Calculation of the magnetic hyperfine structure of spectral lines with allowance for the finite size of the atomic nucleus and a study of the density of nuclear magnetism /

A formula is derived for the correction of the hyperfine structure constant owing to the fact that nuclear magnetism differs in nature from a point magnetic dipole. A possible form of the angular part of the magnetic density is examined for a specified radial part of the density of nuclear magnetism. These angular parts are phenomenologically defined and are able to make a contribution to the magnetic hyperfine structure constant. This contribution is required to close the gap between theory and experiment for the atoms: He3, Li6, Na22, and Na23.Translation supported by the Air Force Cambridge Research Laboratories, Office of Aerospace Research, United States Air Force (L.G. Hanscom Field, Mass.), and translated by the American Meteorological Society, Boston, Massachusetts.Translated from Vilniaus Valstybinio Univ. Mokslo Darbai, v.25 (Mat. fix. chem. ser, 8): pp. 89-99, 1958.AFCRL Research Library.AD 0680365 (from http://www.dtic.mil)."October 1968."Includes bibliographical references (pages 13-14).A formula is derived for the correction of the hyperfine structure constant owing to the fact that nuclear magnetism differs in nature from a point magnetic dipole. A possible form of the angular part of the magnetic density is examined for a specified radial part of the density of nuclear magnetism. These angular parts are phenomenologically defined and are able to make a contribution to the magnetic hyperfine structure constant. This contribution is required to close the gap between theory and experiment for the atoms: He3, Li6, Na22, and Na23.Mode of access: Internet