By L. R. B. Elton (auth.), H. Schopper (eds.)
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S. 63 fm, was discovered to describe adequately the charge distribution. , with slightly different parameters for the Fermi 2 parameter model for the charge distribution resulting, as shown in the Table. , . , observed that the group of elements (,zHf, ,3Ta, ,4W, aoTh, and &J) did not exhibit pronounced diffraction structure in the manner of the other nuclei which they investigated. Contributions to the cross section arising from the non-spherical character of those nuclei were assumed to be filling in the diffraction dip areas and yielding relatively smooth overall cross section behavior.
Ru (3. g. (3, 4. 5) Alle KemgrijBen in der Tabclle schlietlen den EinfluL3 der endlichen Ausdehnung des Protons ein, z. B. a2 (Tabelle) = = a2 (Korpcr) + a2 (Proton). uB (Table) = = u2 (Body) + u2 (Proton). The skin thickness, 1, equals the distance in which the charge density falls from 90% to 10% of its central value. (6) I Die Hautdicke t entspricht der OberflGzhendicke, innerhalb der die Ladungsdichte von 90% auf loo/, des Wertes am Kemmittel1 pm&t abfsllt. s. 03 rD? 22 1) See note 1 added in proof p.
14 fm. See Discussion 16 for explanations of the “Gaussian-uniform” and “uniform-uniform” models. 59 fm. s. 12 fm. , is a phase-shift calculation. , . Instead of analyzing the elastic electron scattering from the nucleus by means of a phcnomenological charge distribution of simple functional form, they have generated charge distributions with the help of singleparticle proton wave functions in a central potential of the Saxon-Woods form, which includes a spinorbit term. namclv, with where R = vo(A - l)ln .
Nuclear Radii by L. R. B. Elton (auth.), H. Schopper (eds.)