2014 A generalization of the non-relativistic Fermi-Segrè formula into a formula which is valid also for angular momentum quantum numbers 1 différent from zero, is derived by means of a phase-integral method. The formula thus obtained, which gives an expression for the limit of u(r)/rl+ 1 as r ~ 0, where u(r) is a normalized bound-state radial wavefunction, in terms of the derivative of the energy level En’ with respect to the radial quantum number n’, is an improvement and generalization of a formula which has been obtained by M. A. Bouchiat and C. Bouchiat. It reduces to their formula for a particular class of potentials and highly excited states with not too large values of l, and it reduces to the Fermi-Segrè formula when l = 0. The accuracy of our formula, as well as that of the Bouchiat-Bouchiat formula, is investigated by application to an exactly soluble model. The formula obtained can also be written in another form by replacing dEn’/dn’ by an expression involving a closed-loop integral in the complex r-plane (around the generalized classical turning points), the integrand being a phase-integral quantity expressed in terms of the potential in which the particle moves. It is also shown that the exact value of the limit of u(r)/rl+1 as r ~ 0 can be expressed as an expectation value of a certain function depending on the physical potential V(r) and r as well as on l and En,. Tome 42 N° 11 NOVEMBRE 1981 J. Physique 42 ( 1981 ) 1491-1504 NOVEMBRE 1981, Classification Physics Abstracts 03.65
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