/*===================================================================*/
 /* NRDF D1885 Data No.2                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,2;
 D#=D1885;
 TITLE=/ Half-life of 228Pu and alpha decay of 228Np /;
 PURPOSE=/ To determine evaporation residue cross sections for 228Pu,
          228Np, and 225U /;
 ATH=(K.NISHIO'1', H.IKEZOE'1', S.MITSUOKA'1', K.SATOU'1', C.J.LIN'1,
     2');
 INST-ATH=(2JPNJAE'1', 3CPRAEP'2');
      /* '1' Advanced Science Research Center */
 REF=PR/C;
 VLP=68(2003)064305;
 RCTS=(198PT(34S,4*N)228PU, 198PT(34S,3*N,P)228NP,
       198PT(34S,3*N,ALPHA)225U);
 PHQS=(XSECTN, HALF-LIFE);
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,2;
 /* 2004-04-13 : Compiled, Kc + On */
 ENR=98%;
 CHM=ELM;
 PHYS-FORM=SLD;
 THK-TGT=0.39MG/CM**2;
 BAC=AL;
 THK-BAC=XMG/CM**2'3';
 /* '3' 1.2 micro-meter thick foil */
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=VDGT;
 INST-ACC=2JPNJAE;
 INC-ENGY-CM=141[143MEV'4';
 /* '4' Energy at the half depth of the target layer determined
        by calculating the energy loss of beam in the Al foil and target
 BEAM-INTNSTY=40[50PNA;
 POL-PRJ=0%;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(MAG'5',SI'6');
 /* '5' JAERI Recoil Mass Separator used to separate evaporation
        residue from the primary beams and other reaction products. */
 /* '6' Double-sided position-sensitive silicon detector (73x55
        mm**2) to construct alpha-decay chain. Typical energy
        resolution of PSD for alpha particle from an 241Am source. */
 /* Related references 
    - R.B.Firestone, FIRESTONE, (1996).
    (Kinetic energy of alpha particles and half-life of this literature
    are tabulated for other than 228Np.)
    - S.A.Kreek et al., PR/C, 50(1994)2288.
    (Kinetic energy of alpha particles and half-life of this literature
    are tabulated for 228Np.)
 RCT=198PT(34S,3*N,P)228NP;
 PHQ=XSECTN;
 DET-PARTCL=(ALPHA'13',ALPHA'14',ALPHA'15',ALPHA'16',ALPHA'17');
 /* '13' Alpha from 228Np */
 /* '14' Alpha from 224Pa */
 /* '15' Alpha from 220Ac */
 /* '16' Alpha from 216Fr */
 /* '17' Alpha from 212At (ground state) */
 /* Comment to data: T1/2 (228Np) = 56+45-17 sec is determined by
    authors. */
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,2;
 RSD=228NP;
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 INC-ENGY-CM XSECTN XSECTN-MAX'18' DELTA-XSECTN
 (MEV) (NB) (NB) (NB)
 141.0 X 1.234 +X-X
 143.0 6.083 X +3.937-2.721
 \END;
 /*===================================================================*/