Related Experiment Video
Updated: Apr 4, 2026

10:42
Infrared Degenerate Four-wave Mixing with Upconversion Detection for Quantitative Gas Sensing
Published on: March 22, 2019
6.7K
InAs Nanocrystal-Based Infrared Imager Operating beyond Telecom Wavelengths
Youngsang Park1, Hyeonjun Jeong1, Adrien Khalili2
1Department of Energy Science (DOES), Sungkyunkwan University (SKKU), Suwon 16419, Republic of Korea.
Nano Letters
|April 2, 2026
Summary
This study presents a new short-wave infrared (SWIR) imager using indium arsenide (InAs) nanocrystals. This cost-effective technology enables real-time, room-temperature infrared imaging at telecom wavelengths.
Area of Science:
- Materials Science
- Nanotechnology
- Optoelectronics
Background:
- Silicon-based photodetectors are limited by their band gap, hindering infrared imaging beyond specific wavelengths.
- Colloidal III-V nanocrystals offer a path to overcome silicon's limitations for cost-effective and CMOS-compatible infrared imaging.
Purpose of the Study:
- To demonstrate a short-wave infrared (SWIR) imager operating at telecom wavelengths.
- To utilize indium arsenide (InAs) nanocrystals for infrared-sensitive photoconductors.
- To develop a scalable and cost-effective infrared imaging technology.
Main Methods:
- Synthesis of InAs nanocrystals with spectral cutoff up to 1600 nm.
- Ligand exchange to create an n-type conductive ink from InAs nanocrystals.
- Characterization using photoemission, optical spectroscopy, and transport measurements to determine electronic structure.
- Fabrication of an infrared-sensitized focal plane array via single-step deposition.
Main Results:
- InAs nanocrystals exhibit electronic properties suitable for infrared detection, with limited trap density.
- A focal plane array was successfully fabricated using the synthesized InAs nanocrystal ink.
- The resulting imager achieved room-temperature, real-time video imaging at telecom wavelengths under ambient conditions.
Conclusions:
- III-V nanocrystal films, specifically InAs, are a viable material for scalable infrared imaging.
- The developed imager demonstrates the potential for cost-effective, CMOS-compatible infrared detection beyond the silicon band gap.
- This technology paves the way for advanced infrared imaging applications at telecom wavelengths.
Related Concept Videos
Infrared (IR) Spectroscopy: Overview
7.3K
When electromagnetic radiation passes through a material, atoms or molecules transition from a lower to a higher energy state by absorbing radiation corresponding to the energy difference between the two states. The absorption of infrared (IR) radiation causes transitions between vibrational energy levels in a molecule. Therefore, IR spectroscopy is a useful analytical tool for determining the molecular structure of molecules.
Different compounds display unique properties due to their...
Different compounds display unique properties due to their...
7.3K
IR Spectrometers
3.4K
There are two main infrared (IR) spectrophotometers: dispersive IR spectrometers and Fourier transform infrared (FTIR) spectrometers. In a dispersive IR spectrometer, a beam of infrared radiation produced by a hot wire is divided into two parallel equal-intensity beams using mirrors. One beam passes through the sample, while another is a reference beam. The beams then move through the monochromator, which separates the radiations into a continuous spectrum of different frequencies. The...
3.4K
Total Internal Reflection Fluorescence Microscopy
13.7K
Total internal reflection fluorescence microscopy or TIRF is an advanced microscopic technique used to visualize fluorophores in samples close to a solid surface with a higher refractive index, such as a glass coverslip. TIRF only allows fluorophores in proximity to the solid surface to be excited. When light from a medium with a lower refractive index (such as air) hits the glass coverslip at a critical angle, the light undergoes total internal reflection stead of passing through the glass.
13.7K
IR Frequency Region: Fingerprint Region
2.3K
IR spectra are divided into two main regions: the diagnostic region and the fingerprint region. The diagnostic region of the spectrum lies above 1500 cm−1. The absorptions resulting from single-bond vibrations of the N–H, C–H, and O–H stretch at higher wavenumbers and appear on the left side of the spectrum. The stretching absorptions of the C≡C and C≡N occur between 2100–2300 cm−1. In contrast, those arising from stretching absorptions of the...
2.3K

