/*===================================================================*/
 /* NRDF D0815 Data No.7                                              */
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 /* Bibliography                                                      */
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 \\BIB,7;
 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,7;
 /* 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=ANGL-DSTRN;
 ANL=DWBA'31';
 /* '31' with the code DWBA74 [R.Shaeffer et al., unpublished]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,7;
 INC-ENGY-LAB=65MEV;
 SYS-ERR=10%'32';
 /* '32' 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'33';
 /* '33' Data-point reader uncertainty */
 DELTA-DSIGMA/DOMEGA/DE=+-4.0%'34';
 /* '34' Data-point reader uncertainty */
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 THTL DSIGMA/DOMEGA/DE
 (DEG) (MB/SR/MEV)
   0.    4.92
  18.3   2.5
  28.5   1.19
  38.6   0.92
  53.7   0.428
  68.3   0.163
  88.2   6.28E-02
 109.9   1.93E-02
 128.4   1.17E-02
 \END;
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