coulomb excitation data analysis codes; gosia 2007 - Physics and ...

11,012,014,016,00,0END,OP,YIELN1=18 internal conversion coefficients (ICCs) are entered for N2=10multipolarity to cover the full range of transition energies.18,10.056,0.068,0.082,0.1,0.12,0.15,0.18,0.22,0.26,0.32,0.38,0.46,0.56,0.68,0.82,1.0,1.2,1.52I 1 =2 indicates that E2 ICCs will follow.41.7,17.6,7.97,3.58,1.78,0.785,0.415,0.212,0.124,0.0660,0.0403,0.0241,0.0148,0.00939,0.00623,0.00413,0.00288,0.001881,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,1,11459014590145901459014590145901459014590145901459014590145This blank line required.IFLAG = 0. “1” selects correction to the gamma-ray yield distribution forthe distance traveled by the decaying nucleus.Experiment 1 has NANG(1)=1 gamma-ray detector.Similar entries are made for the NANG(2)...NANG(27).Note that a negative sign would indicate an identicalgamma-ray detector to the previous experiment.Experiment #1 has one Ge detector of type “1” (IP=1)as defined in file 9, “det.gdt.”, (See OP,FILE above.)The detector is positioned at θ 1 =45° polar angle withrespect to the beam and φ 1 =90° azimuthal angle.Similar records are entered for each experiment that hasa positive value of NANG (above).OP,YIEL defines the gamma-ray detector geometriesand types, internal normalizations and user-provideddata for the investigated nucleus (section 5.30).Energy meshpointsE 1 , E 2 ... [MeV] forICC’s.E2 internal conversioncoefficients CC(I 1 ,1),CC(I 1 ,2)... for theenergy meshpointsabove.172