dc.creator | Sánchez Cano, Robert | |
dc.creator | Porras Montenegro, Nelson | |
dc.date.accessioned | 2020-03-18T23:04:14Z | |
dc.date.accessioned | 2022-09-22T18:52:21Z | |
dc.date.available | 2020-03-18T23:04:14Z | |
dc.date.available | 2022-09-22T18:52:21Z | |
dc.date.created | 2020-03-18T23:04:14Z | |
dc.date.issued | 2012-12 | |
dc.identifier | Sánchez Cano, Robert; Porras Montenegro, Nelson. Ga1- xInxAsySb1- y/GaSb spherical quantum dot in a magnetic field. En: Revista Mexicana de Física. Volumen 58, número 2, (diciembre 2012); páginas 147-150 | |
dc.identifier | http://red.uao.edu.co//handle/10614/12133 | |
dc.identifier.uri | http://repositorioslatinoamericanos.uchile.cl/handle/2250/3460058 | |
dc.description.abstract | Quaternary semiconductor alloys type-I are appropriated materials for heterostructure devices because they provide a natural form to tune the magnitude of the band gap so that it can operate in the mid-infrared (mid-IR) wavelength range. However electron spin degree of freedom and the electron spin splitting g-factor provide a new pathway to the development of a practical quantum communication systems, because the effective g-factor for electrons in III-V semiconductors vary as a function of the chemical concentration. We investigated theoretically electron g-factor in bulk Ga(1-x)In(x)As(y)Sb(1-y) matched to GaSb and the Zeeman effect as well as the Landau levels in GaSb/Ga(1-x)In(x)As(y)Sb(1-y)/GaSb spherical quantum dot heterostructure under the framework of Kane eight-band effective-mass model, in which the mixing of the states in the lower conduction band and the highest valence bands is taken into account. Our calculations show that bulk electron g-factor values are in the range between the electron g-factor measured in bulk GaSb when x -- 0 (g =-9.25) and that measured in InAs when x --1 (g =-18.08), but there is a notable minimum in the g-factor value (g -- -23.14) at x -- 0 . 67. In GaSb/Ga(1-x)In(x)As(y)Sb(1-y)/GaSb spherical quantum dot our calculations show that the electron g-factor decreases as the radius increases reaching the value for the quaternary in bulk for a given In concentration, x, and increases when the radius decreases, approaching to the value in the barrier material, when R -- 0. Also for higher values of concentration of In, the g-factor as a function of R moves to the g-factor bulk limit | |
dc.language | eng | |
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dc.relation | Revista Mexicana de Física. Volumen 58, número 2, (diciembre 2012); páginas 147-150 | |
dc.rights | https://creativecommons.org/licenses/by-nc-nd/4.0/ | |
dc.rights | info:eu-repo/semantics/openAccess | |
dc.rights | Atribución-NoComercial-SinDerivadas 4.0 Internacional (CC BY-NC-ND 4.0) | |
dc.rights | Derechos Reservados - Universidad Autónoma de Occidente | |
dc.title | Ga1- xInxAsySb1- y/GaSb spherical quantum dot in a magnetic field | |
dc.type | Artículo de revista | |