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Andreev levels in a graphene-superconductor surface

机译:石墨烯超导体表面的安德列夫能级

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摘要

In order to consider the Dirac-like spectrum of graphene we employ the Bogoliubov de Gennes-Dirac formalism to determine the quasiparticle Andreev levels in an NS surface (normal-superconductor). The normal region is characterized by a width L while the superconducting region is semi-infinite and both regions are made of doped graphene. The quasiparticle energy spectrum is originated by the Andreev reflections that occur in the NS interface. It is shown that this spectrum depends on the width of the normal region and the Fermi energy in each region. When the Fermi energy in the normal metal is lower than the gap of the superconductor region, the spectrum is affected by specular Andreev reflections. The equation that is obtained to find the spectrum is very general and we solve it for some particular cases. We find that the energy spectrum oscillates when the Fermi energy in graphene is changed. Finally we obtain under some approximations an equation for the energy spectrum which is similar in structure as those obtained for an INS conventional junction.
机译:为了考虑类石墨的狄拉克光谱,我们采用Bogoliubov de Gennes-Dirac形式主义来确定NS表面(正超导体)中的准粒子安德列夫水平。正常区域的特征是宽度L,而超导区域是半无限大,并且两个区域都由掺杂的石墨烯制成。准粒子能谱是由NS界面中发生的Andreev反射引起的。结果表明,该光谱取决于正常区域的宽度和每个区域的费米能量。当普通金属中的费米能小于超导体区的能隙时,光谱受到镜面安德列夫反射的影响。找到光谱的方程非常笼统,我们针对某些特殊情况进行求解。我们发现,当石墨烯中的费米能发生变化时,能谱振荡。最终,我们获得了近似的能谱方程,其结构与INS常规结所获得的方程相似。

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