DARPE: Search Results
 /*===================================================================*/
 /* NRDF D1909 Data No.3                                              */
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 /* Bibliography                                                      */
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 \\BIB,3;
 D#=D1909;
 TITLE=/ Total spin transfer in continuum for 90Zr(p,n) reaction at
         295 MeV /;
 ATH=(T.WAKASA'1', H.SAKAI'2,3', H.OKAMURA'4', H.OTSU'5', T.NONAKA'2',
      T.OHNISHI'3', K.YAKO'2', K.SEKIGUCHI'3', S.FUJITA'2', T.UESAKA'6',
      Y.SATOU'7', S.ISHIDA'3', N.SAKAMOTO'3', M.B.GREENFIELD'8',
      K.HATANAKA'9');
 INST-ATH=(2JPNKYU'1', 2JPNTOK'2', 2JPNIPC'3', 2JPNTOH'4', 2JPNTOH'5',
           2JPNTOK'6', 2JPNTIT'7', 2JPNICU'8', 2JPNRCN'9');
      /* '1' Department of Physics */
      /* '2' Department of Physics */
      /* '4' Cyclotron and Radioisotope Center */
      /* '5' Department of Physics */
      /* '6' Center for Nuclear Study */
      /* '7' Department of Physics */
      /* '8' Division of Natural Science */
 REF=JPJ;
 VLP=73(2004)1611;
 RCTS=90ZR(P,N)90NB;
 PHQS=(DBL-DIFF-XSECTN, POL-TRNSF, POL-TRNSF'10', POL-TRNSF'11',
       TRNSN-STRGTH);
 /* '10' Total spin transfer */
 /* '11' f1=(1-2DNN + DLL)/2(1+DLL) */
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,3;
 /* 2005-04-14 : Compiled, Kc + On */
 ENR=X%;
 CHM=ELM;
 PHYS-FORM=SLD;
 BAC=X;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=CYC'12';
 /* '12' Neutron time-of-flight facility */
 INST-ACC=2JPNRCN;
 INC-ENGY-LAB=295MEV;
 BEAM-INTNSTY=[13NA;
 POL-PRJ=0.50[0.73%;
 DET-PARTCL=N;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(X'13',TOF);
 /* '13' Details of the neutron detection system are shown in [H.
         Sakai et al., Nucl. Instrm. Methods Phys. Res., Sec. A
         320(1992)479]. */
 /* Experimental Method:
    - Time-of-flight
 RCT=90ZR(P,N)90NB;
 PHQ=POL-TRNSF;
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 /* Descriptive Parameters                                            */
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 \\DATA,3;
 INC-ENGY-LAB=295MEV;
 STATIST-ERR=X%'16';
 /* '16' Statistical uncertainties in D(ii) at 0 deg. are in the
         range of 0.03 - 0.08 around the peak of the Gamow-Teller
         excitation and its giant resonance. */
 THTL=0DEG;
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 /* Data Table                                                        */
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 \DATA;
 EXC-ENGY DNN DELTA-DNN'17'
 (MEV) (NODIM) (NODIM)
 6.153E-01 -8.228E-02 +-1.013E-01
 1.547E+00 -1.646E-01 +-5.696E-02
 2.649E+00 -2.215E-01 +-5.063E-02
 3.672E+00 -6.329E-02 +-3.797E-02
 4.607E+00 -6.329E-03 +-6.329E-02
 5.625E+00 -3.165E-02 +-3.797E-02
 6.725E+00 -1.772E-01 +-5.063E-02
 7.658E+00 -1.962E-01 +-3.797E-02
 8.677E+00 -2.025E-01 +-3.165E-02
 9.781E+00 -2.025E-01 +-3.165E-02
 1.063E+01 -1.962E-01 +-2.532E-02
 1.165E+01 -2.405E-01 +-3.165E-02
 1.284E+01 -1.772E-01 +-3.797E-02
 1.368E+01 -2.722E-01 +-5.063E-02
 1.462E+01 -2.025E-01 +-3.797E-02
 1.572E+01 -3.101E-01 +-3.797E-02
 1.674E+01 -1.519E-01 +-4.430E-02
 1.767E+01 -2.785E-01 +-3.797E-02
 1.878E+01 -2.595E-01 +-NEGLIGIBLE
 1.963E+01 -1.899E-01 +-5.063E-02
 2.073E+01 -2.152E-01 +-4.430E-02
 2.175E+01 -2.405E-01 +-3.165E-02
 2.268E+01 -2.215E-01 +-4.430E-02
 2.370E+01 -2.468E-01 +-5.696E-02
 2.464E+01 -1.899E-01 +-4.430E-02
 2.574E+01 -1.899E-01 +-4.430E-02
 2.676E+01 -2.911E-01 +-5.063E-02
 2.777E+01 -3.354E-01 +-5.063E-02
 2.871E+01 -1.772E-01 +-5.063E-02
 2.964E+01 -2.468E-01 +-5.696E-02
 3.066E+01 -3.038E-01 +-5.063E-02
 3.176E+01 -2.911E-01 +-5.063E-02
 3.261E+01 -3.101E-01 +-5.696E-02
 3.372E+01 -1.582E-01 +-5.063E-02
 3.457E+01 -1.582E-01 +-5.063E-02
 3.576E+01 -1.772E-01 +-5.063E-02
 3.686E+01 -2.278E-01 +-6.962E-02
 3.762E+01 -1.962E-01 +-5.696E-02
 3.873E+01 -2.025E-01 +-6.329E-02
 4.068E+01 -1.266E-01 +-6.962E-02
 4.187E+01 -1.962E-01 +-6.962E-02
 4.263E+01 -1.266E-01 +-6.962E-02
 4.374E+01 -1.899E-01 +-6.329E-02
 4.459E+01 -1.582E-01 +-6.329E-02
 4.569E+01 -1.646E-01 +-5.696E-02
 4.679E+01 -8.861E-02 +-6.329E-02
 4.764E+01 -1.582E-01 +-6.329E-02
 4.874E+01 -2.278E-01 +-6.962E-02
 4.977E+01 -1.013E-01 +-7.595E-02
 \END;
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