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 /* NRDF D1816 Data No.62                                             */
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 /* Bibliography                                                      */
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 \\BIB,62;
 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);
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,62;
 /* 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        of Colorado, unpublished].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=SPEC-FCTR;
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 /* Descriptive Parameters                                            */
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 \\DATA,62;
 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;
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 /* Data Table                                                        */
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 \DATA;
 EXC-ENGY DELTA-EXC-ENGY TRNSF-L J-PTY SQRT-C2S
 (MEV) (KEV) (NODIM) (NODIM) (NODIM)
 0.000 +-X 0 1/2+ 0.15
 0.099 +-2 2 5/2+ 1.90
 0.233 +-5 4 7/2+ 1.32
 0.355 +-7 2 3/2+ 0.07
 0.541 +-15 0 1/2+ 0.19
 0.621 +-20 2 5/2+ 0.30
 0.686 +-17 X X X
 0.789 +-9 2 3/2+ 0.13
 0.909 +-15 0 1/2+ 0.06
 0.952 +-15 2 5/2+ 0.16
 1.047 +-23 X X X
 1.182 +-17 2 3/2+ 0.15
 1.262 +-27 0 1/2+ 0.01
 1.340 +-28 4 7/2+ 0.25
 1.382 +-12 X X X
 1.489 +-36 2 5/2+ 0.08
 1.549 +-36 2 3/2+ 0.20
 1.744 +-36 2 5/2+ 0.08
 1.832 +-38 1 1/2- 0.06
 1.947 +-38 X X X
 2.064 +-50 1 1/2- 0.03
 2.087 +-50 1 1/2- 0.07
 2.145 +-50 4 9/2+ 1.65
 2.203 +-50 1 1/2- 0.24
 2.373 +-50 1 3/2- 0.23
 2.473 +-50 1 3/2- 0.30
 2.579 +-50 1 1/2- 0.18
 2.650 +-50 1 3/2- 0.07
 2.743 +-50 1 1/2- 0.07
 2.774 +-50 1 1/2- 0.06
 2.847 +-50 X X X
 2.921 +-50 1 1/2- 0.18
 \END;
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