Abstract

A three-port optical phase-shifter and Mach-Zehnder modulator (MZM) based on PNP-type bipolar junction transistor (BJT) is demonstrated. Significant plasma (injected carrier) induced changes of the refractive index for the optical waveguide become possible with an extremely small driving-voltage and a compact device size during operation of this BJT between the saturation and forward active modes. Devices with a standard MZM structure and a small foot-print (0.5 mm) exhibit a moderate optical insertion loss (2 dB), extremely small V π (0.18V) and P π (0.21mW), fast rise/fall time (~1ns), and a residue-amplitudemodulation (RAM) as small as 0.18 dB. Furthermore, thanks to the ultra-high modulation efficiency characteristic of our device, a +4.0 dB net RF-linking gain can be obtained under dynamic operation. Compared to 2-port (base-collector) forward bias operation, under three-port operation, the extra bias current from the base-emitter junction provides a lower V π (0.18 vs. 0.22 V), a smaller RAM (0.18 vs. 0.6 dB), and a larger RF-linking gain (+4 vs. -3.2 dB). The superior performances of the three-port to two-port operations can be attributed to the additional forward bias B-E junction being able to provide more injected carriers to induce stronger plasma effects for optical phase-shifting.

Highlights

  • Silicon photonics (SiPs) play a leading role in the development of technology ranging from radio frequency (RF) microwave photonics to sensing systems

  • We demonstrate three-port (PNP)-type bipolar junction transistor (BJT) based phase-shifters and Mach-Zehnder modulator (MZM) fabricated on a standard commercial Si-photonic foundry platform

  • During dynamic and static operation, our device operates in the saturation regions, which indicates that both the VEB and VCB junctions are under forward bias

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Summary

Introduction

Silicon photonics (SiPs) play a leading role in the development of technology ranging from radio frequency (RF) microwave photonics to sensing systems. With a short device length (0.5 mm) and an acceptable insertion loss (2 dB), our device exhibits excellent performance in terms of fast rise time (tR ≈ 1ns), small driving-voltage and small power consumption for π phase-shift (Pπ : 0.21 mW; Vπ : 0.18 V), extremely small RAM (0.18 dB) [14], and a +4.0 dB net RF linking gain at an operating frequency of 100 MHz. Compared with our previous work [15], the doping profile is further optimized by greatly reducing the doping level in the p-type collector layer (from 3 × 1019 to 5 × 1017 cm−3).

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