DARPE: Search Results
 /*===================================================================*/
 /* NRDF D1702 Data No.13                                             */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,13;
 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,13;
 /* 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=28SI(D,N,P)28SI;
 PHQ=ENGY-SPEC;
 INC-ENGY-LAB-RANGE=270MEV;
 DET-PARTCL=(N,P);
 COINC=(N,P);
 SOLID-ANGL=XMSR'37';
 /* '37' 0.48 msr for neutron and 60x120 mrad**2 for proton */
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,13;
 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'38'
 (MEV) (MB/SR**2/MEV) (MB/SR**2/MEV)
 108.50 222.79 +-24.388
 109.50 313.89 +-28.946
 110.50 327.53 +-29.645
 111.50 331.96 +-29.769
 112.50 395.46 +-32.649
 113.50 463.53 +-35.279
 114.50 458.19 +-35.134
 115.50 470.57 +-35.522
 116.50 531.98 +-37.853
 117.50 537.27 +-37.953
 118.50 551.21 +-38.652
 119.50 581.78 +-39.961
 120.50 618.61 +-40.845
 121.50 635.33 +-41.542
 122.50 625.06 +-41.126
 123.50 575.56 +-39.379
 124.50 688.73 +-43.443
 125.50 558.50 +-39.082
 126.50 558.94 +-39.313
 127.50 521.41 +-37.944
 128.50 542.86 +-38.802
 129.50 506.12 +-37.832
 130.50 484.94 +-37.158
 131.50 502.23 +-37.385
 132.50 474.87 +-37.030
 133.50 520.75 +-38.184
 134.50 467.80 +-36.867
 135.50 516.49 +-38.111
 136.50 457.49 +-36.170
 137.50 455.39 +-35.685
 138.50 426.13 +-34.384
 139.50 377.49 +-32.388
 140.50 448.48 +-35.566
 141.50 477.05 +-37.008
 142.50 544.45 +-39.127
 143.50 494.83 +-36.916
 144.50 498.74 +-37.194
 145.50 477.98 +-36.140
 146.50 482.42 +-36.316
 147.50 564.08 +-39.348
 148.50 612.07 +-40.922
 149.50 522.91 +-37.811
 150.50 577.93 +-39.656
 151.50 541.53 +-38.432
 152.50 507.19 +-37.164
 153.50 471.28 +-35.525
 154.50 409.54 +-33.571
 155.50 425.14 +-33.794
 156.50 352.35 +-30.726
 157.50 300.78 +-28.384
 158.50 319.58 +-29.429
 159.50 232.15 +-24.887
 160.50 257.92 +-26.249
 161.50 185.44 +-22.505
 162.50 161.31 +-20.927
 163.50 139.59 +-19.234
 164.50 113.56 +-17.346
 165.50 104.00 +-16.597
 166.50 82.918 +-14.817
 167.50 67.466 +-13.794
 168.50 43.508 +-10.730
 169.50 30.265 +-8.9476
 170.50 45.306 +-11.911
 171.50 18.132 +-8.5351
 172.50 18.310 +-7.6917
 173.50 16.608 +-11.744
 \END;
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