Thermal emission of one-dimensional conjugated photonic crystals heterojunction embedded with graphene

2019 ◽  
Vol 92 (3) ◽  
Author(s):  
Yifan He ◽  
Liang Guo ◽  
Jincheng Li ◽  
Yihang Chen ◽  
Chengping Yin
Author(s):  
Azka Umar ◽  
Chun Jiang

This paper focuses on manipulating thermal emission and radiation loss of heat energy in a heat waveguide. A One-Dimensional Photonic Crystal is used as a waveguide clad to prohibit the thermal emission from escaping. The model may reduce the radiation loss of heat energy in the waveguide core, and heat energy can be confined to propagate along the waveguide’s longitude axis. The waveguide clad comprises alternative layers of high and low refractive index materials containing sufficient electromagnetic stop bands to trap the thermal emission from escaping out of the waveguide. The numerical simulation of the model shows that the forbidden bandgap of photonic crystal structures with alternative layers of silica and silicon has width enough to make heat energy be confined within the waveguide core so that efficient heat energy transmission can be achieved along the longitude axis of the waveguide.


2005 ◽  
Vol 87 (7) ◽  
pp. 071904 ◽  
Author(s):  
B. J. Lee ◽  
C. J. Fu ◽  
Z. M. Zhang

2021 ◽  
Vol 68 (3) ◽  
pp. 125-133
Author(s):  
Hassan S. Ashour ◽  
Mazen M. Abadla ◽  
Khedr M. Abohassan

2021 ◽  
Vol 22 ◽  
pp. 103882
Author(s):  
Khedr M. Abohassan ◽  
Hassan S. Ashour ◽  
Mazen M. Abadla

2012 ◽  
Vol 614-615 ◽  
pp. 1629-1632
Author(s):  
Gang Xu ◽  
Yun Sun

Applying transfer matrix method, we get reflection and transmission coefficient of finite one dimensional photonic crystals. At the same time, we consider the position influence of single defect. We find the frequency of defect mode is same, but the height of transmission peak is not same when single defect is in different position of crystal. The transmission peak is maximum when the defect is in center of finite one dimensional photonic crystals.


2016 ◽  
Vol 94 (12) ◽  
Author(s):  
E. S. Sedov ◽  
E. D. Cherotchenko ◽  
S. M. Arakelian ◽  
A. V. Kavokin

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