{"id":4749,"date":"2023-10-13T12:08:10","date_gmt":"2023-10-13T10:08:10","guid":{"rendered":"https:\/\/www.institut-foton.eu\/?p=4749"},"modified":"2025-07-17T11:06:36","modified_gmt":"2025-07-17T09:06:36","slug":"imagerie-lidar","status":"publish","type":"post","link":"https:\/\/www.institut-foton.eu\/en\/imagerie-lidar\/","title":{"rendered":"Lidar imaging"},"content":{"rendered":"\n\n\n\n

Presentation<\/h2>\n\n\n
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Lidar (Light Detection and Ranging), is an increasingly widespread imaging technique, especially in the context of the development of autonomous systems (unmanned vehicles, drones) in different fields of application (meteorology, navigation assistance, monitoring, detection, threat detection, etc.) In the DOP team, we are looking to improve existing Lidar techniques by offering new features for increased performance.<\/p>\n\n\n\n

Lidar-radar<\/h3>\n\n\n\n

Compared to conventional lidar techniques, where the distance to the target is deduced from the measurement of the time-of-flight of the light pulse, the lidar-radar offers a number of advantages. It uses a modulated light source instead of laser pulses. It allows velocimetry measurements, and offers the ability to filter the signal by eliminating specific noise components in the return signal. We have developed techniques for generating waveforms adapted to lidar-radar, by frequency-shifted optical reinjection in a Q-switched laser. The pulse-to-pulse coherence of the modulation makes it possible to perform lidar telemetry, as well as velocity measurements. The implementation of this type of laser source at different wavelengths (1 \u00b5m and 0.5 \u00b5m) allows to consider different aerial and underwater applications.<\/p>\n\n\n\n

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Fig.1 Principles of velocimetry by a lidar-radar system. The modulated waveforms (left), are produced by reinjection using a frequency shifting external cavity [Vallet2013].<\/figcaption><\/figure>\n\n\n\n

Coherent dual-comb lidar<\/h3>\n\n\n\n

Both time-of-flight lidar and lidar-radar are based on the measurement of the intensity of the light returned by the target. In coherent lidar, the electric field of the light is detected, rather than the intensity, which brings other advantages: range in 1\/r (instead of 1\/r2), ability to measure displacements or speeds with interferometric accuracy, and possibility to filter the signal even at short time scales. The coherent lidar is used for anemometry, among others. The main limitation of coherent lidar is the spatial resolution: to access a high spatial resolution requires to develop coherent and broadband light sources. Multi-heterodyne interferometry (or dual-comb), makes it possible to engineer coherent lidar systems offering a high resolution (sub cm), and with a moderate detection bandwidth. At FOTON Institute, we develop dual-comb architectures from twin frequency shifting loops. One produces the frequency comb of the measurement arm, and the other of the reference channel \u2013 or local oscillator. Besides its simplicity, the specificity of this architecture is to be able to produce quasi-continuous waveforms, while maintaining a resolution limited by the spectrum thanks to a pulse compression effect. Configurations using acousto-optic frequency shifters offer a spatial resolution of the order of cm for an ambiguity distance of a few meters, while electro-optic frequency shifters achieve a sub-mm optical resolution for an ambiguity distance of a few tens of cm. The applications of our systems concern high-resolution automatic vision or underwater imaging.<\/p>\n\n\n\n

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Fig.2 Principle of the dual-comb coherent lidar in a double frequency shifting loop. Recombination of the measure comb (in red) with the reference one (in blue) on a detector produces a signal that reproduces the reflectivity profile along the measuring arm. Insert: coin image [Billault2021].<\/figcaption><\/figure>\n\n\n\n

Financial support<\/h2>\n\n\n\n

ANR<\/a> (COCOA projetc)<\/p>\n\n\n\n

Research staff involved<\/h2>\n\n\n\n

Research engineers, researchers and professors<\/h3>\n\n\n\n
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PhD and post-doc<\/h3>\n\n\n\n
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To learn more…<\/h2>\n\n\n\n