DARPE: Search Results
 /*===================================================================*/
 /* NRDF D1702 Data No.12                                             */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,12;
 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,12;
 /* 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=40CA(D,N,P)40CA;
 PHQ=ENGY-SPEC;
 INC-ENGY-LAB-RANGE=270MEV;
 DET-PARTCL=(N,P);
 COINC=(N,P);
 SOLID-ANGL=XMSR'35';
 /* '35' 0.48 msr for neutron and 60x120 mrad**2 for proton */
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,12;
 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'36'
 (MEV) (MB/SR**2/MEV) (MB/SR**2/MEV)
 108.50 497.90 +-32.539
 109.50 605.21 +-35.926
 110.50 704.80 +-38.762
 111.50 752.21 +-40.039
 112.50 771.08 +-40.553
 113.50 798.98 +-41.273
 114.50 844.35 +-42.483
 115.50 873.39 +-43.245
 116.50 1016.3 +-46.631
 117.50 1006.0 +-46.362
 118.50 1104.6 +-48.725
 119.50 1060.7 +-47.653
 120.50 1117.3 +-48.841
 121.50 1050.6 +-47.480
 122.50 1053.3 +-47.571
 123.50 920.99 +-44.437
 124.50 1014.8 +-46.728
 125.50 882.04 +-43.663
 126.50 959.36 +-45.678
 127.50 831.05 +-42.461
 128.50 859.50 +-43.081
 129.50 779.80 +-41.273
 130.50 794.55 +-41.786
 131.50 762.50 +-40.871
 132.50 779.75 +-41.434
 133.50 741.80 +-40.294
 134.50 733.86 +-40.176
 135.50 783.10 +-41.359
 136.50 702.96 +-39.330
 137.50 814.25 +-42.248
 138.50 790.06 +-41.609
 139.50 873.16 +-43.483
 140.50 944.18 +-45.379
 141.50 918.23 +-44.843
 142.50 984.54 +-46.139
 143.50 974.08 +-46.044
 144.50 982.58 +-46.185
 145.50 1018.0 +-46.876
 146.50 1008.6 +-46.716
 147.50 1046.4 +-47.498
 148.50 1105.9 +-48.785
 149.50 1034.2 +-47.189
 150.50 1013.0 +-46.587
 151.50 928.83 +-44.685
 152.50 856.64 +-43.036
 153.50 872.81 +-43.182
 154.50 700.08 +-38.540
 155.50 607.35 +-36.167
 156.50 571.42 +-34.810
 157.50 587.40 +-35.274
 158.50 450.54 +-31.025
 159.50 436.39 +-30.357
 160.50 332.08 +-26.477
 161.50 340.19 +-26.840
 162.50 293.20 +-24.870
 163.50 273.56 +-24.164
 164.50 207.48 +-20.914
 165.50 161.45 +-18.524
 166.50 131.93 +-16.671
 167.50 101.12 +-14.697
 168.50 45.060 +-9.7330
 169.50 29.410 +-7.8587
 170.50 43.525 +-9.5558
 171.50 26.584 +-7.4592
 172.50 17.260 +-6.0085
 173.50 13.653 +-5.8222
 174.50 17.523 +-10.671
 175.50 23.314 +-16.485
 176.50 11.930 +-8.4492
 \END;
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