The Optical Transmission Characteristic of Hollow Carbon-Coated <named-content content-type="math" xlink:type="simple"> <inline-formula> <tex-math notation="LaTeX">$\hbox{Fe}_{3}\hbox{O}_{4}$</tex-math></inline-formula></named-content> Colloidal Photonic Crystal

The optical transmission characteristics for the hollow carbon-coated Fe<sub>3</sub>O<sub>4</sub> colloidal photonic crystal have been calculated with the finite-difference time-domain (FDTD) method. We analyze the influence of the factors on the photonic band gap (PBG) that...

Full description

Bibliographic Details
Main Authors: Yan Huang, Gongying Liang, Xuegang Lu, Xuejiao Bie, Wenyu Li
Format: Article
Language:English
Published: IEEE 2015-01-01
Series:IEEE Photonics Journal
Subjects:
PBG
Online Access:https://ieeexplore.ieee.org/document/7000990/
id doaj-d39fa9060aea4a748deb6ec629a44d63
record_format Article
spelling doaj-d39fa9060aea4a748deb6ec629a44d632021-03-29T17:21:16ZengIEEEIEEE Photonics Journal1943-06552015-01-017111210.1109/JPHOT.2014.23872587000990The Optical Transmission Characteristic of Hollow Carbon-Coated <named-content content-type="math" xlink:type="simple"> <inline-formula> <tex-math notation="LaTeX">$\hbox{Fe}_{3}\hbox{O}_{4}$</tex-math></inline-formula></named-content> Colloidal Photonic CrystalYan Huang0Gongying Liang1Xuegang Lu2Xuejiao Bie3Wenyu Li4Key Lab. of Shaanxi for Adv. Mater. &amp; Mesoscopic Phys., Xi'an Jiaotong Univ., Xi'an, ChinaKey Lab. of Shaanxi for Adv. Mater. &amp; Mesoscopic Phys., Xi'an Jiaotong Univ., Xi'an, ChinaKey Lab. of Shaanxi for Adv. Mater. &amp; Mesoscopic Phys., Xi'an Jiaotong Univ., Xi'an, ChinaKey Lab. of Shaanxi for Adv. Mater. &amp; Mesoscopic Phys., Xi'an Jiaotong Univ., Xi'an, ChinaKey Lab. of Shaanxi for Adv. Mater. &amp; Mesoscopic Phys., Xi'an Jiaotong Univ., Xi'an, ChinaThe optical transmission characteristics for the hollow carbon-coated Fe<sub>3</sub>O<sub>4</sub> colloidal photonic crystal have been calculated with the finite-difference time-domain (FDTD) method. We analyze the influence of the factors on the photonic band gap (PBG) that include lattice constant a, the number of the particles in propagating direction N<sub>y</sub>, the thickness of carbon layer H<sub>c</sub> and Fe<sub>3</sub>O<sub>4</sub> cluster layer H<sub>f</sub>, and the thickness ratio of the two layers. The results show that the PBGs red shift and the bandwidth first increases and then decreases with the increasing a. In the situation of increasing N<sub>y</sub>, the PBG changes from irregular to uniform, followed by the oscillations on both sides of the PBG growing in number and the deepened PBG in the low-frequency region. The PBGs move toward the low frequency direction with the increase of H<sub>c</sub>, and the optimal value of H<sub>c</sub> for the uniform color response is 10 nm ~25 nm. The PBGs red shift with the increasing H<sub>f</sub>, and the first bandwidth increases while the second decreases. The optimal H<sub>f</sub> for the ideal PBG is 35 nm ~55 nm. The stop bands move to the high-frequency direction with the increasing thickness ratio (H<sub>c</sub> : H<sub>f</sub>), and the best ratio is 10 nm : 55 nm for the complete PBG and wider bandwidth.https://ieeexplore.ieee.org/document/7000990/photonic crystaltransmission characteristicPBGFDTDcarbon-coated Fe3O4hollow structure
collection DOAJ
language English
format Article
sources DOAJ
author Yan Huang
Gongying Liang
Xuegang Lu
Xuejiao Bie
Wenyu Li
spellingShingle Yan Huang
Gongying Liang
Xuegang Lu
Xuejiao Bie
Wenyu Li
The Optical Transmission Characteristic of Hollow Carbon-Coated <named-content content-type="math" xlink:type="simple"> <inline-formula> <tex-math notation="LaTeX">$\hbox{Fe}_{3}\hbox{O}_{4}$</tex-math></inline-formula></named-content> Colloidal Photonic Crystal
IEEE Photonics Journal
photonic crystal
transmission characteristic
PBG
FDTD
carbon-coated Fe3O4
hollow structure
author_facet Yan Huang
Gongying Liang
Xuegang Lu
Xuejiao Bie
Wenyu Li
author_sort Yan Huang
title The Optical Transmission Characteristic of Hollow Carbon-Coated <named-content content-type="math" xlink:type="simple"> <inline-formula> <tex-math notation="LaTeX">$\hbox{Fe}_{3}\hbox{O}_{4}$</tex-math></inline-formula></named-content> Colloidal Photonic Crystal
title_short The Optical Transmission Characteristic of Hollow Carbon-Coated <named-content content-type="math" xlink:type="simple"> <inline-formula> <tex-math notation="LaTeX">$\hbox{Fe}_{3}\hbox{O}_{4}$</tex-math></inline-formula></named-content> Colloidal Photonic Crystal
title_full The Optical Transmission Characteristic of Hollow Carbon-Coated <named-content content-type="math" xlink:type="simple"> <inline-formula> <tex-math notation="LaTeX">$\hbox{Fe}_{3}\hbox{O}_{4}$</tex-math></inline-formula></named-content> Colloidal Photonic Crystal
