ENTRY 21594 19810408 00002159400000001 SUBENT 21594001 19810408 00002159400100001 BIB 15 31 2159400100002 INSTITUTE (2FR ILL) 2159400100003 REFERENCE (J,PL/B,53,45,7411) 2159400100004 AUTHOR (G.SIEGERT,H.WOLLNIK,J.GREIF,G.FIEDLER,M.ASGHAR, 2159400100005 G.BAILLEUL,J.P.BOCQUET,J.P.GAUTHERON,H.SCHRADER, 2159400100006 H.EWALD,P.ARMBRUSTER) 2159400100007 TITLE -DIRECT DETERMINATION OF THE NUCLEAR CHARGE DISTRIBUTI 2159400100008 OF MASS SEPERATED FISSION PRODUCTS FROM U-235(N,F) -. 2159400100009 FACILITY (SPECM) LOHENGRIN ON-LINE MASS SEPERATOR. 2159400100010 (REAC ) HIGH FLUX REACTOR. 2159400100011 INC-SOURCE (REAC ) THERMAL NEUTRONS FROM REACTOR. 2159400100012 INC-SPECT .MAXWELLIAN THERMAL NEUTRON SPECTRUM. 2159400100013 SAMPLE .URANIUM DIOXIDE, ENRICHED TO 93 PERCENT U-235, 2159400100014 THICKNESS OF 400 MICRO-GM/CM*2. 2159400100015 METHOD (ASEP ) ON-LINE MASS SEPERATION, WITH RESOLVING POWER 2159400100016 OF 1/400. CHARGE SEPERATION WITHIN EACH MASS CHAIN BY 2159400100017 USING DELTA-E SILICON SURFACE BARRIER DETECTORS WITH 2159400100018 A NUCLEAR CHARGE RESOLVING POWER OF 1/43 FOR FRAGMENT 2159400100019 WITH KINETIC ENERGY OF 100 MEV. 2159400100020 DETECTOR (SOLST) SOLID STATE SILICON SURFACE BARRIER DETECTORS, 2159400100021 A 8 MICRO-M THICK ORTEC DETECTOR FOR DELTA-E MEASURE- 2159400100022 MENT. 2159400100023 ANALYSIS .CHARGE DISTRIBUTIONS FOR EACH MASS CHAIN ARE FITTED 2159400100024 TO A GAUSSIAN DISTRIBUTION. WEIGHTED AVERAGES OF 2159400100025 SEVERAL INDEPENDANT MEASUREMENTS ARE QUOTED. 2159400100026 STATUS .TABLE 1, PL/B,53,45. 2159400100027 HISTORY (800619C) 2159400100028 (800718E) 2159400100029 CORRECTION .CORRECTED FOR CHARGE DEPENDENT EFFICIENCY OF THE MASS 2159400100030 SPECTROMETER. 2159400100031 ERR-ANALYS .ONE STANDARD DEVIATION FROM COUNTING STATISTICS AND 2159400100032 FROM UNCERTAINTIES IN THE ANALYSIS AND CORRECTIONS. 2159400100033 ENDBIB 31 0 2159400100034 COMMON 1 3 2159400100035 EN-DUMMY 2159400100036 EV 2159400100037 2.5300E-02 2159400100038 ENDCOMMON 3 0 2159400100039 ENDSUBENT 38 0 2159400199999 SUBENT 21594002 19800718 00002159400200001 BIB 3 6 2159400200002 REACTION ((92-U-235(N,F)ELEM/MASS,IND,FY,,MXW)/ 2159400200003 (92-U-235(N,F)MASS,CHN,FY,,MXW)) 2159400200004 FRACTIONAL INDEPENDENT THERMAL FISSION YIELDS. 2159400200005 STATUS .TABLE 1. 2159400200006 HISTORY (800619C) 2159400200007 (800718E) 2159400200008 ENDBIB 6 0 2159400200009 NOCOMMON 0 0 2159400200010 DATA 4 7 2159400200011 ELEMENT MASS RATIO RATIO-ERR 2159400200012 NO-DIM NO-DIM NO-DIM NO-DIM 2159400200013 3.5000E+01 9.0000E+01 1.0600E-01 1.0000E-02 2159400200014 3.5000E+01 9.1000E+01 4.0000E-02 5.0000E-03 2159400200015 3.6000E+01 9.0000E+01 7.5300E-01 2.0000E-02 2159400200016 3.6000E+01 9.1000E+01 5.4200E-01 1.0000E-02 2159400200017 3.7000E+01 9.0000E+01 1.4200E-01 1.0000E-02 2159400200018 3.7000E+01 9.1000E+01 3.7300E-01 1.0000E-02 2159400200019 3.8000E+01 9.1000E+01 4.5000E-02 5.0000E-02 2159400200020 ENDDATA 9 0 2159400200021 ENDSUBENT 20 0 2159400299999 SUBENT 21594003 19810408 00002159400300001 BIB 3 5 2159400300002 REACTION (92-U-235(N,F)MASS,,ZP,,MXW) AVERAGE NUCLEAR CHARGE. 2159400300003 STATUS .TABLE 1. 2159400300004 (DEP,21594002) 2159400300005 HISTORY (800619C) 2159400300006 (800718E) 2159400300007 ENDBIB 5 0 2159400300008 NOCOMMON 0 0 2159400300009 DATA 2 2 2159400300010 MASS DATA 2159400300011 NO-DIM NO-DIM 2159400300012 9.0000E+01 3.6040E+01 2159400300013 9.1000E+01 3.6420E+01 2159400300014 ENDDATA 4 0 2159400300015 ENDSUBENT 14 0 2159400399999 ENDENTRY 3 0 2159499999999