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De Broglie waves meet Schrodinger's equation

机译:德布罗意波符合薛定inger方程

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For a quantum-mechanical free particle, de Broglie's hypothesis relates group velocity v_g to phase velocity v_p via v_gv_p = c~2. However, the relation has not yet been grounded in the usual definition v_g = dω)/dk. This article provides the missing dispersion relation to evaluate dω/dk. Direct solution of Schrodinger's equation in one dimension yields the dispersion relation co = (h/ 2 m)k~2, from which follows the relation vg = 2v_p Further implications of the dispersion relation are explored. Because the free-particle Schrodinger equation is a heat equation with an imaginary heat constant, its Green's function is a linear chirp that fills all space starting the instant after a deltafunction initial condition. Particle localization is possible only when the Green's function is spatially convolved (at a time t) with a substantially band-limited initial wavefunction. The faster expansion of a wavefunction when it is initially narrow could be a realization of the uncertainty principle. All of this Schrodinger-equation analysis, however, makes a disconcerting break with relativistic quantum mechanics. Free-particle solution of the Klein-Gordon equation vindicates V_gV_p = c~2. The nonrelativistic noncorrespondence of Schrodinger and Klein-Gordon, or more simply of v_g = 2v_p with v_gv_p = c~2, leads us to ask which can be trusted in the nonrelativistic velocity limit.
机译:对于量子力学自由粒子,德布罗意的假设通过v_gv_p = c〜2使群速度v_g与相速度v_p相关。但是,该关系尚未基于通常的定义v_g =dω)/ dk。本文提供了缺失的色散关系来评估dω/ dk。一维Schrodinger方程的直接解产生色散关系co =(h / 2 m)k〜2,从中得出关系vg = 2v_p进一步探讨了色散关系的含义。因为自由粒子的薛定inger方程是一个具有虚热常数的热方程,所以它的格林函数是线性rp,它会在出现增量函数初始条件后立即填充所有空间。仅当格林函数(在时间t处)在空间上卷积具有基本带宽受限的初始波函数时,才可能进行粒子定位。当波函数最初很窄时,它的快速扩展可能是不确定性原理的一种实现。然而,所有这些薛定inger方程分析都与相对论量子力学产生了令人不安的突破。 Klein-Gordon方程的自由粒子解证明了V_gV_p = c〜2。 Schrodinger和Klein-Gordon的非相对论性不对应,或更简单地说v_g = 2v_p且v_gv_p = c〜2,使我们想起在非相对论性速度极限中哪个值得信赖。

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