/*===================================================================*/
 /* NRDF D0815 Data No.8                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,8;
 D#=D815;
 TITLE=/Analyzing power of the neutron continuum spectrum for the
        93Nb(p,nX) reaction at 65 MeV and a DWBA analysis/;
 PURPOSE=/To provide stringent test for various theories by simultaneous
          fitting of analyzing powers as well as cross sections for both
          neutron and proton spectra/;
 ATH=(H.SAKAI'1', K.HATANAKA'1', N.MATSUOKA'1', T.SAITO'1',
      A.SHIMIZU'1', T.MOTOBAYASHI'2', T.SHIBATA'1');
 INST-ATH=(2JPNRCN'1', 2JPNOSA'2');
      /* '2' Department of Physics */
 REF=PL/B;
 VLP=133(1983)375;
 RCTS=93NB(P,N)X;
 PHQS=(ENGY-SPEC'3', ANALPW, ANGL-DSTRN);
 /* '3' Double differential cross section */
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,8;
 /* 2003-10-24 : Converted, Data converted to EXFOR E815 and EXFOR
    O0522 */
 ENR=X%;
 CHM=ELM;
 PHYS-FORM=SLD'4';
 /* '4' Metallic foil */
 THK-TGT=43.6MG/CM**2;
 BAC=SELF;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=CYC'5';
 /* '5'Isochronous cyclotron, RCNP AVF cyclotron */
 INST-ACC=2JPNRCN;
 INC-ENGY-LAB=65MEV;
 BEAM-INTNSTY=50NA'6';
 /* '6' maximum beam current */
 POL-PRJ=82.5+-2.5%'7';
 /* '7' The beam polarization was measured continuously with a
        12C-polarimeter placed down stream the main scattering chamber
 DET-PARTCL=N;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=SCT'8';
 /* '8' two liquid scintillation counters (NE213) to detect
        neutrons */
 /* Experimental Method:
    - Time-of-flight (To determine outgoing neutron energy. The time
      resolution (FWHM) of the beam burst was typically 1.0-1.5 ns, and
      corresponding energy resolutions of the neutrons were about 4 and
      2 MeV for 50 and 30 MeV neutrons, respectively.)
 RCT=93NB(P,N)X;
 PHQ=ANALPW;
 ANL=DWBA'35';
 /* '35' with the code DWBA74 [R.Shaeffer et al., unpublished]
         which includes knock-on exchange amplitudes. A microscopic
         form factor was employed. The effective two-body interaction
         was taken from [G.Bertsch et al., Nucl. Phys. A284(1977)399].
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,8;
 INC-ENGY-LAB=65MEV;
 SYS-ERR=10%'36';
 /* '36' Estimated errors in the absolute magnitude of the cross
         section due to uncertainties in the neutron detection
         efficiency calculation */
 EMT=N;
 EXC-ENGY-MIN=12MEV;
 EXC-ENGY-MAX=16MEV;
 DELTA-THTL=+-0.6DEG'37';
 /* '37' Data-point reader uncertainty */
 DELTA-ANALPW=+-0.6%'38';
 /* '38' Data-point reader uncertainty */
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 THTL ANALPW DELTA-ANALPW'39'
 (DEG) (NODIM) (%)
  15.9      0.012         +-2.
  25.      -0.008         +-X
  33.6      0.091         +-X
  51.7      0.248         +-3.
  65.7      0.212         +-X
  86.2      0.138         +-X
 106.2      0.116         +-X
 126.7      0.081         +-X
 \END;
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