DARPE: Search Results
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 /* NRDF D0021 Data No.1                                              */
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 /* Bibliography                                                      */
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 \\BIB,1;
 D#=D21;
 TITLE=/ Difference in analyzing powers for (p,t) reactions due to a
         phase change of interference between direct and indirect
         processes in two-nucleon transfer reactions /;
 ATH=(K.YAGI'1', S.KUNORI'1', Y.AOKI'1', Y.HIGASHI'1', J.SANADA'1',
      Y.TAGISHI'1');
 INST-ATH=(2JPNTSU'1');
      /* '1' Institute of Physics and Tandem Accelerator Center */
 REF=PRL;
 VLP=40(1978)161;
 RCTS=(128TE(P,T)126TE, 110PD(P,T)108PD);
 PHQS=(VCTR-ANALPW, ANGL-DSTRN);
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 /* Experimental Conditions                                           */
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 \\EXP,1;
 /* 2009-08-21 : Compiled+Checked, Nh */
 /* Related references 
    - R.B.Firestone et al., FIRESTONE, (1996).
    (Level energies of 1st 2+ states are not given in K.Yagi et al.
    J.PRL,40,161,1978, and taken from this book by compiler.)
 ENR=X%'2';
 /* '2' Enriched sample */
 CHM=ELM;
 PHYS-FORM=SLD;
 THK-TGT=0.5MG/CM**2;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=VDG'3';
 /* '3' 12UD Pelletron */
 INST-ACC=2JPNTSU'4';
 /* '4' 12UD Pelletron */
 INC-ENGY-LAB-RANGE=22.0MEV;
 BEAM-INTNSTY=50NA;
 POL-PRJ=85+-2%;
 ION-SOURCE=/ Lamb-shift source /;
 DET-PARTCL=T;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(MAG,SI);
 ERS-DET=40KEV;
 ANL=(CCBA,RPA);
 RCT=128TE(P,T)126TE;
 PHQ=VCTR-ANALPW;
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 /* Descriptive Parameters                                            */
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 \\DATA,1;
 INC-ENGY-LAB=22.0MEV;
 DELTA-THTL=1.5DEG;
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 /* Data Table                                                        */
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 \DATA;
 EXC-ENGY'5' THTC AY DELTA-AY FLAG'6'
 (KEV) (DEG) (NODIM) (NODIM) (NODIM)
 0.0 1.502E+01 -5.719E-03 +-3.158E-02 1.
 0.0 2.024E+01 4.494E-02 +-5.369E-02 1.
 0.0 2.501E+01 1.619E-01 +-3.158E-02 1.
 0.0 3.008E+01 1.336E-01 +-3.158E-02 1.
 0.0 3.517E+01 2.004E-02 +-3.158E-02 1.
 0.0 4.025E+01 -1.567E-01 +-3.474E-02 1.
 0.0 4.519E+01 -4.250E-01 +-4.105E-02 1.
 0.0 5.011E+01 -3.554E-01 +-4.736E-02 1.
 666.338 1.525E+01 7.317E-02 +-3.913E-02 2.
 666.338 2.049E+01 9.973E-02 +-4.226E-02 2.
 666.338 2.527E+01 1.200E-01 +-4.696E-02 2.
 666.338 2.989E+01 4.175E-02 +-3.443E-02 2.
 666.338 3.544E+01 3.701E-02 +-4.852E-02 2.
 666.338 4.068E+01 1.506E-02 +-4.539E-02 2.
 666.338 4.576E+01 -8.045E-02 +-5.635E-02 2.
 666.338 5.069E+01 -5.858E-02 +-4.383E-02 2.
 \END;
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