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Resonant, non-resonant, and anomalous states of Dirac electrons in a parabolic well in the presence of magnetic fields

机译:Dirac电子的共振,非共振和异常状态   在存在磁场的情况下抛物线良好

摘要

We report on several new basic properties of a parabolic dot in the presenceof a magnetic field. The ratio between the potential strength and the Landaulevel (LL) energy spacing serves as the coupling constant of this problem. Inthe weak coupling limit the energy spectrum in each Hilbert subspace of anangular momentum consists of discrete LLs of graphene. In the intermediatecoupling regime non-resonant states form a closely spaced energy spectrum. Wefind, counter-intuitively, that resonant quasi-boundstates of both positive andnegative energies exist in the spectrum. The presence of resonantquasi-boundstates of negative energies are a unique property of massless Diracfermions. As the strong coupling limit is approached resonant and non-resonantstates transform into anomalous states, whose probability densities develop anarrow peak inside the well and another broad peak under the potential barrier.These properties may investigated experimentally by measuring opticaltransition energies that can be described by a scaling function of the couplingconstant.
机译:我们报道了在磁场存在下抛物线点的几个新的基本性质。势能与Landaulevel(LL)能量间距之间的比率用作此问题的耦合常数。在弱耦合极限中,角动量的每个希尔伯特子空间中的能谱由石墨烯的离散LL组成。在中间耦合状态下,非共振态形成了紧密间隔的能谱。反直觉地,我们发现,在光谱中同时存在正能量和负能量的共振准结合态。负能量的共振准束缚态的存在是无质量Diracfermion的独特属性。随着接近强耦合极限,共振态和非共振态转变为异常态,其概率密度在井内形成一个尖峰,并在势垒下形成另一个宽峰,这些性质可以通过测量光学跃迁能来实验研究,可以用耦合常数的缩放函数。

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