DARPE: Search Results
 /*===================================================================*/
 /* NRDF D1702 Data No.11                                             */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,11;
 D#=D1702;
 TITLE=/ Mechanism of the forward-angle (d,pn) reaction at
         intermediate energies /;
 ATH=(H.OKAMURA'1', S.ISHIDA'1', N.SAKAMOTO'1', H.OTSU'1', T.UESAKA'1',
      T.WAKASA'1', H.SAKAI'1', T.NIIZEKI'2', H.TOYOKAWA'2', Y.TAJIMA'2',
      H.OHNUMA'2', M.YOSOI'3', K.HATANAKA'4', T.ICHIHARA'5');
 INST-ATH=(2JPNTOK'1', 2JPNTIT'2', 2JPNKTO'3', 2JPNRCN'4',
           2JPNIPC'5');
      /* '1' Department of Physics */
      /* '2' Department of Physics */
      /* '3' Department of Physics */
 REF=PR/C;
 VLP=58(1998)2180;
 /* '6' Main reference, Analysis with Coulomb and nuclear
        interaction given */
 /* Secondary reference 
    - PL/B, 424(1998)219 (J.A.Tostevin et al., Analysis with Coulomb
      interaction given)
 RCTS=(208PB(D,N,P)208PB, 165HO(D,N,P)165HO, 118SN(D,N,P)118SN,
       90ZR(D,N,P)90ZR, 40CA(D,N,P)40CA, 28SI(D,N,P)28SI,
       12C(D,N,P)12C, 208PB(D,D)208PB, 40CA(D,D)40CA, 12C(D,D)12C);
 PHQS=(ENGY-SPEC, X'7', OPT-POTL-PARA, ANGL-DSTRN, XSECTN-RATIO,
       ANGL-CORRL);
 /* '7' Incident energy dependence of dsigma/domega/domega at 0deg
    for neutron and proton */
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,11;
 /* 2002-07-26 : Converted, Ay + On. Data converted to EXFOR E1702
 /* 2004-01-22 : Altered, On. Data replaced by data sent from
    author. Data for Fig.6 (0 deg) are deleted, which are repetition
    of bottom panel of Fig.5. Absolute cross sections and Rutherford
    ratios for elastic channels are added. */
 /* 2010-01-07 : Altered, Nf. 030-035: CRITIQUE added */
 ENR=X%'8';
 /* '8' Natural or isotropically enriched */
 CHM=ELM;
 PHYS-FORM=SLD;
 THK-TGT=XMG/CM**2;
 BAC=SELF;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=CYC;
 INST-ACC=2JPNIPC'9';
 /* '9' RIKEN Accelerator Research Facility (RARF) */
 BEAM-INTNSTY=0.01[0.4NA;
 POL-PRJ=0%;
 ANT-COINC=NO;
 DET-SYS=(MAG'10',MWDC,SCT'11');
 /* '10' Spectrograph SMART, to detect proton, See [T.Ichihara et
         al., Nucl.Phys.A569(1994)287c]. */
 /* '11' Liquid scintillator to detect neutron */
 ERS-DET=2.5MEV;
 CALB-DET=/ The neutron detection efficiency was calibrated using the
            7Li(p,n)7Be(g.s.+0.43MeV) reaction at Ep=70MeV and 135MeV.
 ANL=DWBA;
 /* Author's comments: Large solid angle of detector used in this
    experiment must be considered. Real data are expected to
    drastically vary in each solid angle. After this experiment,
    authors did another experiment with better angular resolution.
    Publication of new data is planned. */
 /* 2004-08-17 : Altered, On. Particle field of EN-SEC corrected */
 RCT=90ZR(D,N,P)90ZR;
 PHQ=ENGY-SPEC;
 INC-ENGY-LAB-RANGE=270MEV;
 DET-PARTCL=(N,P);
 COINC=(N,P);
 SOLID-ANGL=XMSR'33';
 /* '33' 0.48 msr for neutron and 60x120 mrad**2 for proton */
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,11;
 SYS-ERR=30%'12';
 /* '12' The systematic error, including those arising from
         uncertainties of the beam intensity and the target thickness,
         is estimated to be 30%. */
 INC-ENGY-LAB=270MEV;
 EMT-1=N;
 EMT-2=P;
 THTL-1=0DEG;
 THTL-2=0DEG;
 EXC-ENGY=0.0MEV;
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 ENGY-EMT-LAB DSIGMA/DOMEGA/DOMEGA/DE
 DELTA-DSIGMA/DOMEGA/DOMEGA/DE'34'
 (MEV) (MB/SR**2/MEV) (MB/SR**2/MEV)
 108.50 1452.8 +-68.165
 109.50 1641.7 +-72.466
 110.50 1925.5 +-78.544
 111.50 2036.1 +-80.754
 112.50 2234.1 +-84.617
 113.50 2417.5 +-88.008
 114.50 2788.1 +-94.559
 115.50 2793.5 +-94.740
 116.50 3090.8 +-99.492
 117.50 3179.6 +-100.97
 118.50 3415.8 +-104.69
 119.50 3454.6 +-105.26
 120.50 3373.8 +-104.16
 121.50 3298.5 +-102.88
 122.50 3535.3 +-106.75
 123.50 3521.9 +-106.41
 124.50 3454.1 +-105.44
 125.50 2925.2 +-97.125
 126.50 3186.1 +-101.33
 127.50 2685.0 +-93.207
 128.50 2928.0 +-97.413
 129.50 2768.4 +-94.504
 130.50 2766.6 +-94.360
 131.50 2691.1 +-93.405
 132.50 2854.9 +-96.154
 133.50 2832.5 +-95.885
 134.50 2749.9 +-94.611
 135.50 2694.7 +-93.697
 136.50 2865.4 +-96.529
 137.50 2717.2 +-93.848
 138.50 2943.1 +-97.672
 139.50 2956.5 +-97.890
 140.50 3294.1 +-103.20
 141.50 3547.2 +-107.02
 142.50 3776.9 +-110.39
 143.50 3816.1 +-111.14
 144.50 4096.7 +-115.08
 145.50 3838.1 +-111.12
 146.50 3916.7 +-112.23
 147.50 3955.0 +-112.78
 148.50 3931.7 +-112.44
 149.50 3797.8 +-110.62
 150.50 3758.6 +-109.80
 151.50 3503.3 +-105.93
 152.50 3295.7 +-102.67
 153.50 2960.2 +-97.359
 154.50 2868.5 +-95.843
 155.50 2261.2 +-85.178
 156.50 2138.7 +-82.588
 157.50 2015.3 +-80.039
 158.50 1719.7 +-73.975
 159.50 1502.7 +-69.198
 160.50 1255.6 +-63.401
 161.50 1015.9 +-56.784
 162.50 971.01 +-55.583
 163.50 698.41 +-47.242
 164.50 569.31 +-42.551
 165.50 497.52 +-39.705
 166.50 433.45 +-37.055
 167.50 378.31 +-34.604
 168.50 346.52 +-33.098
 169.50 248.03 +-27.987
 170.50 127.04 +-20.019
 171.50 79.980 +-15.868
 172.50 29.607 +-9.6507
 173.50 42.469 +-12.743
 174.50 21.523 +-8.2252
 175.50 18.250 +-12.915
 \END;
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