS (SPSDD,V0043007) Superseded by EXFOR V0043.007 V002900700030 HISTORY (20110131U) On. Upper to lower cases, 4 digits year V002900700031 ENDBIB 29 0 V002900700032 NOCOMMON 0 0 V002900700033 NODATA 0 0 V002900700034 ENDSUBENT 33 0 V002900799999 SUBENT V0029008 20110131 V028V002900800001 BIB 5 19 V002900800002 REACTION (16-S-32(N,P)15-P-32,,SIG,,,EVAL) V002900800003 REL-REF (E,11571001,L.Allen+,J,PR,107,1363,195709) =57AL1V002900800004 (E,10022006,R.C.Barrall+,R,AFWL-TR-68-134,1969) =69BA1V002900800005 (E,,J.D.Hemmingway,R,AERE-X/PR-2491,6,1963) =63HE1V002900800006 (E,40223011,V.Levkovskii+,J,YF,8,(1),7,196807) =69LE1V002900800007 and Soviet J.Nucl.PhyS.8(1969)4, English translation V002900800008 (E,20889017,A.Pasquarelli,J,NP/A,93,218,196703) =67PA1V002900800009 (E,20799010,J.C.Robertson+,J,JNE,27,531,197308) =73RO2V002900800010 (E,,W.Schantl,T,SCHANTL,1970) =70SC1V002900800011 * Following activation measurements are excluded V002900800012 from the evaluation, the reasons of which are V002900800013 mentioned in subentry .001. Marked with N. V002900800014 (N,80250002,V.N.Levkovskii,J,ZET,45,305,1963) V002900800015 and JETP,18(1964)213, English translation. V002900800016 COMMENT The results of other evaluations are, V002900800017 ENDF/B-IV 219.mb, V002900800018 Spaepen(1969),Tech.Report IAEA-107, 223.mb. V002900800019 STATUS (SPSDD,V0043008) Superseded by EXFOR V0043.008 V002900800020 HISTORY (20110131U) On. Upper to lower cases, 4 digits year V002900800021 ENDBIB 19 0 V002900800022 NOCOMMON 0 0 V002900800023 NODATA 0 0 V002900800024 ENDSUBENT 23 0 V002900899999 SUBENT V0029009 20110131 V028V002900900001 BIB 5 18 V002900900002 REACTION (1-H-1(N,EL)1-H-1,,SIG,,,EVAL) V002900900003 REL-REF (E,,J.C.Robertson+,J,JNE,27,139,1973) =73RO1V002900900004 Gammel's value(0.658 b) is corrected by Hopkins-Breit.V002900900005 J.L.Gammel,Fast Neutron Physics (ed.Marion,Fowler), V002900900006 Wiley,New York (1963). V002900900007 J.C.Hopkins and G.Breit,Nucl.Data Tabl,A9(1971)137. V002900900008 (E,,T.B.Ryves+,J,MET,14,(3),127,197806) =78RY1V002900900009 Halperns-Breit's data are re-evaluated for use of V002900900010 relativistic kinematics.(Correction of the cross- V002900900011 section by 1% AT 20 MeV) V002900900012 (E,,D.J.Thomas+,J,NIM,179,397,1981) =81TH1V002900900013 Explicit cross-section values are not given in the V002900900014 above-mentioned related references. V002900900015 COMMENT The results of other evaluations are, V002900900016 ENDF/B-IV 661.1 mb, V002900900017 GAMMEL(1963),IBID. 661.3 mb. V002900900018 STATUS (SPSDD,V0043009) Superseded by EXFOR V0043.009 V002900900019 HISTORY (20110131U) On. Upper to lower cases, 4 digits year V002900900020 ENDBIB 18 0 V002900900021 NOCOMMON 0 0 V002900900022 NODATA 0 0 V002900900023 ENDSUBENT 22 0 V002900999999 ENDENTRY 9 0 V002999999999