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arXiv 0810.4897math-phmath.MP
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经典磁场中非对算符的本征函数

On the eigenfunctions of no-pair operators in classical magnetic fields

Oliver Matte, Edgardo Stockmeyer

摘要:

本文考虑了类氢原子在经典外磁场中的相对论非对模型。首先,我们证明了对于所有小于或等于Brown-Ravenhall模型已知的临界耦合常数的耦合常数,相应的哈密顿量是下半有界的,即,用于消除磁场。给出了保证其本质谱等于[1,\infty)且存在无穷多个小于1的特征值的条件. (The在我们的单位中,电子的静止能量是1。)假设磁矢势是光滑的,并且它的所有偏导数都是次指数增长的,我们最后证明了对应于本征值λ<1的本征函数在远离核的地方是光滑的,并且它的任何阶的偏导数都以任何速率a<(1-λ^2)^{1/2}逐点指数衰减,对于λ \in [0,1),和a<1,对于λ<0。

英文摘要:

We consider a relativistic no-pair model of a hydrogenic atom in a classical, exterior magnetic field. First, we prove that the corresponding Hamiltonian is semi-bounded below, for all coupling constants less than or equal to the critical one known for the Brown-Ravenhall model, i.e., for vanishing magnetic fields. We give conditions ensuring that its essential spectrum equals [1,\infty) and that there exist infinitely many eigenvalues below 1. (The rest energy of the electron is 1 in our units.) Assuming that the magnetic vector potential is smooth and that all its partial derivatives increase subexponentially, we finally show that an eigenfunction corresponding to an eigenvalue λ<1 is smooth away from the nucleus and that its partial derivatives of any order decay pointwise exponentially with any rate a<(1-λ^2)^{1/2}, for λ\in[0,1), and a<1, for λ<0.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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