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| /*===================================================================*/
/* NRDF D1923 Data No.4 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,4;
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,4;
/* 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(12C,X)X;
THK-TGT=55.60MG/CM**2;
INC-ENGY-LAB=400MEV/A;
BEAM-INTNSTY=1.77e+9PPS;
ANL=MONTE-MTHD'12';
/* '12' Transport model PHITS */
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,4;
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)
11.0 22 X 82053.5184 +-0.107 3
11.0 24 X 2234.4 +-0.545 4
12.0 27 X 82053.5184 +-0.121 5
12.0 28 X 4604256 +-0.054 6
13.0 29 X 567.48 +-0.237 7
17.0 34 1 +-0.069 8
17.0 38 X 82053.5184 +-0.221 9
17.0 39 X +-0.087 10
18.0 41 X 4604256 +-0.109 11
19.0 43 X 1224 +-0.080 13
21.0 43 X 53852.4 +-0.160 14
24.0 48 X +-0.020 20
24.0 49 X 53852.4 +-0.479 21
24.0 51 X 128160 +-1.061 22
25.0 56 X 75276 +-0.232 24
26.0 59 X 82053.5184 +-0.174 26
27.0 55 X 1224 +-0.078 27
27.0 56 X 3336 +-0.359 28
27.0 57 X +-5.189 29
27.0 61 X 80280 +-1.333 32
28.0 57 X 4604256 +-0.062 34
28.0 65 X 1224 +-0.095 35
29.0 60 X 567.48 +-0.247 36
29.0 61 X 2308.2 +-1.180 37
30.0 62 X 4604256 +-0.059 39
30.0 63 X 567.48 +-0.491 40
30.0 65 X 82053.5184 +-0.121 41
\END;
/*===================================================================*/
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