/*===================================================================*/
 /* NRDF D1851 Data No.1                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,1;
 D#=D1851;
 TITLE=/ Characteristics of binary scission configurations in
         proton-induced fission of actinides /;
 PURPOSE=/ To clarify the correlation between mass yield
           distributions and scission configurations in low-energy
           proton-induced fission of actinides, and to elucidate how
           the bimodal properties vary as a function of fissioning
           nuclei in wide range of actinide fission /;
 ATH=(Y.L.ZHAO'1,3', T.OHTSUKI'2', Y.NAGAME'3', I.NISHINAKA'3',
      K.TSUKADA'3', S.ICHIKAWA'3', H.IKEZOE'3', Y.HATSUKAWA'3',
      K.HATA'3', M.TANIKAWA'4', Z.QIN'3', K.SUEKI'1', Y.OURA'1',
      H.KUDO'5', H.NAKAHARA'1');
 INST-ATH=(2JPNTMU'1', 2JPNTOH'2', 2JPNJAE'3', 2JPNTOK'4',
           2JPNNII'5');
      /* '1' Department of Chemistry */
      /* '2' Laboratory of Nuclear Science */
      /* '4' Department of Chemistry */
      /* '5' Department of Chemistry */
 REF=JRN;
 VLP=239(1999)113;
 RCTS=238U(P,FISSN), 232TH(P,FISSN), 244PU(P,FISSN);
 PHQS=(ENGY-SPEC'6', FISSN-YLD);
 /* '6' Total kinetic energy distribution */
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,1;
 /* 2003-11-04 : Converted, Data converted from EXFOR O0699 */
 /* Related references 
    - Y.Nagame et al., PL/B, 387(1996)26.
    (Detail of experimental procedure and two-Gaussian analysis)
    - Y.Nagame et al., JRN, 239(1999)97.
 RTY=FISSN;
 /* Additional results shown but not compiled
    - Comparison with calculated values (Two-gaussian analysis. The
      elongation properties of nuclei at scission in a wide range of
      actinides fissions are studied. The results suggest that the
      compact and the elongated scission configurations in light
      actinides fission smoothly change to the scission properties of
      the symmetric and the asymetric modes in heavy actinides
      fission.)
    - Distance of two charge centers at scission configurations
      evaluated from the total kinetic energy of the fragment mass for
      13 MeV p+238U fission. See Fig.2 of this reference.
 CHM=ELM;
 PHYS-FORM=SLD;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=VDGT;
 INST-ACC=2JPNJAE;
 POL-PRJ=0%;
 DET-PARTCL=X'7';
 /* '7' Fission fragments */
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(MCPLT'8',SBD'9',MCPLT'10',PPAC'11',TOF'12');
 /* '8' Used as stop detector of ToF1 telescope placed at
        theta(lab)=50 deg */
 /* '9' Used as stop and energy signals, located behind the ToF1
        stop detector */
 /* '10' Used as start detector of ToF2 telescope placed at
         theta(lab)=130 deg */
 /* '11' Used as stop detector of ToF2 telescope placed at
         theta(lab)=130 deg */
 /* '12' Flight pathes of two telescopes are 55 cm and 50 cm,
         respectively. */
 SOLID-ANGL=XMSR'13';
 /* '13' 0.17 and 32 msr for ToF1 and ToF2, respectively */
 ERS-DET=[2.5MEV'14';
 /* '14' Overall resolution of kinetic energy. Resolution of mass
         is about 2.0 u. */
 CALB-DET=/ Velocity calibration was performed using the 240 MeV 127I
            beam to bombard the thin targets (60 micro-gram/cm2 thick),
            natAg, natIn, and 209Bi. Each target was evaporated on 30
            micro-gram/cm2 thick carbon foils. The recoil nuclei and
            the elastically scattered 127I ions were detected with the
            present ToF system. /;
 /* Experimental Method:
    - Time-of-flight (Flight pathes of two telescopes are 55 cm and
      50 cm, respectively.)
 RCT=238U(P,FISSN);
 PHQ=ENGY-SPEC'15';
 /* '15' Total kinetic energy distribution */
 THK-TGT=[0.07MG/CM**2;
 BAC=C;
 THK-BAC=0.03MG/CM**2;
 INC-ENGY-LAB=13MEV;
 /* Analysis:
    - Decomposition of total kinetic energy (TKE) distribution into
      low- and high-TKE components was done by using the two-Gaussian
      analysis, described in detail in [Y.Nagame et al., Phys. Lett.
      B387(1996)26].
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,1;
 INC-ENGY-LAB=13MEV;
 EMT=FF;
 A=126;
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 TOT-KIN-ENGY'16' COUNTS'17' DATA1'18' DATA2'19'
 (MEV) (NODIM) (NODIM) (NODIM)
 132. 0.98636 1.6148 X
 134. 1.973 2.6463 X
 136. 2.9597 4.2002 X
 138. 9.8675 6.4563 X
 140. 6.9078 9.6118 X
 142. 16.777 13.859 X
 144. 22.701 19.352 X
 146. 21.715 26.172 0.15012
 148. 28.628 34.28 0.26943
 150. 39.49 43.485 0.46682
 152. 44.43 53.424 0.78079
 154. 60.27 63.567 1.2607
 156. 69.25 73.253 1.965
 158. 82.757 81.755 2.9566
 160. 98.962 88.369 4.2945
 162. 114.58 92.508 6.0216
 164. 117.55 93.79 8.1508
 166. 83.968 92.095 10.651
 168. 102.75 87.58 13.435
 170. 110.66 80.663 16.36
 172. 95.963 71.951 19.231
 174. 74.98 62.159 21.822
 176. 68.186 52.007 23.905
 178. 69.178 42.142 25.28
 180. 64.241 33.073 25.807
 182. 56.338 25.137 25.432
 184. 52.389 18.504 24.194
 186. 26.69 13.192 22.218
 188. 26.692 9.1085 19.697
 190. 16.807 6.0909 16.857
 192. 11.864 3.9447 13.927
 194. 9.8873 2.4743 11.107
 196. 4.944 1.503 8.5513
 \END;
 /*===================================================================*/