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Inverse square root potential
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Inverse square root potential : ウィキペディア英語版
Inverse square root potential

The inverse square root potential is a three-parametric quantum-mechanical potential for which the one-dimensional Schrödinger equation is exactly solvable in terms of the confluent hypergeometric functions.〔("Exact solution of the Schrödinger equation for the potential V0/√x" )〕〔("Discretization of Natanzon potentials" )〕
The potential is defined as:
:V(x) = V_c+\frac{\sqrt{x-x_0}}.
==Comments==
Omitting the non-essential constants V_c , x_0 the general solution of the Schrödinger equation
:\frac+\frac(E-V(x))\psi=0
for the potential V(x) = V_0/ for arbitrary V_0 is written as
:\psi(x)= e^\frac,
where
:u=e^\left(c_1 \cdot H_a(y)+c_2 \cdot ;\frac;y^2)\right).
Here c_ are arbitrary constants, H_a is the Hermite function (for a non-negative integer a it becomes the Hermite polynomial; however, in general a is arbitrary). ,
and the involved parameters \delta and a are given as
: \delta=\sqrt,
: a=\frac{\hbar (-2 m E)^{3/2}} .

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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