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The Energy Level Shifts, Wave Functions and the Probability Current Distributions for the Bound Scalar and Spinor Particles Moving in a Uniform Magnetic Field

机译:能级偏移,波函数和概率电流   均匀运动的束缚标量和旋转粒子的分布   磁场

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摘要

We discuss the equations for the bound one-active electron states based onthe analytic solutions of the Schrodinger and Pauli equations for a uniformmagnetic field and a single attractive $\delta({\bf r})$-potential. It is varyimportant that ground electron states in the magnetic field differ essentiallyfrom the analogous state of spin-0 particles, whose binding energy wasintensively studied more than forty years ago. We show that binding energyequations for spin-1/2 particles can be obtained without using the language ofboundary conditions in the $\delta$-potential model developed in pioneeringworks. We use the obtained equations to calculate the energy leveldisplacements analytically and demonstrate nonlinear dependencies on fieldintensity. We show that the magnetic field indeed plays a stabilizing role inconsidered systems in a case of the weak intensity, but the opposite occurs inthe case of strong intensity. These properties may be important for realquantum mechanical fermionic systems in two and three dimensions. We alsoanalyze the exact solution of the Pauli equation for an electron moving in thepotential field determined by the three-dimensional $\delta$-well in thepresence of a strong magnetic field. We obtain asymptotic expressions for thissolution for different values of the problem parameters. In addition, weconsider electron probability currents and their dependence on the magneticfield. We show that including the spin in the framework of the nonrelativisticapproach allows correctly taking the effect of the magnetic field on theelectric current into account. The obtained dependencies of the currentdistribution, which is an experimentally observable quantity, can be manifesteddirectly in scattering processes, for example.
机译:我们基于均匀磁场和单个有吸引力的$ \ delta({\ bf r})$势的Schrodinger和Pauli方程的解析解,讨论束缚的一活电子态的方程。重要的是,磁场中的基态电子与自旋-0粒子的相似状态本质上不同,自旋-0粒子的结合能在四十多年前得到了深入研究。我们表明,在pioneeringworks开发的$ \ delta-势能模型中,无需使用边界条件的语言即可获得自旋1/2粒子的结合能方程。我们使用获得的方程来分析计算能级位移,并证明了场强的非线性依赖性。我们表明,在强度较弱的情况下,磁场确实在所考虑的系统中起稳定作用,而在强度较强的情况下则相反。这些性质对于二维和三维的实量子机械费米子系统可能很重要。我们还分析了在强磁场存在下,电子在三维三维δ阱中确定的势场中移动的电子的保利方程的精确解。我们针对问题参数的不同值为此解决方案获得渐近表达式。另外,我们考虑电子概率电流及其对磁场的依赖性。我们表明,在非相对论方法的框架中包括自旋,可以正确考虑磁场对电流的影响。所获得的电流分布的依存关系是实验上可观察到的量,例如可以直接在散射过程中表现出来。

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