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The ordinary negative changing refractive index for estimation of optical confinement factor Cover

The ordinary negative changing refractive index for estimation of optical confinement factor

Open Access
|Jun 2022

Figures & Tables

Figure 1

Applied electric field along z-direction changes the refractive index of crystal.
Applied electric field along z-direction changes the refractive index of crystal.

Figure 2

(a) A Mach–Zehnder interferometer modulator MZIM. (b) The cross-sectional diagram of the MZIM and the channel of the waveguides.
(a) A Mach–Zehnder interferometer modulator MZIM. (b) The cross-sectional diagram of the MZIM and the channel of the waveguides.

Figure 3

Integrated LN Mach-Zehnder modulator MZM: (a) top view and (b) cross-section area.
Integrated LN Mach-Zehnder modulator MZM: (a) top view and (b) cross-section area.

Figure 4

MZI electro-optic modulator based on LiNbO3.
MZI electro-optic modulator based on LiNbO3.

Figure 5

The ordinary negative changing of refractive index by applying electric field versus different lengths of arms.
The ordinary negative changing of refractive index by applying electric field versus different lengths of arms.

Figure 6

The ordinary negative changing of refractive index as a function of the confinement factor under different intensity of the applied electrical field.
The ordinary negative changing of refractive index as a function of the confinement factor under different intensity of the applied electrical field.

Figure 7

The ordinary negative changing of refractive index as a function of refractive index versus different lengths of arms for LiTaO3.
The ordinary negative changing of refractive index as a function of refractive index versus different lengths of arms for LiTaO3.

Figure 8

The ordinary negative changing of refractive index as a function of electro-optic coefficient versus different lengths of arms for LiTaO3.
The ordinary negative changing of refractive index as a function of electro-optic coefficient versus different lengths of arms for LiTaO3.

Figure 9

The ordinary negative changing of refractive index with wavelength under different applied electric fields for LiTaO3.
The ordinary negative changing of refractive index with wavelength under different applied electric fields for LiTaO3.

Electro-optic coefficients (r33), refractive index (no) and wavelengths (λ), for LN_4_

r33 (pm/V)Wavelength (nm)noReference
316332.2864(Casson et al., 2004)
2515602.2108(Casson et al., 2004)

The comparison between the reference paper (Chang et al_, 2017; Qi and Li, 2020) and this work_

ReferenceΔnLdΔØEΓModulator type
(Qi and Li, 2020) and (He et al., 2019)LargeLarge In mmSmallπ/2E = V/dLargeTransvers
This workLargeSmall In μmπE = V/LLargeLongitudinal
Language: English
Submitted on: Dec 23, 2021
Published on: Jun 29, 2022
Published by: Professor Subhas Chandra Mukhopadhyay
In partnership with: Paradigm Publishing Services
Publication frequency: 1 issue per year

© 2022 Ahmad S. Abdullah, Sadeq Adnan Hbeeb, published by Professor Subhas Chandra Mukhopadhyay
This work is licensed under the Creative Commons Attribution-NonCommercial-NoDerivatives 4.0 License.