翻訳と辞書
Words near each other
・ Lambeth London Borough Council election, 1968
・ Lambeth London Borough Council election, 1971
・ Lambeth London Borough Council election, 1974
・ Lambeth London Borough Council election, 1978
・ Lambeth London Borough Council election, 1982
・ Lambeth London Borough Council election, 1986
・ Lambeth London Borough Council election, 1990
・ Lambeth London Borough Council election, 1994
・ Lambeth London Borough Council election, 1998
・ Lambeth London Borough Council election, 2002
・ Lambeth London Borough Council election, 2006
・ Lambeth London Borough Council election, 2010
・ Lambeth London Borough Council election, 2014
・ Lambeth London Borough Council elections
・ Lambert-Sigisbert Adam
Lambert-W step-potential
・ Lambertella
・ Lambertellinia
・ Lamberti
・ Lambertia
・ Lambertia echinata
・ Lambertia ericifolia
・ Lambertia fairallii
・ Lambertia formosa
・ Lambertia ilicifolia
・ Lambertia inermis
・ Lambertia multiflora
・ Lambertia orbifolia
・ Lambertia rariflora
・ Lambertia uniflora


Dictionary Lists
翻訳と辞書 辞書検索 [ 開発暫定版 ]
スポンサード リンク

Lambert-W step-potential : ウィキペディア英語版
Lambert-W step-potential

The Lambert-W step-potential〔("The Lambert W-barrier - an exactly solvable confluent hypergeometric potential" )〕 affords the fifth – next to those of the harmonic oscillator plus centrifugal, the Coulomb plus inverse square, the Morse, and the inverse square root〔("Exact solution of the Schrödinger equation for the potential V0/√x" )〕 potentials – exact solution to the stationary one-dimensional Schrödinger equation in terms of the confluent hypergeometric functions.〔("Discretization of Natanzon potentials" )〕 The potential is given as
: V(x) = \frac.
where W is the Lambert function also known as the product logarithm. This is an implicitly elementary function that resolves the equation We^W=z.
The Lambert W-potential is an asymmetric step of height V_0 whose steepness and asymmetry are controlled by parameter \sigma. If the space origin and the energy origin are also included, it presents a four-parametric specification of a more general five-parametric potential which is also solvable in terms of the confluent hypergeometric functions. This generalized potential, however, is a conditionally integrable one (that is, it involves a fixed parameter).
==Solution==
The general solution of the one-dimensional Schrödinger equation for a particle of mass m and energy E:
:\frac+\frac(E-V(x))\psi=0,
for the Lambert W-barrier for arbitrary V_0 and \sigma is written as
:\psi(x)=z^e^\left(\frac-i\fracu(z)\right), z=W(e^),
where u(z) is the general solution of the scaled confluent hypergeometric equation
:u''(z)+\left(\frac-is\right)u'(z)+\fracu(z)=0
and the involved parameters are given as
:a=\frac+\frac, \delta=2\sigma\sqrt}, s=2\sigma\sqrt}.
A peculiarity of the solution is that each of the two fundamental solutions composing the general solution involves a combination of two confluent hypergeometric functions.
If the quantum transmission above the Lambert W-potential is discussed, it is convenient to choose the general solution of the scaled confluent hypergeometric equation as
:u=c_1(isz)^_1F_1 and U are the Kummer and Tricomi confluent hypergeometric functions, respectively. The two confluent hypergeometric functions are here chosen such that each of them stands for a separate wave moving in a certain direction. For a wave incident from the left, the reflection coefficient written in terms of the standard notations for the wave numbers
:k_1=\sqrt},k_2=\sqrt}
reads
:R=e^\frac(k_1-k_2)^2\right)}}(k_1+k_2)^2\right)}}

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
ウィキペディアで「Lambert-W step-potential」の詳細全文を読む



スポンサード リンク
翻訳と辞書 : 翻訳のためのインターネットリソース

Copyright(C) kotoba.ne.jp 1997-2016. All Rights Reserved.