Using nearly monoenergetic unpolarised Kα x-ray photons coherent (Rayleigh) and incoherent (atomic Compton) scattering cross sections in the atomic region 13 ≤ Z ≤ 82 have been measured at 23.18, 24.14, 25.19, 26.27 and 30.85 keV. Experimental scattering cross sections in the momentum transfer region 1.322 h Å−1 ≤ q ≤ 1.759 h Å−1 [q = sin (θ/2)λ(Å)] were obtained at an angle of 90°. Experimental coherent scattering cross sections are in good agreement with second order S-matrix calculations, compared to theoretical estimates based on form factor approximations. Experimental incoherent scattering cross sections are higher than the theoretical estimates calculated using non-relativistic incoherent scattering functions for low and medium Z elements and lower for heavy elements. The latter is due to the binding effects at low photon energies.
Rayleigh and Compton scattering cross sections for low, medium and high Z elements in the energy region 23.18 ≤ E ≤ 30.85 keV / D. V., Rao; R., Cesareo; Gigante, Giovanni Ettore. - In: PHYSICA SCRIPTA. - ISSN 0031-8949. - STAMPA. - 54:4(1996), pp. 362-364. [10.1088/0031-8949/54/4/011]
Rayleigh and Compton scattering cross sections for low, medium and high Z elements in the energy region 23.18 ≤ E ≤ 30.85 keV
GIGANTE, Giovanni Ettore
1996
Abstract
Using nearly monoenergetic unpolarised Kα x-ray photons coherent (Rayleigh) and incoherent (atomic Compton) scattering cross sections in the atomic region 13 ≤ Z ≤ 82 have been measured at 23.18, 24.14, 25.19, 26.27 and 30.85 keV. Experimental scattering cross sections in the momentum transfer region 1.322 h Å−1 ≤ q ≤ 1.759 h Å−1 [q = sin (θ/2)λ(Å)] were obtained at an angle of 90°. Experimental coherent scattering cross sections are in good agreement with second order S-matrix calculations, compared to theoretical estimates based on form factor approximations. Experimental incoherent scattering cross sections are higher than the theoretical estimates calculated using non-relativistic incoherent scattering functions for low and medium Z elements and lower for heavy elements. The latter is due to the binding effects at low photon energies.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.