Abstract:Cross sections for the elastic scattering of 88.03-keV For gold, 7.3 keV above its threshold, the experiment agrees with the S-matrix prediction. However, for lead some 25 eV above threshold, the experimental value is about 40% larger than predicted, while for bismuth (2.5 keV below threshold), experiment lies 70% above theory. The measured K-shell photoeff'ect cross section of lead is within 10%%uo of the prediction based on the independent-particle approximation.
“…The experimental total incoherent scattering di †erential cross-sections per atom is calculated by using the following equation [2] given by Standing et al [19], Basavaraju et al [20] and Kane et al [8,11,12]. This method is explained by Standing et al [19] and Basavaraju et al [20].…”
With the help of a Ge(Li) detector, the incoherent scattering
differential cross-sections were determined for 59.5keV gamma rays
scattered by Fe, Zn and Nb through angles from 55–105°. The
background correction and detection efficiency are also included in
the study. The experimental results are given and compared with some
available theoretical data obtained with some approximation
methods.
“…The experimental total incoherent scattering di †erential cross-sections per atom is calculated by using the following equation [2] given by Standing et al [19], Basavaraju et al [20] and Kane et al [8,11,12]. This method is explained by Standing et al [19] and Basavaraju et al [20].…”
With the help of a Ge(Li) detector, the incoherent scattering
differential cross-sections were determined for 59.5keV gamma rays
scattered by Fe, Zn and Nb through angles from 55–105°. The
background correction and detection efficiency are also included in
the study. The experimental results are given and compared with some
available theoretical data obtained with some approximation
methods.
“…As described previously [1], the error in the measured elastic-scattering cross section der, &ld0 is reduced if the elastic-scattering counts due to a target under study are compared with the Compton scattering counts %co p due to an aluminum target. With such a procedure, the source strength and the detector solid angle do not need to be determined, and only ratios of quantities such as detection ef5ciencies and target transmissions for similar energies are needed.…”
A high-purity germanium detector was used to determine differential cross sections for the elastic scattering of 81-keV y rays by aluminum, nickel, tantalum, gold, and lead through angles of 60', 90', 120', and
Summary. --Total atomic incoherent-scattering differential cross-sections were determined experimentally for 59.5 keV gamma-rays in Ti, Ni, Zn, Se, Mo, Ru, Cd, Sn, Te, Yt, W and Pb at 120 ~ scattering angle using Ge(Li) detector. The background correction and detection efficiency are also included in the study. The experimental values have been compared with those estimated on the basis of the non-relativistic Hartree-Fock wave functions. Good agreement is observed between theory and experiment.
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