/*===================================================================*/ /* NRDF D1923 Data No.6 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,6; 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,6; /* 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'14'; /* '14' Transport model PHITS */ /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,6; 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 53852.4 +-0.285 3 11.0 24 X 80280 +-0.827 4 12.0 27 X 53852.4 +-0.348 5 12.0 28 X 4604256 +-0.171 6 13.0 29 X 393.6 +-0.493 7 17.0 34 1 4604256 +-0.138 8 17.0 38 X 82053.5184 +-0.344 9 17.0 39 X 4604256 +-0.132 10 18.0 41 X 1224 +-0.215 11 19.0 43 X 82053.5184 +-0.137 13 21.0 43 X 75276 +-0.206 14 24.0 48 X +-0.053 20 24.0 49 X 75276 +-0.663 21 24.0 51 X 539395.2 +-1.486 22 25.0 56 X 2234.4 +-0.389 24 26.0 59 X 567.48 +-0.303 26 27.0 55 X 82053.5184 +-0.162 27 27.0 56 X 14137.2 +-0.586 28 27.0 57 X +-7.923 29 27.0 61 X 2538 +-2.164 32 28.0 57 X 1224 +-0.131 34 28.0 65 X 82053.5184 +-0.192 35 29.0 60 X 1920 +-0.536 36 29.0 61 X +-2.030 37 30.0 62 X 82053.5184 +-0.132 39 30.0 63 X 1920 +-0.940 40 30.0 65 X 393.6 +-0.306 41 \END; /*===================================================================*/ |