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 /* NRDF D1816 Data No.61                                             */
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 /* Bibliography                                                      */
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 \\BIB,61;
 D#=D1816;
 TITLE=/100Mo(p,d)99Mo reaction at 21 MeV and direct reaction analysis
        of the low-lying continuum spectrum/;
 PURPOSE=/To discuss the nuclear structure models of the 3s-1g shell
          nuclei/;
 ATH=(S.HIROWATARI'1', SYAFARUDIN'1', F.ARAMAKI'1', A.NOHTOMI'1',
      G.WAKABAYASHI'1', Y.UOZUMI'1', N.IKEDA'1', M.MATOBA'1', Y.AOKI'2',
      K.HIROTA'2', N.OKUMURA'2', T.JOH'2');
 INST-ATH=(2JPNKYU'1', 2JPNTSU'2');
      /* '1' Department of Nuclear Engineering */
      /* '2' Tandem Accelerator Center */
 REF=NP/A;
 VLP=714(2003)3;
 RCTS=100MO(P,D)99MO;
 PHQS=(ANGL-DSTRN, VCTR-ANALPW, OPT-POTL-PARA, SPEC-FCTR);
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 /* Experimental Conditions                                           */
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 \\EXP,61;
 /* 2003-09-04 : Compiled */
 RTY=POL-RCT;
 /* Additional result not compiled:
    - Energy distribution (Typical deuteron energy spectrum (theta=20
      deg) given in Fig.1, p6 in reference)
 ENR=97.27%;
 CHM=ELM;
 PHYS-FORM=SLD;
 THK-TGT=0.505MG/CM**2;
 BAC=X;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=VDGT;
 INST-ACC=2JPNTSU'3';
 /* '3' Tandem Accelerator Center */
 INC-ENGY-LAB=21MEV;
 BEAM-INTNSTY=40[200NA;
 POL-PRJ=[80%;
 DET-PARTCL=D;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(MAG'4',PROP-CNTR'5');
 /* '4' ESP-90 [M.Matoba et al., Nucl. Instrum. Methods
        196(1982)257, H.Iida et al., Nucl. Instrum. Methods
        224(1984)432]. */
 /* '5' Position sensitive */
 ERS-DET=<50KEV'6';
 /* '6' About 50 keV (in FWHM) for the region above 2 MeV, and
        better than 40 keV for the lower region */
 CALB-DET=/ Energy calibration of spectrum was performed by remapping
            some positions - which was done by adjusting the strength
            of the magnetic field - of well-known low-lying levels in
            99Mo, namely ground state, 0.0978, 0.2355, 0.3512 and
            0.6150, over a wide region in the spectrum. /;
 ANL=DWBA'7';
 /* '7' Differential cross section and analyzing power data were
        analyzed with DWBA code DWUCK [P.D.Kunz, code DWUCK, University
        of Colorado, unpublished]. */
 RCT=100MO(P,D)99MO;
 PHQ=OPT-POTL-PARA;
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 /* Descriptive Parameters                                            */
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 \\DATA,61;
 INC-ENGY-LAB=21MEV;
 NORM=/ Normalization of cross section was performed by scaling the
        measured p+100Mo elastic scattering cross section to an optical
        model prediction using parameters of global potentials
        [F.D.Becchetti Jr. and G.W.Greenlees, Phys.Rev.182(1969)1190].
 RSD=99MO;
 POTL-FORM=/ unknown /;
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 /* Data Table                                                        */
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 \DATA;
 V RR AR RC WV RIV AIV WS RIS AIS VSO RRSO ARSO DATA1'62'
 DATA2'63' FLAG'64'
 (MEV) (FM) (FM) (FM) (MEV) (FM) (FM) (MEV) (FM) (FM) (MEV) (FM)
 (FM) (FM) (FM) (NODIM)
 54.74 1.17 0.75 1.25 1.92 1.32 0.62 8.47 1.32 0.62 6.20 1.01 0.75 0.85
 0.621 1
 X 1.17 0.78 1.25 X 1.29 0.63 X 1.29 0.63 6.20 1.06 0.75 0.85 X 2
 X 1.25 0.65 X X X X X X X X X X 0.54 X 3
 \END;
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