/*===================================================================*/
 /* NRDF D0713 Data No.1                                              */
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 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,1;
 D#=D713;
 TITLE=/ Splitting of low-lying octupole vibrational strength in
         76,78,80,82Kr /;
 ATH=(S.MATSUKI'1', K.OGINO'2', Y.KADOTA'2', N.SAKAMOTO'3', T.TANABE'4',
      M.YASUE'4', A.YOKOMIZO'4', S.KUBONO'4', Y.OKUMA'5');
 INST-ATH=(2JPNKTO'1', 2JPNKTO'2', 2JPNJPN'3', 2JPNINS'4',
           2JPNRCN'5');
      /* '1' Cyclotron Laboratory, Institute for Chemical Research */
      /* '2' Department of Nuclear Engineering */
      /* '3' Department of Physics, Nara Women's University, Nara */
 REF=PL/B;
 VLP=113(1982)21;
 RCTS=(78KR(P,T)76KR, 80KR(P,T)78KR, 82KR(P,T)80KR, 84KR(P,T)82KR);
 PHQS=ANGL-DSTRN;
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,1;
 /* 2009-08-10 : Compiled+Checked, Nh */
 PHQ=ANGL-DSTRN;
 CHM=ELM;
 PHYS-FORM=SLD;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=CYC;
 INST-ACC=2JPNINS;
 INC-ENGY-LAB-RANGE=51.9MEV;
 POL-PRJ=0%;
 DET-PARTCL=T;
 COINC=NO;
 ANT-COINC=NO;
 ANL=(DWBA'6',IBM);
 /* '6' program DWUCK */
 RCT=78KR(P,T)76KR;
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,1;
 INC-ENGY-LAB=51.9MEV;
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 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 EXC-ENGY-FINAL THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA
 (MEV) (DEG) (MB/SR) (MB/SR)
 2.260 1.119E+01 2.641E+01 +-NEGLIGIBLE
 2.260 1.274E+01 2.550E+01 +-NEGLIGIBLE
 2.260 1.304E+01 3.223E+01 +-NEGLIGIBLE
 2.260 1.521E+01 2.795E+01 +-NEGLIGIBLE
 2.260 1.753E+01 2.652E+01 +-NEGLIGIBLE
 2.260 2.016E+01 2.385E+01 +-NEGLIGIBLE
 2.260 2.279E+01 2.145E+01 +-NEGLIGIBLE
 2.260 2.543E+01 1.611E+01 +-NEGLIGIBLE
 2.260 2.791E+01 1.348E+01 +-NEGLIGIBLE
 2.260 3.039E+01 1.279E+01 +-NEGLIGIBLE
 2.260 3.302E+01 1.150E+01 +-NEGLIGIBLE
 2.260 3.551E+01 8.795E+00 +-NEGLIGIBLE
 2.260 3.830E+01 7.100E+00 +-NEGLIGIBLE
 2.260 4.081E+01 2.997E+00 +-3.422E-01
 2.260 4.591E+01 3.118E+00 +-3.198E-01
 2.260 5.084E+01 3.883E+00 +-NEGLIGIBLE
 2.872 1.338E+01 3.266E+01 +-NEGLIGIBLE
 2.872 1.492E+01 3.090E+01 +-NEGLIGIBLE
 2.872 1.552E+01 2.724E+01 +-NEGLIGIBLE
 2.872 1.769E+01 2.815E+01 +-NEGLIGIBLE
 2.872 1.999E+01 2.390E+01 +-NEGLIGIBLE
 2.872 2.246E+01 2.218E+01 +-NEGLIGIBLE
 2.872 2.522E+01 1.848E+01 +-NEGLIGIBLE
 2.872 2.767E+01 1.513E+01 +-NEGLIGIBLE
 2.872 3.026E+01 9.645E+00 +-1.289E+00
 2.872 3.289E+01 1.070E+01 +-NEGLIGIBLE
 2.872 3.520E+01 9.584E+00 +-NEGLIGIBLE
 2.872 3.797E+01 8.578E+00 +-NEGLIGIBLE
 2.872 4.042E+01 7.024E+00 +-NEGLIGIBLE
 2.872 4.301E+01 4.558E+00 +-NEGLIGIBLE
 2.872 4.790E+01 2.745E+00 +-3.666E-01
 2.872 5.285E+01 2.930E+00 +-3.907E-01
 \END;
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