Published online by Cambridge University Press: 24 October 2008
The object of this paper is to make certain calculations which will be required in the estimation of the quantum defect. Hartree has defined certain solutions Gi(σ, ζ), Hi(σ, ζ) of the wave equation for an electron in a Coulomb field, viz.
* Proc. Camb. Phil. Soc. xxiv, 426 (1928).Google Scholar
* See e.g Whittaker, and Watson, , Modern Analysis, pp. 354–357.Google Scholar
† See § 2 of the Precceding Paper by Dr D. R. Hartree
* Whittaker, and Watson, , he. cit., p. 376.Google Scholar
† See the appendix.
* Neumann, , Theorie der Besiel' schen Functionen (Leipzig, 1867), p. 52.Google Scholar The expansion and proof are given by Watson (Bessel Functions, 1922, p. 71). (There is a misprint in the latter; the second Jn in the expression for Y(n) should read Jm.)
* Loc. cit. p. 276.