Related Experiment Video
Updated: Jan 4, 2026

09:59
Fabrication of Flexible Image Sensor Based on Lateral NIPIN Phototransistors
Published on: June 23, 2018
8.1K
Alignment tolerant, low voltage, 0.23 V.cm, push-pull silicon photonic switches based on a vertical pn junction
Optics Express
|November 6, 2019
Summary
This study introduces a highly efficient silicon-photonic switch using a vertical pn junction. The device achieves fast switching times and is compatible with commercial complementary-metal-oxide semiconductor (CMOS) foundries.
Area of Science:
- Photonics
- Semiconductor Devices
- Integrated Optics
Background:
- Silicon photonics offers a promising platform for optical communication and computation.
- Carrier depletion switches are crucial components for optical signal processing.
- Existing designs often face challenges in efficiency and fabrication compatibility.
Purpose of the Study:
- To design, fabricate, and characterize a novel carrier depletion silicon-photonic switch.
- To achieve high modulation efficiency and fast switching speeds.
- To ensure compatibility with standard complementary-metal-oxide semiconductor (CMOS) fabrication processes.
Main Methods:
- Utilized a highly doped vertical pn junction design.
- Employed a lumped configuration for fast switching.
- Characterized device performance including modulation efficiency and switching time.
- Assessed fabrication tolerance for commercial foundry integration.
Main Results:
- Achieved a high modulation efficiency of 0.23 V·cm.
- Demonstrated fast switching times as low as 60 ps.
- Fabrication process showed high tolerance to deviations.
- Seamless transfer to a 350 nm CMOS process node is feasible.
Conclusions:
- Successfully demonstrated a highly efficient carrier depletion silicon-photonic switch.
- The vertical pn junction design is key to achieving superior performance.
- The developed technology is suitable for mass production in commercial CMOS foundries.
- Medium resolution lithography is sufficient for fabricating these advanced devices.
Related Concept Videos
Biasing of P-N Junction
1.7K
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...
1.7K
Semiconductors
1.3K
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...
1.3K
Biasing of Metal-Semiconductor Junctions
506
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...
506
P-N junction
1.1K
A p-n junction is formed when p-type and n-type semiconductor materials are joined together. At the interface of the p-n junction, holes from the p-side and electrons from the n-side begin to diffuse into the opposite sides due to the concentration gradient. This diffusion of carriers leads to a region around the junction where there are no free charge carriers, known as the depletion region. The charge density within the depletion region for the n-side and p-side can be described by the...
1.1K
MOSFET: Enhancement Mode
727
Enhancement-mode MOSFETs are pivotal components in electronics, distinguished by their capacity to act as highly efficient switches. They are part of the larger family of metal-oxide Semiconductor Field-Effect Transistors (MOSFETs). They are available in two types: p-channel and n-channel, each tailored to specific polarity operations.
In their basic form, enhancement-mode MOSFETs are typically non-conductive when the gate-source voltage (Vgs) is zero. This default 'off' state means no...
In their basic form, enhancement-mode MOSFETs are typically non-conductive when the gate-source voltage (Vgs) is zero. This default 'off' state means no...
727
Metal-Semiconductor Junctions
850
The contact of metal and semiconductor can lead to the formation of a junction with either Schottky or Ohmic behavior.
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The...
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The...
850

