Related Experiment Video
Updated: May 25, 2026

05:57
Characterization of SiN Integrated Optical Phased Arrays on a Wafer-Scale Test Station
Published on: April 1, 2020
Zero-bias 40Gbit/s germanium waveguide photodetector on silicon
Laurent Vivien1, Andreas Polzer, Delphine Marris-Morini
1Institut d’Electronique Fondamentale (IEF), Université Paris-Sud, CNRS, Orsay France. laurent.vivien@u-psud.fr
Optics Express
|January 26, 2012
Summary
We developed novel germanium photodetectors on silicon waveguides, achieving 120GHz bandwidth and 0.8 A/W responsivity. These devices demonstrate open eye diagrams at 40Gb/s, enabling high-speed optical communication.
Area of Science:
- Optoelectronics
- Materials Science
- Nanotechnology
Background:
- Silicon photonics is a key technology for high-speed optical communication.
- Germanium photodetectors are crucial for detecting optical signals in silicon photonic integrated circuits.
- Integrating high-performance photodetectors onto silicon platforms remains a challenge.
Purpose of the Study:
- To report on the development and characterization of lateral pin germanium photodetectors.
- To demonstrate the high-speed performance of these germanium photodetectors integrated with silicon waveguides.
- To assess their suitability for next-generation optical communication systems.
Main Methods:
- Selective growth of lateral pin germanium photodetectors at the end of silicon waveguides.
- Characterization of optical bandwidth using three experimental setups.
- Measurement of responsivity at 1550 nm.
- Demonstration of open eye diagrams at 40Gb/s under zero-bias conditions.
Main Results:
- A very high optical bandwidth, estimated up to 120 GHz, was achieved for 10 µm long germanium photodetectors.
- A responsivity of 0.8 A/W at 1550 nm was measured.
- Open eye diagrams at 40 Gb/s were demonstrated under zero-bias operation at 1.55 µm wavelength.
Conclusions:
- Lateral pin germanium photodetectors can be successfully integrated with silicon waveguides.
- These photodetectors exhibit excellent high-speed performance, suitable for 40Gb/s and beyond optical communications.
- The demonstrated performance highlights the potential of these devices for advanced photonic integrated circuits.
More Related Videos
Related Concept Videos
Biasing of Metal-Semiconductor Junctions
Biasing metal-semiconductor junctions involves applying a voltage across the junction. Specifically, the metal is connected to a voltage source, while the semiconductor is grounded. This technique is essential for controlling the direction and magnitude of current flow in electronic devices, including diodes, transistors, and photovoltaic cells.
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
Diode: Forward bias
In semiconductor devices, diodes play a crucial role in directing current flow, and its operation is primarily categorized into forward bias and reverse bias. A diode is said to be forward-biased when its p-type region is connected to the positive terminal of a battery and its n-type region is linked to the negative terminal. This configuration reduces the potential barrier within the diode, allowing current to flow easily from the p to the n-type region.
The behavior of a diode in forward bias...
The behavior of a diode in forward bias...
Diode: Reverse bias
A diode is reverse-biased when the positive terminal of an external voltage source is connected to the n-type material and the negative terminal to the p-type material. This configuration opposes the natural direction of current flow through the diode, effectively increasing the width of the depletion region and the barrier potential. The reverse bias condition produces a minimal leakage current, primarily due to minority charge carriers. This leakage becomes significant when the reverse...
Biasing of P-N Junction
The operation of a p-n junction diode involves various biasing conditions, including forward bias, reverse bias, and equilibrium.
In equilibrium, no external voltage is applied across the p-n junction. The depletion region is formed at the junction interface due to the diffusion of carriers, which leaves behind charged dopants, acceptors on the p-side, and donors on the n-side. These immobile charges create an electric field that prevents further diffusion of carriers. The related energy band...
In equilibrium, no external voltage is applied across the p-n junction. The depletion region is formed at the junction interface due to the diffusion of carriers, which leaves behind charged dopants, acceptors on the p-side, and donors on the n-side. These immobile charges create an electric field that prevents further diffusion of carriers. The related energy band...
Schottky Barrier Diode
Schottky barrier diodes are specialized semiconductor devices characterized by their unique construction. This construction involves combining a metal layer with a moderately doped n-type semiconductor material. This combination leads to the formation of a Schottky barrier, a pivotal element that defines the diode's operational characteristics. The core functionality of Schottky barrier diodes is their capacity to allow current to flow in only one direction due to their distinctive...
Semiconductors
There is variation in the electrical conductivity of materials - metals, semiconductors, and insulators that are showcased with the help of the energy band diagrams.
Metals such as copper (Cu), zinc (Zn), or lead (Pb) have low resistivity and feature conduction bands that are either not fully occupied or overlap with the valence band, making a bandgap non-existent. This allows electrons in the highest energy levels of the valence band to easily transition to the conduction band upon gaining...
Metals such as copper (Cu), zinc (Zn), or lead (Pb) have low resistivity and feature conduction bands that are either not fully occupied or overlap with the valence band, making a bandgap non-existent. This allows electrons in the highest energy levels of the valence band to easily transition to the conduction band upon gaining...

