Related Experiment Video
Updated: May 5, 2026

11:26
Integrating a Triplet-triplet Annihilation Up-conversion System to Enhance Dye-sensitized Solar Cell Response to Sub-bandgap Light
Published on: September 12, 2014
12.1K
Reduction in Dark Current in Photodiodes: A Review
Alper Ülkü1, Ralph Potztal1, Tobias Blaettler1
1ESPROS Photonics AG, 7320 Sargans, Switzerland.
Micromachines
|May 4, 2026
Summary
Dark current limits photodiode performance. This review details dark current generation mechanisms and explores reduction techniques like surface passivation and guard rings to improve low-light detection.
Area of Science:
- Optoelectronics and Semiconductor Device Physics
- Materials Science for Photodetection
Background:
- Dark current is a primary noise source in photodiodes, limiting sensitivity in low-light conditions.
- Understanding dark current mechanisms is crucial for advancing photodetector technology.
Purpose of the Study:
- To comprehensively review the physical mechanisms of dark current generation in photodiodes.
- To survey and categorize diverse techniques for mitigating dark current.
- To provide a structured overview of literature relevant to various photodiode applications.
Main Methods:
- Literature review of publications on dark current mechanisms and reduction strategies.
- Categorization of dark current mechanisms: diffusion, SRH, tunneling, and surface leakage.
- Classification of reduction techniques: thermal management, passivation (e.g., ALD Al2O3), guard rings, gettering, doping optimization, and advanced architectures (e.g., pinned photodiodes, black silicon).
Main Results:
- Detailed examination of the physical origins and signatures of different dark current components.
- Systematic organization of reduction strategies applicable across various material systems (Si, Ge, III-V).
- Identification of key findings and material relevance for near-infrared, CMOS imaging, SPADs, and ToF applications.
Conclusions:
- Effective dark current reduction is essential for high-performance photodiodes.
- A variety of physical mechanisms and engineering solutions exist, tailored to specific materials and applications.
- This review consolidates knowledge to guide future photodiode research and development.
Related Concept Videos
Diode: Reverse bias
2.7K
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...
2.7K
P-N junction
1.7K
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...
1.7K
Photoreceptors and Visual Pathways
8.5K
At the molecular level, visual signals trigger transformations in photopigment molecules, resulting in changes in the photoreceptor cell's membrane potential. The photon's energy level is denoted by its wavelength, with each specific wavelength of visible light associated with a distinct color. The spectral range of visible light, classified as electromagnetic radiation, spans from 380 to 720 nm. Electromagnetic radiation wavelengths exceeding 720 nm fall under the infrared category,...
8.5K
Biasing of P-N Junction
2.7K
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...
2.7K
Small-signal Diode Model
1.9K
In analyzing the behavior of diodes in circuits, the relationship between the current through a diode and the voltage across it is of particular interest, especially when considering the effect of a direct current (DC) bias voltage. When applied, this DC bias influences the diode's operating point, known as the Q point, around which the current-voltage (I-V) characteristic of the diode exhibits exponential behavior. Introducing a small, time-varying signal on top of this bias aids in examining...
1.9K
Diode: Forward bias
2.6K
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...
2.6K

