Lamas-Martínez K J, Briones-Torres J A, Molina-Valdovinos S, Rodríguez-Vargas I
Unidad Académica de Ciencia y Tecnología de la Luz y la Materia, Universidad Autónoma de Zacatecas, Circuito Marie Curie S/N, Parque de Ciencia y Tecnología QUANTUM Ciudad del Conocimiento, 98160 Zacatecas, Zacatecas, Mexico.
Ingeniería en Nanotecnología, Universidad de La Ciénega del Estado de Michoacán de Ocampo, Avenida Universidad 3000, Col. Lomas de la Universidad, Sahuayo, Michoacán 59103, Mexico.
J Phys Condens Matter. 2024 Oct 18;37(2). doi: 10.1088/1361-648X/ad8618.
Fano resonances appear in plenty of physical phenomena due to the interference phenomena of a continuum spectrum and discrete states. In gated bilayer graphene junctions, the chiral matching at oblique incidence between the spectrum of electron states outside the electrostatic barrier and hole bound states inside it gives rise to an asymmetric line shape in the transmission as a function of the energy or Fano resonance. Here, we show that Fano resonances are also possible in gated phosphorene junctions along the zigzag direction. The special pseudospin texture of the charge carriers in the zigzag direction allows at oblique incidence the interference phenomena of the spectrum of electron states outside the electrostatic barrier with hole bound states inside it, giving rise to an asymmetric Fano line shape in the transmission. Due to the energy scale of the electrostatic barriers in phosphorene ultra thin barriers are required to observe the Fano resonance phenomenon. The preservation of the pseudospin texture with the closing of the phosphorene band gap opens the possibility to observe Fano resonances in smaller and wider electrostatic barriers. The asymmetric Fano line shape is susceptible to the transverse wave vector, the strength and width of the electrostatic barrier. Additionally, the conductance shows a characteristic mark in the position where the Fano resonances take place. The similarities and differences with respect to Fano resonances in bilayer graphene are also addressed.
由于连续谱与离散态的干涉现象,法诺共振出现在众多物理现象中。在门控双层石墨烯结中,静电势垒外电子态谱与势垒内空穴束缚态在斜入射时的手性匹配,导致透射率随能量变化呈现不对称线形,即法诺共振。在此,我们表明沿锯齿方向的门控磷烯结中也可能出现法诺共振。锯齿方向上电荷载流子特殊的赝自旋结构使得在斜入射时,静电势垒外电子态谱与势垒内空穴束缚态发生干涉现象,从而导致透射率出现不对称的法诺线形。由于磷烯中静电势垒的能量尺度,需要超薄势垒才能观测到法诺共振现象。随着磷烯带隙关闭,赝自旋结构得以保留,这为在更小和更宽的静电势垒中观测法诺共振开辟了可能性。不对称的法诺线形对横向波矢、静电势垒的强度和宽度敏感。此外,电导在法诺共振发生的位置呈现出特征标记。我们还讨论了与双层石墨烯中法诺共振的异同。