Monolithic On-chip Magneto-optical Isolator with 3 dB Insertion Loss and 40 dB Isolation Ratio

ACS Photonics ◽  
2018 ◽  
Vol 5 (12) ◽  
pp. 5010-5016 ◽  
Author(s):  
Qingyang Du ◽  
Chuangtang Wang ◽  
Yifei Zhang ◽  
Yan Zhang ◽  
Takian Fakhrul ◽  
...  
2021 ◽  
Author(s):  
Hao Tian ◽  
Junqiu Liu ◽  
Anat Siddharth ◽  
Rui Ning Wang ◽  
Terence Blesin ◽  
...  
Keyword(s):  

Electronics ◽  
2018 ◽  
Vol 7 (10) ◽  
pp. 236 ◽  
Author(s):  
Wonseok Choe ◽  
Jinho Jeong

A waveguide-to-microstrip transition is an essential component for packaging integrated circuits (ICs) in rectangular waveguides, especially at millimeter-wave and terahertz (THz) frequencies. At THz frequencies, the on-chip transitions, which are monolithically integrated in ICs are preferred to off-chip transitions, as the former can eliminate the wire-bonding process, which can cause severe impedance mismatch and additional insertion loss of the transitions. Therefore, on-chip transitions can allow the production of low cost and repeatable THz modules. However, on-chip transitions show limited performance in insertion loss and bandwidth, more seriously, this is an in-band resonance issue. These problems are mainly caused by the substrate used in the THz ICs, such as an indium phosphide (InP), which exhibits a high dielectric constant, high dielectric loss, and high thickness, compared with the size of THz waveguides. In this work, we propose a broadband THz on-chip transition using a dipole antenna with an integrated balun in the InP substrate. The transition is designed using three-dimensional electromagnetic (EM) simulations based on the equivalent circuit model. We show that in-band resonances can be induced within the InP substrate and also prove that backside vias can effectively eliminate these resonances. Measurement of the fabricated on-chip transition in 250 nm InP heterojunction bipolar transistor (HBT) technology, shows wideband impedance match and low insertion loss at H-band frequencies (220–320 GHz), without in-band resonances, due to the properly placed backside vias.


2018 ◽  
Vol 32 (22) ◽  
pp. 1850258 ◽  
Author(s):  
Wenlong Liu ◽  
Xuebin Liu ◽  
Qiangqiang Yan ◽  
Simiao Qiang ◽  
Haifeng Pi ◽  
...  

Breaking Lorentz reciprocity is one necessary condition of optical isolator design. Unidirectional wavelength-mode conversion will be realized in a time-dependent system through a short operating range. Based on plasma dispersion effect, generate space-asymmetric periodical time-space modulation on silicon waveguide, and non-reciprocal propagation is realized in the waveguide. The designed unidirectional wavelength-mode conversion waveguide demonstrated that in the forward direction, input 1.55 [Formula: see text]m fundamental mode light signal and then output 1.5492 [Formula: see text]m is of 1st-order mode, while in the backward direction, input 1.5492 [Formula: see text]m is of 1st-order mode light signal and then output 1.5484 [Formula: see text]m is of fundamental mode. Based on this non-reciprocal structure, mode conversion waveguide and two-ring resonance filters were designed then, to accomplish on-chip optical isolation. The scale of the designed isolator is 160 [Formula: see text]m × 60 [Formula: see text]m, and the isolation is 21 dB, revealing perfect application potential.


2018 ◽  
Vol 6 (5) ◽  
pp. 380 ◽  
Author(s):  
Zepeng Pan ◽  
Songnian Fu ◽  
Luluzi Lu ◽  
Dongyu Li ◽  
Weijie Chang ◽  
...  

2014 ◽  
Vol 6 (10) ◽  
pp. 879 ◽  
Author(s):  
Lei Zhang ◽  
Yunjia Man ◽  
Xianfang Tan ◽  
Mei Yang ◽  
Ting Hu ◽  
...  

2021 ◽  
Vol 16 (1) ◽  
Author(s):  
Hao Hu ◽  
Jiwei Qi ◽  
Qiang Wu ◽  
Xianhui Fu ◽  
Hongjin Wu ◽  
...  

AbstractWe designed a simple on-chip integrated optical isolator made up of a metal–insulator–metal waveguide and a disc cavity filled with magneto-optical material to enhance the transverse magneto-optical effect through the coin paradox spin–orbit interaction (SOI). The simulation results of the non-reciprocal transmission properties of this optical structure show that a high-performance on-chip integrated optical isolator is obtained. The maximum isolation ratio is greater than 60 dB with a corresponding insertion loss of about 2 dB. The great performance of the optical isolator is attributed to the strong transverse magneto-optical effect, which is enhanced by the coin paradox SOI. Moreover, the enhancement of the transverse magneto-optical effect through the coin paradox SOI is more substantial for smaller azimuthal mode number n. Benefiting from this, the transverse magneto-optical effect remains strong in a wide wavelength range. Additionally, a smaller cavity has a stronger transverse magneto-optical effect in the same wavelength range. Our research provides a new perspective for creating highly integrated magneto-optical devices.


2021 ◽  
Vol 8 ◽  
Author(s):  
Jia-Jian Chen ◽  
Zi-Hao Wang ◽  
Wen-Qi Wei ◽  
Ting Wang ◽  
Jian-Jun Zhang

A feedback insensitive laser is a prerequisite for a desirable laser source for silicon photonic integration, as it is not possible to include an on-chip optical isolator. This work investigates the feedback insensitivity of an InAs/GaAs quantum dot laser epitaxially grown on an Si (001) substrate by operating in a sole excited state. The experimental results show that the sole excited-state lasing InAs quantum dot lasers on Si are less sensitive to external optical feedback than both Fabry-Perot and distributed-feedback quantum-well lasers. By comparing the laser behavior under different feedback levels, sole excited-state InAs quantum dot lasers on Si exhibit at least a 28 dB stronger feedback tolerance than quantum-well lasers. This result proposes a possible route for a high feedback insensitive laser as an on-chip light source towards Si waveguide integration with the absence of an optical isolator.


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