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 /* NRDF D1868 Data No.2                                              */
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 /* Bibliography                                                      */
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 \\BIB,2;
 D#=D1868;
 TITLE=/ Production of pure 123I by the 127I(p,5n)123Xe -> 123I
         reaction /;
 PURPOSE=/ To study incident proton energy region to obtain pure 123I
           effectively /;
 ATH=(K.SUZUKI'1');
 INST-ATH=(2JPNIRS'1');
      /* '1' Section of Cyclotron */
 REF=RI;
 VLP=35(1986)235;
 /* '2' Written in Japanese */
 RCTS=(127I(P,)123XE, 127I(P,)125XE, 127I(P,)127XE);
 PHQS=XSECTN;
 /*===================================================================*/
 /* Experimental Conditions                                           */
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 \\EXP,2;
 /* 2004-02-18 : Compiled+Checked */
 /* 2023-04-06 : Altered, MA. REACTION in 002-004 were modified. */
 PHQ=XSECTN;
 CHM=X'3';
 /* '3' Sodium iodide */
 PHYS-FORM=SLD'4';
 /* '4' Disk (12 mm diameter) */
 THK-TGT=100[150MG/CM**2;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=CYC;
 INST-ACC=2JPNIRS;
 BEAM-INTNSTY=0.1[0.2UA;
 POL-PRJ=0%;
 DET-PARTCL=GAMMA'5';
 /* '5' . No description for decay data measured */
 COINC=NO;
 ANT-COINC=NO;
 /* Experimental Method:
    - Activation
    - Stacked target irradiation (Stack of sodium iodide disks and
      copper foils. Energy loss in each disk is calculated using table
      of range / stopping power [K.Hata et al., JAERI-M-5558(1974)].)
 /* 2023-04-06 : Altered, MA. SF3: X -> 3N */
 /* Related references 
    - A.M.J.Paans et al., ARI, 27(1976)465.
    Reference with which data agree. See also EXFOR A0161.003.
    - S.R.Wilkins et al., ARI, 26(1975)279.
    Reference with which data disagree. See also EXFOR A0265.003.
    - D.B.Syme et al., ARI, 29(1978)29.
    Reference with which data disagree. See also EXFOR B0148.003.
 RCT=127I(P,)125XE;
 DET-SYS=(GE(LI),SI(LI));
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 /* Descriptive Parameters                                            */
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 \\DATA,2;
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 /* Data Table                                                        */
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 \DATA;
 INC-ENGY-LAB XSECTN
 (MEV) (MB)
 20 10
 22 140
 24 450
 26 750
 28 920
 30 890
 32 800
 34 660
 36 510
 38 390
 40 290
 42 230
 44 180
 46 150
 48 130
 50 120
 52 105
 54 95
 56 90
 58 88
 \END;
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