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/* NRDF D1923 Data No.5 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,5;
D#=D1923;
TITLE=/ Cross sections for the production of residual nuclides by
high-energy heavy ions /;
ATH=(H.YASHIMA'1', Y.UWAMINO'2', H.IWASE'1', H.SUGITA'1',
T.NAKAMURA'1', S.ITO'2', A.FUKUMURA'3');
INST-ATH=(2JPNTOH'1', 2JPNIPC'2', 2JPNIRS'3');
/* '1' Cyclotron and Radioisotope Center */
REF=NIM/B;
VLP=226(2004)243;
RCTS=(CU(20NE,X)X, CU(12C,X)X, CU(40AR,X)X, CU(28SI,X)X,
12C(20NE,X)X, 12C(12C,X)X, 12C(40AR,X)X, 12C(28SI,X)X,
27AL(20NE,X)X, 27AL(12C,X)X, 27AL(40AR,X)X, 27AL(28SI,X)X,
CR(20NE,X)X, CR(12C,X)X, CR(ALPHA,X)X, CR(P,X)X, CR(40AR,X)X,
CR(28SI,X)X, FE(20NE,X)X, FE(12C,X)X, FE(ALPHA,X)X, FE(P,X)X,
FE(40AR,X)X, FE(28SI,X)X, NI(20NE,X)X, NI(12C,X)X, NI(ALPHA,X)X,
NI(P,X)X, NI(40AR,X)X, NI(28SI,X)X, PB(20NE,X)X, PB(12C,X)X,
PB(ALPHA,X)X, PB(P,X)X, PB(40AR,X)X, PB(28SI,X)X);
PHQS=XSECTN;
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,5;
/* 2004-11-28 : Recieved, On. Data received by e-mail from
H.Yashima */
/* 2005-04-17 : Compiled, Am + On. */
/* Related references
- R.B.Firestone et al., FIRESTONE, (1996).
Reference from which data were used (Properties of product nuclei
given)
- H.Iwase et al., NST, 39(2002)1142.
Reference used in the evaluation (Description of PHITS code)
PHQ=XSECTN;
/* Additional results shown but not compiled
- Mass distribution (Isobaric yield)
- Charge distribution (Fractional yield)
CHM=ELM;
PHYS-FORM=SLD;
POL-TGT=0%;
ALGN-TGT=0%;
ACC=SYN;
INST-ACC=2JPNIRS'4';
/* '4' HIMAC facility */
POL-PRJ=0%;
COINC=NO;
ANT-COINC=NO;
DET-SYS=HPGE'5';
/* '5' To measure gamma spectra */
/* Experimental Method:
- Activation (See Table 1 for irradiation time)
- Stacked target irradiation (Samples are inserted into composite
Cu target)
/* Analysis:
- Decay curve analysis (Half-lives are identified by 4 HPGe
detectors.)
RCT=CU(40AR,X)X;
THK-TGT=24.08MG/CM**2;
INC-ENGY-LAB=400MEV/A;
BEAM-INTNSTY=2.37e+8PPS;
ANL=MONTE-MTHD'13';
/* '13' Transport model PHITS */
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,5;
TOT-ERR=2[40%;
SYS-ERR=(0.5[7.2%'6',1[6%'7');
/* '6' Error of peak efficiency */
/* '7' Error of beam intensity */
STATIST-ERR=1[40%'8';
/* '8' Error of total counts of gamma-ray peak area */
INC-ENGY-LAB=400MEV/A;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
Z A ISOMER HALF-LIFE
(NODIM) (NODIM) (NODIM) (MB) (MB) (SEC)
4.0 7 X +-2.478 1
19.0 42 X 2234.4 +-0.610 12
21.0 44 0 6560.4 +-0.400 15
21.0 44 1 80280 +-0.384 16
21.0 46 0 44496 +-0.423 17
21.0 47 X 75276 +-0.164 18
21.0 48 X 4604256 +-0.128 19
25.0 54 X 539395.2 +-1.538 23
26.0 52 0 +-0.018 25
27.0 58 0 +-2.300 30
27.0 60 0 21104064 +-1.268 31
27.0 62 1 1224 +-0.215 33
29.0 64 X +-9.584 38
\END;
/*===================================================================*/
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