Temperature dependence of band gap ratio and Q-factor defect mode in a semiconductor quaternary alloy hexagonal photonic-crystal hole slab
We present numerical predictions for the photonic TE-like band gap ratio and the quality factors of symmetric localized defect as a function of the thickness slab and temperature by the use of plane wave expansion and the finite-difference time-domain methods. The photonic-crystal hole slab is compo...
- Autores:
-
Sánchez Cano, Robert
Porras Montenegro, Nelson
- Tipo de recurso:
- Article of journal
- Fecha de publicación:
- 2016
- Institución:
- Universidad Autónoma de Occidente
- Repositorio:
- RED: Repositorio Educativo Digital UAO
- Idioma:
- eng
- OAI Identifier:
- oai:red.uao.edu.co:10614/11077
- Acceso en línea:
- http://hdl.handle.net/10614/11077
https://link.springer.com/article/10.1007/s00339-016-9906-0
https://link.springer.com/content/pdf/10.1007%2Fs00339-016-9906-0.pdf
- Palabra clave:
- Campos electromagnéticos
Electromagnetic fields
Electromagnetismo
Optoelectrónica
Aleaciones magnéticas
Optoelectronics
Electromagnetism
Magnetic alloys
- Rights
- openAccess
- License
- Derechos Reservados - Springer-Verlag Berlin Heidelberg 2016
Summary: | We present numerical predictions for the photonic TE-like band gap ratio and the quality factors of symmetric localized defect as a function of the thickness slab and temperature by the use of plane wave expansion and the finite-difference time-domain methods. The photonic-crystal hole slab is composed of a 2D hexagonal array with identical air holes and a circular cross section, embedded in a non-dispersive III–V semiconductor quaternary alloy slab, which has a high value of dielectric function in the near-infrared region, and the symmetric defect is formed by increasing the radius of a single hole in the 2D hexagonal lattice. We show that the band gap ratio depends linearly on the temperature in the range 150–400 K. Our results show a strong temperature dependence of the quality factor Q, the maximum ( Q=7000 ) is reached at T=350K, but if the temperature continues to increase, the efficiency drops sharply. Furthermore, we present numerical predictions for the electromagnetic field distribution at T=350K |
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