DARPE: Search Results
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 /* NRDF D1910 Data No.4                                              */
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 /* Bibliography                                                      */
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 \\BIB,4;
 D#=D1910;
 TITLE=/ Angular-momentum effect in the fusion reaction of 141Pr with
         40Ar projectiles /;
 PURPOSE=/ To attempt direct measurements of the cross sections for
           both particle evaporation and fission in the reaction of
           141Pr with 40Ar ions by a radiochemical method to elucidate
           the relation of the critical angular momenta with the
           measured cross sections /;
 ATH=(H.KUSAWAKE'1', T.SAITO'1', A.YOKOYAMA'1', K.TAKESAKO'1',
      N.TAKAHASHI'1', H.BABA'1', Y.OHKUBO'2', A.SHINOHARA'3');
 INST-ATH=(2JPNOSA'1', 2JPNIPC'2', 2JPNNAG'3');
      /* '1' Department of Chemistry and Laboratory of Nuclear Studies,
            Faculty of Science */
      /* '3' Department of Chemistry, Faculty of Science */
 REF=RCA;
 VLP=69(1995)65;
 RCTS=141PR(40AR,X)X;
 PHQS=(XSECTN'4', XSECTN'5');
 /* '4' Cummulative yield */
 /* '5' Independent yield */
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 /* Experimental Conditions                                           */
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 \\EXP,4;
 /* 2005-09-14 : Compiled, Kc + On */
 /* Related references 
    - U.Reus et al., AND, 29(1983)1.
    Reference from which data were used (Energies and half-lives for
    assignments of gamma-ray peaks)
 /* Additional results shown but not compiled
    - Mass distribution (Distribution of cummulative yields of the
      products in each foil)
 CHM=ELM;
 PHYS-FORM=SLD'6';
 /* '6' Metal foils */
 THK-TGT=(3MG/CM**2,6MG/CM**2);
 BAC=AL'7';
 /* '7' Target was sandwiched by Al catcher foils. In some runs, Al
        foils were replaced by graphite foils with nearly the same
        stopping power. */
 THK-BAC=XMG/CM**2'8';
 /* '8' Between 3-micrometer and 50 micro-meter */
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=CYC;
 INST-ACC=2JPNIPC'9';
 /* '9' RIKEN ring cyclotron (RRC) facility */
 POL-PRJ=0%;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=error'10';
 /* '10' Relative efficiencies of 10-15 % and resolution of around
         2 keV at 1.33 MeV */
 /* Experimental Method:
    - Activation (Irradiated typically 20 min for short-lived
      products and 2 hour for long-lived products)
    - Energy degradation by foils (Energy degration of 40Ar ions in
      target stack was calculated using the OSCAR code [K. Hata and H.
      Baba, INDC(NDS)-195-GZ, p131 (1988)].)
    - Gamma ray spectrometry (Assignments of gamma-ray peaks were
      made according to their energies and half-lives.)
 /* Analysis:
    - Decay curve analysis (Decay-growth analysis of observed
      photopeak intensities for cross section calculation)
 RCT=141PR(40AR,X)X;
 PHQ=XSECTN'17';
 /* '17' Independent yield */
 INC-ENGY-LAB=9.8MEV/A;
 CHRG-INC-ION=17+;
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 /* Descriptive Parameters                                            */
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 \\DATA,4;
 INC-ENGY-LAB=9.8MEV/A;
 TOT-ERR=X%'18';
 /* '18' Mainly due to statistical errors in counting gamma-ray
         emission and expected errors in the photoemission probability
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 /* Data Table                                                        */
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 \DATA;
 Z A ISOMER XSECTN DELTA-XSECTN HALF-LIFE
 (NODIM) (NODIM) (NODIM) (MB) (MB) (SEC)
 33 72 X 14.3 +-0.7 93600
 33 74 X 16.0 +-0.7 1536192
 33 76 X 7.7 +-1.0 94752
 37 82 1 19.2 +-1.3 23292
 37 84 1 11.5 +-0.7 1215.6
 39 84 1 0.9 +-0.2 2400
 39 86 0 18.5 +-2.1 53064
 39 86 1 17.8 +-0.8 2880
 39 88 X 9.3 +-0.9 9210240
 42 93 1 10.3 +-1.1 24660
 43 94 0 9.8 +-0.9 17568
 43 95 1 3.0 +-0.6 5270400
 43 96 0 11.6 +-0.6 369792
 45 99 0 2.5 +-0.6 1382400
 45 100 0 12.1 +-0.6 74880
 47 106 1 8.8 +-1.2 730944
 49 108 1 2.9 +-0.6 3480
 49 110 1 0.8 +-0.4 4146
 49 110 0 11.0 +-1.4 17640
 50 117 1 1.2 +-0.3 1137024
 51 116 0 3.3 +-2.1 948
 51 116 1 7.7 +-1.5 3618
 51 118 1 1.1 +-0.5 18000
 52 119 1 4.6 +-0.3 405216
 52 121 1 7.5 +-1.3 13305600
 53 120 0 1.7 +-0.6 4860
 53 120 1 4.6 +-0.4 3180
 56 129 1 10.4 +-3.1 7668
 56 131 1 2.0 +-0.7 876
 57 130 X 13.0 +-1.8 522
 57 132 0 8.4 +-1.3 17280
 57 132 1 17.7 +-6.0 1458
 58 133 0 14.9 +-1.9 17748
 58 137 1 16.0 +-1.3 123840
 59 136 X 21.9 +-1.9 786
 59 138 1 29.8 +-1.5 7560
 60 139 1 41.8 +-2.0 19800
 61 140 1 29.7 +-1.6 357
 \END;
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