title_fullStr The Optical Transmission Characteristic of Hollow Carbon-Coated <named-content content-type="math" xlink:type="simple"> <inline-formula> <tex-math notation="LaTeX">$\hbox{Fe}_{3}\hbox{O}_{4}$</tex-math></inline-formula></named-content> Colloidal Photonic Crystal
title_full_unstemmed The Optical Transmission Characteristic of Hollow Carbon-Coated <named-content content-type="math" xlink:type="simple"> <inline-formula> <tex-math notation="LaTeX">$\hbox{Fe}_{3}\hbox{O}_{4}$</tex-math></inline-formula></named-content> Colloidal Photonic Crystal
title_sort optical transmission characteristic of hollow carbon-coated <named-content content-type="math" xlink:type="simple"> <inline-formula> <tex-math notation="latex">$\hbox{fe}_{3}\hbox{o}_{4}$</tex-math></inline-formula></named-content> colloidal photonic crystal
publisher IEEE
series IEEE Photonics Journal
issn 1943-0655
publishDate 2015-01-01
description The optical transmission characteristics for the hollow carbon-coated Fe<sub>3</sub>O<sub>4</sub> colloidal photonic crystal have been calculated with the finite-difference time-domain (FDTD) method. We analyze the influence of the factors on the photonic band gap (PBG) that include lattice constant a, the number of the particles in propagating direction N<sub>y</sub>, the thickness of carbon layer H<sub>c</sub> and Fe<sub>3</sub>O<sub>4</sub> cluster layer H<sub>f</sub>, and the thickness ratio of the two layers. The results show that the PBGs red shift and the bandwidth first increases and then decreases with the increasing a. In the situation of increasing N<sub>y</sub>, the PBG changes from irregular to uniform, followed by the oscillations on both sides of the PBG growing in number and the deepened PBG in the low-frequency region. The PBGs move toward the low frequency direction with the increase of H<sub>c</sub>, and the optimal value of H<sub>c</sub> for the uniform color response is 10 nm ~25 nm. The PBGs red shift with the increasing H<sub>f</sub>, and the first bandwidth increases while the second decreases. The optimal H<sub>f</sub> for the ideal PBG is 35 nm ~55 nm. The stop bands move to the high-frequency direction with the increasing thickness ratio (H<sub>c</sub> : H<sub>f</sub>), and the best ratio is 10 nm : 55 nm for the complete PBG and wider bandwidth.
topic photonic crystal
transmission characteristic
PBG
FDTD
carbon-coated Fe3O4
hollow structure
url https://ieeexplore.ieee.org/document/7000990/
work_keys_str_mv AT yanhuang theopticaltransmissioncharacteristicofhollowcarboncoatednamedcontentcontenttypemathxlinktypesimpleinlineformulatexmathnotationlatexhboxfe3hboxo4texmathinlineformulanamedcontentcolloidalphotoniccrystal
AT gongyingliang theopticaltransmissioncharacteristicofhollowcarboncoatednamedcontentcontenttypemathxlinktypesimpleinlineformulatexmathnotationlatexhboxfe3hboxo4texmathinlineformulanamedcontentcolloidalphotoniccrystal
AT xueganglu theopticaltransmissioncharacteristicofhollowcarboncoatednamedcontentcontenttypemathxlinktypesimpleinlineformulatexmathnotationlatexhboxfe3hboxo4texmathinlineformulanamedcontentcolloidalphotoniccrystal
AT xuejiaobie theopticaltransmissioncharacteristicofhollowcarboncoatednamedcontentcontenttypemathxlinktypesimpleinlineformulatexmathnotationlatexhboxfe3hboxo4texmathinlineformulanamedcontentcolloidalphotoniccrystal
AT wenyuli theopticaltransmissioncharacteristicofhollowcarboncoatednamedcontentcontenttypemathxlinktypesimpleinlineformulatexmathnotationlatexhboxfe3hboxo4texmathinlineformulanamedcontentcolloidalphotoniccrystal
AT yanhuang opticaltransmissioncharacteristicofhollowcarboncoatednamedcontentcontenttypemathxlinktypesimpleinlineformulatexmathnotationlatexhboxfe3hboxo4texmathinlineformulanamedcontentcolloidalphotoniccrystal
AT gongyingliang opticaltransmissioncharacteristicofhollowcarboncoatednamedcontentcontenttypemathxlinktypesimpleinlineformulatexmathnotationlatexhboxfe3hboxo4texmathinlineformulanamedcontentcolloidalphotoniccrystal
AT xueganglu opticaltransmissioncharacteristicofhollowcarboncoatednamedcontentcontenttypemathxlinktypesimpleinlineformulatexmathnotationlatexhboxfe3hboxo4texmathinlineformulanamedcontentcolloidalphotoniccrystal
AT xuejiaobie opticaltransmissioncharacteristicofhollowcarboncoatednamedcontentcontenttypemathxlinktypesimpleinlineformulatexmathnotationlatexhboxfe3hboxo4texmathinlineformulanamedcontentcolloidalphotoniccrystal
AT wenyuli opticaltransmissioncharacteristicofhollowcarboncoatednamedcontentcontenttypemathxlinktypesimpleinlineformulatexmathnotationlatexhboxfe3hboxo4texmathinlineformulanamedcontentcolloidalphotoniccrystal
_version_ 1724198007730077696