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In quantum mechanics the delta potential is a potential well mathematically described by the Dirac delta function - a generalized function. Qualitatively, it corresponds to a potential which is zero everywhere, except at a single point, where it takes an infinite value. This can be used to simulate situations where a particle is free to move in two regions of space with a barrier between the two regions. For example, an electron can move almost freely in a conducting material, but if two conducting surfaces are put close together, the interface between them acts as a barrier for the electron that can be approximated by a delta potential. The delta potential well is a limiting case of the finite potential well, which is obtained if one maintains the product of the width of the well and the potential constant while decreasing the well's width and increasing the potential. This article, for simplicity, only considers a one-dimensional potential well, but analysis could be expanded to more dimensions. == Single delta potential == The time-independent Schrödinger equation for the wave function ''ψ''(''x'') of a particle in one dimension in a potential ''V''(''x'') is : where ''ħ'' is the reduced Planck constant and ''E'' is the energy of the particle. The delta potential is the potential : where δ(''x'') is the Dirac delta function. It is called a ''delta potential well'' if ''λ'' is negative and a ''delta potential barrier'' if ''λ'' is positive. The delta has been defined to occur at the origin for simplicity; a shift in the delta function's argument does not change any of the proceeding results. 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「Delta potential」の詳細全文を読む スポンサード リンク
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