DARPE: Search Results
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 /* NRDF D1910 Data No.7                                              */
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 /* Bibliography                                                      */
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 \\BIB,7;
 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,7;
 /* 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'23';
 /* '23' Cummulative yield */
 INC-ENGY-LAB=93.7MEV/A;
 CHRG-INC-ION=18+;
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 /* Descriptive Parameters                                            */
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 \\DATA,7;
 INC-ENGY-LAB=93.7MEV/A;
 TOT-ERR=X%'24';
 /* '24' 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)
 30 65 X 2.7 +-0.6 21090240
 30 69 1 0.4 +-0.1 49536
 30 72 X 0.4 +-0.2 167400
 31 66 X 5.2 +-1.5 33840
 31 67 X 10.7 +-0.7 281664
 32 69 X 7.5 +-1.3 140580
 33 71 X 8.2 +-0.5 233280
 34 72 X 1.4 +-0.2 725760
 34 73 0 6.9 +-0.6 25740
 34 75 X 13.5 +-1.0 10350720
 35 75 X 7.8 +-1.2 5832
 35 76 0 8.7 +-2.7 58320
 35 77 0 10.4 +-0.6 205632
 36 79 0 11.9 +-1.7 126144
 37 81 0 19.2 +-1.0 16488
 37 83 X 20.6 +-1.0 7447680
 37 84 0 2.7 +-0.3 2839968
 38 82 X 5.1 +-0.7 2207520
 38 83 0 14.9 +-1.5 116640
 38 85 0 27.0 +-1.2 5602176
 39 87 0 25.0 +-1.0 289440
 39 87 1 4.9 +-0.3 46440
 40 86 X 5.0 +-2.3 59400
 40 88 X 16.9 +-1.5 7205760
 40 89 0 19.6 +-0.9 282528
 41 90 0 21.1 +-1.0 52560
 42 90 X 4.7 +-0.9 20412
 43 93 0 18.0 +-1.9 9900
 43 95 0 20.2 +-0.9 72000
 44 95 X 7.3 +-1.5 5940
 44 97 X 19.6 +-0.9 250560
 45 99 1 20.1 +-1.6 16200
 45 101 1 25.8 +-1.9 374976
 46 99 X 17.9 +-2.0 1284
 46 100 X 10.3 +-0.8 313632
 46 101 X 22.7 +-2.3 30492
 47 103 0 13.9 +-2.6 3942
 47 104 0 12.0 +-3.5 4152
 47 105 0 27.8 +-1.5 3567456
 48 104 X 8.2 +-9.8 3462
 48 107 X 34.9 +-9.9 23400
 49 109 0 35.4 +-1.7 15120
 49 111 0 34.4 +-1.5 244512
 50 109 X 19.6 +-2.7 1080
 50 110 X 8.6 +-3.1 14400
 50 113 0 56.2 +-2.9 9944640
 51 113 X 34.3 +-1.6 400.2
 51 115 X 46.4 +-2.6 1926
 51 117 X 8.5 +-0.6 10080
 52 114 X 17.6 +-1.3 912
 52 116 X 32.3 +-2.7 8964
 52 117 X 36.6 +-3.0 3708
 52 118 X 23.5 +-2.9 518400
 52 119 0 40.9 +-2.0 57780
 52 121 0 47.6 +-2.8 1451520
 53 118 0 26.9 +-2.6 822
 53 119 X 46.7 +-2.7 1146
 53 121 X 91.2 +-4.6 7632
 53 123 X 88.8 +-5.3 47520
 54 122 X 42.0 +-3.2 72360
 54 123 X 56.7 +-2.8 7488
 54 125 0 65.9 +-3.3 60840
 54 127 0 44.0 +-2.2 3145824
 55 125 X 73.3 +-9.0 2700
 55 127 X 70.5 +-3.6 22500
 55 129 X 81.7 +-4.0 115560
 56 124 X 53.9 +-5.3 714
 56 126 X 30.4 +-3.5 6012
 56 128 X 58.7 +-2.9 209952
 56 131 0 73.0 +-3.7 1019520
 56 133 0 87.1 +-7.3 332389.44
 57 129 X 25.0 +-1.7 696
 57 131 X 82.4 +-6.4 3540
 58 130 X 30.7 +-4.4 1500
 58 131 0 69.5 +-1.3 600
 58 132 X 64.8 +-3.8 12636
 58 134 X 70.6 +-8.6 273024
 58 135 0 95.1 +-5.9 63360
 58 139 0 171.7 +-8.7 11897280
 59 137 X 102.5 +-9.9 4608
 59 139 X 189.2 +-9.6 15876
 60 135 0 24.0 +-3.4 744
 60 136 X 20.4 +-1.8 3042
 \END;
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