ENTRY 23545 20230324 231623545 0 1 SUBENT 23545001 20230324 231623545 1 1 BIB 12 30 23545 1 2 TITLE Emission of Be, C and O isotopes in 235U(nth,f) 23545 1 3 AUTHOR (A.Sicre,W.Baum,C.Barreau,T.P.Doan,A.Goepfert,B.Leroux,23545 1 4 M.Mutterer,J.P.Theobald,H.Faust) 23545 1 5 REFERENCE (C,89LENING,,223,1989) 23545 1 6 (S,JINR-E4-93-58,353,1993) - data on figs. 23545 1 7 (C,92BERNKAST,,477,1992) 23545 1 8 INSTITUTE (2FR GRA) A.Sicre,C.Barreau,T.P.Doan,B.Leroux, 23545 1 9 (2GERTHD) W.Baum,A.Goepfert,M.Mutterer,J.P.Theobald 23545 1 10 (2FR ILL) H.Faust 23545 1 11 FACILITY (REAC,2FR ILL) Lohengrin spectrometer at High Flux 23545 1 12 Reactor al ILL in Grenoble. 23545 1 13 INC-SOURCE (REAC) 23545 1 14 INC-SPECT Thermal neutron flux 1.E+14 n/(cm2*sec) 23545 1 15 SAMPLE No information in the article. 23545 1 16 DETECTOR (TELES,PROPC,SIBAR) 23545 1 17 Recoil spectrometer separated particles 23545 1 18 according to A/q and E/q ( q - ionic charge). 23545 1 19 dE-E detector to identify nuclear charge, placed 23545 1 20 at the focal plane of spectrometer; consist of a gas 23545 1 21 proportional counter (to measure energy loss dE) and 23545 1 22 10 independent surface barrier detectors (to measure 23545 1 23 residual energy). 23545 1 24 METHOD (EDE) 23545 1 25 Mass resolution function was determined for 23545 1 26 4He(2+) at E=10 MeV. 23545 1 27 CORRECTION Relative yields were corrected for variation of source 23545 1 28 strength with time. 23545 1 29 HISTORY (20200402C) M.M. 23545 1 30 (20220209U) SD:Refs added(JINR-E4-93-58;92BERNKAST,477)23545 1 31 (20230324U) SD: Page corrected in ref.(JINR-E4-93-58). 23545 1 32 ENDBIB 30 0 23545 1 33 NOCOMMON 0 0 23545 1 34 ENDSUBENT 33 0 23545 199999 SUBENT 23545002 20200402 228723545 2 1 BIB 3 5 23545 2 2 REACTION ((92-U-235(N,F)ELEM/MASS,TER,FY)/ 23545 2 3 (92-U-235(N,F)2-HE-4,TER,FY)) 23545 2 4 ERR-ANALYS (DATA-ERR) Type of uncertainty is not explained in the 23545 2 5 article. 23545 2 6 STATUS (TABLE) Table 1 of Conf.Proc.,89LENING,,p.223,1989 23545 2 7 ENDBIB 5 0 23545 2 8 COMMON 1 3 23545 2 9 EN-DUMMY 23545 2 10 EV 23545 2 11 0.0253 23545 2 12 ENDCOMMON 3 0 23545 2 13 DATA 5 14 23545 2 14 ELEMENT MASS DATA DATA-MAX DATA-ERR 23545 2 15 NO-DIM NO-DIM NO-DIM NO-DIM NO-DIM 23545 2 16 4. 9. 4.20 E-04 0.10 E-04 23545 2 17 4. 10. 32.00 E-04 0.07 E-04 23545 2 18 4. 11. 2.96 E-04 0.35 E-04 23545 2 19 4. 12. 1.45 E-04 0.20 E-04 23545 2 20 4. 14. 0.003E-04 0.003E-04 23545 2 21 6. 13. 0.40 E-04 0.15 E-04 23545 2 22 6. 14. 9.80 E-04 0.70 E-04 23545 2 23 6. 15. 1.85 E-04 0.16 E-04 23545 2 24 6. 16. 1.55 E-04 0.20 E-04 23545 2 25 6. 17. 0.14 E-04 0.04 E-04 23545 2 26 6. 18. 0.05 E-04 0.02 E-04 23545 2 27 6. 20. 3.60 E-07 23545 2 28 8. 20. 0.18 E-04 0.04 E-04 23545 2 29 8. 21. 0.12 E-04 23545 2 30 ENDDATA 16 0 23545 2 31 ENDSUBENT 30 0 23545 299999 SUBENT 23545003 20200402 228723545 3 1 BIB 4 5 23545 3 2 REACTION (92-U-235(N,F)ELEM/MASS,TER,KE) 23545 3 3 MISC-COL (MISC) FWHM of energy distribution 23545 3 4 ERR-ANALYS (DATA-ERR) Type of uncertainty is not explained in the 23545 3 5 article. 23545 3 6 STATUS (TABLE) Table 1 of Conf.Proc.89LENING,,p.223,1989 23545 3 7 ENDBIB 5 0 23545 3 8 COMMON 1 3 23545 3 9 EN-DUMMY 23545 3 10 EV 23545 3 11 0.0253 23545 3 12 ENDCOMMON 3 0 23545 3 13 DATA 6 8 23545 3 14 ELEMENT MASS DATA DATA-ERR MISC MISC-ERR 23545 3 15 NO-DIM NO-DIM MEV MEV MEV MEV 23545 3 16 4. 9. 18.90 0.50 18.5 1.70 23545 3 17 4. 10. 17.20 0.10 17.80 0.30 23545 3 18 4. 11. 16.30 0.70 16.20 1.70 23545 3 19 4. 12. 15.40 0.80 14.30 1.60 23545 3 20 6. 14. 22.30 0.50 21.50 1.30 23545 3 21 6. 15. 21.90 0.50 18.10 0.90 23545 3 22 6. 16. 20.70 0.70 17.60 1.10 23545 3 23 8. 20. 24.24 1.50 21.22 3.23 23545 3 24 ENDDATA 10 0 23545 3 25 ENDSUBENT 24 0 23545 399999 ENDENTRY 3 0 2354599999999