/*===================================================================*/ /* NRDF D1923 Data No.3 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,3; 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,3; /* 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'11'; /* '11' Transport model PHITS */ /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,3; 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 11998.8 +-1.254 1 19.0 42 X 75276 +-0.387 12 21.0 44 0 1920 +-0.296 15 21.0 44 1 3336 +-0.278 16 21.0 46 0 2234.4 +-0.304 17 21.0 47 X 567.48 +-0.094 18 21.0 48 X 4604256 +-0.076 19 25.0 54 X 166238.8704 +-1.018 23 26.0 52 0 +-0.007 25 27.0 58 0 +-1.507 30 27.0 60 0 29790 +-0.604 31 27.0 62 1 4604256 +-0.100 33 29.0 64 X +-3.688 38 \END; /*===================================================================*/ |