/*===================================================================*/
 /* NRDF D1912 Data No.19                                             */
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 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,19;
 D#=D1912;
 TITLE=/ Isovector and isoscalar spin-flip M1 strengths in 11B /;
 ATH=(T.KAWABATA'1', H.AKIMUNE'2', H.FUJIMURA'3', H.FUJITA'4',
      Y.FUJITA'5', M.FUJIWARA'6,7', K.HARA'8', K.Y.HARA'2',
      K.HATANAKA'6', T.ISHIKAWA'9', M.ITOH'6', J.KAMIYA'10', S.KISHI'3',
      M.NAKAMURA'11', K.NAKANISHI'6', T.NORO'12', H.SAKAGUCHI'3',
      Y.SHIMBARA'6', H.TAKEDA'13', A.TAMII'6', S.TERASHIMA'3',
      H.TOYOKAWA'14', M.UCHIDA'3', H.UENO'13', T.WAKASA'12',
      Y.YASUDA'3', H.P.YOSHIDA'6', M.YOSOI'3');
 INST-ATH=(2JPNTOK'1', 2JPNKON'2', 2JPNKTO'3', 3SAFWIT'4', 2JPNOSA'5',
           2JPNRCN'6', 2JPNJAE'7', 2JPNKEK'8', 2JPNTOH'9', 2JPNJAE'10',
           2JPNJPN'11', 2JPNKYU'12', 2JPNIPC'13', 2JPNJSR'14');
      /* '1' Center for Nuclear Study (CNS) */
      /* '2' Department of Physics */
      /* '3' Department of Physics */
      /* '4' School of Physics */
      /* '5' Department of Physics */
      /* '7' Advanced Photon Research Center */
      /* '9' Laboratory of Nuclear Science */
      /* '11' Wakayama Medical University, Wakayama */
      /* '12' Department of Physics */
 REF=PR/C;
 VLP=70(2004)034318;
 RCTS=(11B(3HE,T)11C, 11B(D,D)11B, 12C(D,D)12C, 11B(P,P)11B);
 PHQS=(ANGL-DSTRN, VCTR-ANALPW, TNSR-ANALPW, POL'15', POL-TRNSF'16',
       OPT-POTL-PARA);
 /* '15' Induced polarization */
 /* '16' Polarization transfer coefficient */
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,19;
 /* 2005-03-10 : Compiled, Kc + On */
 ENR=X%'17';
 /* '17' Contamining impurities in the 11B target were identified
         by the kinematic energy shift in the elastic scattering at
         backward angles, and those contributions were estimated to be
         less than 1, 0.8 and 0.08 % for 10B, 12C and 16O,
         respectively. */
 CHM=ELM;
 PHYS-FORM=SLD;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=CYC;
 INST-ACC=2JPNRCN;
 BEAM-INTNSTY=1[10PNA;
 POL-PRJ=X%'18';
 /* '18' 200-MeV polarized deuteron and 392-MeV polarized proton
         beams were used. Both beams were obtaned from the
         high-intensity polarized ion source [ K.Hatanaka et al., Nucl.
         Instrum. Methods Phs, Res. A 384(1997)575]. */
 ION-SOURCE=/ Polarized ion source /;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(MAG'19',MWDC'19',SCT'19');
 /* '19' Grand Raiden [M.Fujiwara et al., Nucl. Instrum. Methods
         Phys. Res. A 422(1999)484] for momentum analisis */
 ANL=DWIA'20';
 /* '20' Using a computer code DWBA98 */
 RCT=11B(D,D)11B;
 RTY=ELA-SCATT;
 PHQ=ANGL-DSTRN;
 THK-TGT=16.7MG/CM**2;
 BAC=SELF;
 INC-ENGY-LAB=200MEV;
 DET-PARTCL=D;
 ERS-DET=150KEV'51';
 /* '51' FWHM */
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,19;
 INC-ENGY-LAB=200MEV;
 EMT=D;
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA'52'
 (DEG) (MB/SR) (MB/SR)
 3.598 2872.191 +-85.757
 4.796 2683.871 +-83.216
 5.396 2510.934 +-67.300
 6.594 1955.198 +-58.329
 7.792 1510.156 +-15.126
 8.990 1034.401 +-11.007
 10.187 581.114 +-4.804
 11.384 351.388 +-3.210
 12.580 179.763 +-1.820
 13.776 99.791 +-1.156
 14.971 50.822 +-0.710
 16.165 33.792 +-0.544
 17.358 25.798 +-0.219
 18.551 22.026 +-0.188
 20.337 16.607 +-0.131
 21.527 13.720 +-0.110
 23.310 8.571 +-0.108
 24.497 6.318 +-0.087
 26.275 3.448 +-0.060
 27.459 2.475 +-0.049
 29.232 1.440 +-0.034
 30.412 1.093 +-0.029
 \END;
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