2016
DOI: 10.1016/j.spmi.2016.04.044
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Coherent electron transparent tunneling through a single barrier within a Fabry-Perot cavity

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Cited by 7 publications
(5 citation statements)
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“…where p = 2m(E − h F P ) for a rectangular barrier of height h F P , m is the effective mass of the tunnel barrier, h is the Planck's constant, E is the electron energy and λ is the reference wavelength (here, the wavelength of the well region on both sides of the tunnel barrier). The refractive index n is thus given by [36,37]…”
Section: Cavity Physics and Transmission Functionmentioning
confidence: 99%
“…where p = 2m(E − h F P ) for a rectangular barrier of height h F P , m is the effective mass of the tunnel barrier, h is the Planck's constant, E is the electron energy and λ is the reference wavelength (here, the wavelength of the well region on both sides of the tunnel barrier). The refractive index n is thus given by [36,37]…”
Section: Cavity Physics and Transmission Functionmentioning
confidence: 99%
“…An optical analogy 11 of Schrodinger waves propagating in one dimension from a region of fixed potential energy V 0 (the incident medium) into a region of varying potential energy V can be set up. The region with potential energy V has an equivalent refractive index (complex) given by: where m is the effective mass of the electron inside the region of potential energy V , and m 0 is the mass of the electron in the incident medium.…”
Section: The Analogy Between Schrodinger Wave Mechanics and Electromamentioning
confidence: 99%
“…The coating of an optical element with layers of selected refractive index and thickness can be used to suppress reflections, to induce transmission and to create band pass filters. The design of structures that show enhanced transmission for matter waves is also possible and the fabrication of resonant structures with the properties of a Fabry-Perot interferometer 10 , 11 consisting of two identical barriers separated by a region of constant potential, has already been implemented in the resonant tunnelling or Esaki diode. The resonant cavity idea is not well suited to antireflection of general barriers, because of its inconvenient reliance on the symmetry of two participating barriers.…”
Section: Introductionmentioning
confidence: 99%
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“…Another approach is the transfer matrix (TM) method. This method is often used in the field of modeling semiconductor materials and optoelectronic devices as a computational method for solving the 1-dimensional Schrödinger equation. Effective mass is also included in the Schrödinger equation describing the motion of the electron. In this method, the original potential is divided into a series of rectangular barriers, and the wavefunctions for each sliced barrier are solved.…”
Section: Introductionmentioning
confidence: 99%