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首页> 外文期刊>Journal of Physics. Condensed Matter >Resonant, non-resonant and anomalous states of Dirac electrons in a parabolic well in the presence of magnetic fields
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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:磁场作用下抛物阱中狄拉克电子的共振,非共振和异常状态

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摘要

We report on several new basic properties of a parabolic dot in the presence of a magnetic field. The ratio between the potential strength and the Landau level (LL) energy spacing serves as the coupling constant of this problem. In the weak coupling limit the energy spectrum in each Hilbert subspace of an angular momentum consists of discrete LLs of graphene. In the intermediate coupling regime non-resonant states form a closely spaced energy spectrum. We find, counter-intuitively, that resonant quasi-bound states of both positive and negative energies exist in the spectrum. The presence of resonant quasi-bound states of negative energies is a unique property of massless Dirac fermions. As the strong coupling limit is approached resonant and non-resonant states transform into anomalous states, whose probability densities develop a narrow peak inside the well and another broad peak under the potential barrier. These properties may investigated experimentally by measuring optical transition energies that can be described by a scaling function of the coupling constant.
机译:我们报告了在磁场存在下抛物线点的几个新的基本特性。势能与朗道能级(LL)的能量间距之比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都由离散的石墨烯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。与直觉相反,我们发现频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狄拉克费米子的独特性质。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窄峰,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进行实验研究,所述光学跃迁能可以通过耦合常数的比例函数来描述。

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