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Langer correction : ウィキペディア英語版
Langer correction

The Langer correction is a correction when WKB approximation method is applied to three-dimensional problems with spherical symmetry.
When applying WKB approximation method to the radial Schrödinger equation
: -\frac \frac + () R(r) = 0
where the effective potential is given by
:V_\textrm(r)=V(r)-\frac
the eigenenergies and the wave function behaviour obtained are different from real solution.
In 1937, Rudolph E. Langer suggested a correction
:\ell(\ell+1) \rightarrow \left(\ell+\frac\right)^2
which is known as Langer correction. This is equivalent to inserting a 1/4 constant factor whenever ℓ(ℓ + 1) appears. Heuristically, it is said that this factor arises because the range of the radial Schrödinger equation is restricted from 0 to infinity, as opposed to the entire real line.
By such a changing of constant term in the effective potential, the results obtained by WKB approximation reproduces the exact spectrum for many potentials.
==References==

* (The original publication. )

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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