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Numerous applications of Short Wave Infra-Red (SWIR) imaging require short exposure times, typically below 10 ms. Cooled SWIR cameras are over optimized for these applications cases. C-RED 3 is an uncooled, compact, and cost-optimized VGA (640x512) InGaAs camera which offers high imaging performances for short exposure time imaging. C-RED 3 opens new opportunities for industrial and scientific applications.
C-RED 3 is an uncooled camera based on the TECless SNAKE detector from LYNRED. The wager of an uncooled approach was made to offer the best compromise in terms of performance, compactness, and cost-effectiveness.
The first camera developed by First Light Imaging was OCAM2, a fast and low noise camera specifically designed for wavefront sensing applications in the visible range. But astronomers were frustrated not being able to use the infrared spectrum… where sky coverage is more important and stars brighter. The C-RED One camera, based on e- APD technology, was developed as the SWIR counterpart of the OCAM2. However, this camera is rather bulky and targets ultra-high performance applications. The legacy of the C-RED One camera was transferred to the InGaAs technology, giving the C-RED 2 camera. This high speed, low noise cooled camera targets intermediate performance applications, such as low order wavefront sensing. However, in applications when signal level is high there is not necessarily any need for cooling. This leads to the C-RED 3 camera where all the cooling system has been removed and electronics squeezed to give a very small high-speed SWIR camera suited for applications requiring SWaP optimized cameras. Dimensions are reduced to 55 x 55 x 60 mm.
The main characteristics of C-RED 3 are summed up in the table on the left. You can refer to the camera datasheet for more information.
C-RED 3 has been designed to be versatile and easy to integrate, it offers:
C-RED 3 can be controlled via the First Light Vision software. Alternatively, a Software Development Kit (SDK) is available to help you integrate C-RED 3 in your own environment.
Test Measurement | Result | Unit |
Maximum speed (full frame) | 602 | FPS |
Mean dark + readout noise at 600 FPS | < 50 | e- |
Quantization | 14 | Bit |
Quantum effiency (0.9 to 1.7 µm) | > 70 | % |
Operability | > 99.7 | % |
Full well capacity at low gain, 600 FPS | 1400 | ke- |
Full well capacity at high gain, 600 FPS | 33 | ke- |
Maximum soeed 32 x 4 window | 32066 | FPS |
Maximum soeed 320 x 256 window | 1779 | FPS |
Power consumption | 6.5 | W |
Let us try to understand when and how to use C-RED 3…
Potential users may be anxious at the idea of using an uncooled camera… Understanding the impacts of a higher working temperature on the imaging performances is the first step to adopting C-RED 3.
Illustrated below is the Quantum Efficiency (QE) response of InGaAs versus wavelength and operating temperature.
The quantum efficiency is both shifted (1) and reduced (2) when temperature increases:
Example: Your laser emits at 1200 nm, the QE curve shift does not affect your measurement. If the camera is at 30°C, the QE is 15% less than if the camera was cooled to 0°C. To reach an equivalent signal level, you can integrate for longer.
The useful dynamic is the part of the integrating capacity which is available for photons. It is limited by dark signal, caused by thermally generated electrons in the sensor.
The dark signal increases linearly with integration time and exponentially with temperature until the detector saturates.
For short integration times the dark signal is low and the useful dynamic is preserved. The figure above shows typical values in medium gain.
Example: Your application requires a 1 ms integration time and medium gain mode. The room temperature is elevated, the camera is operating at 40°C. In this case, 600 e- are thermally generated… occupying ~0.5 % of the full dynamic!
The two main noise sources linked to the detector are: dark current noise and readout noise. Dark current noise is the square root of the dark signal, hence increasing with both integration time and temperature.
The figure above illustrates that in medium gain mode for high framerates / short integration times, the total noise is kept small.
To accurately detect a signal, it must be at least 3 times higher than the dark noise.
Example: A 1300 nm laser incident on the detector provides 1014 photons⋅s-1 ⋅mm-2 (15 µW⋅mm-2 ). In medium gain and tint 1 ms, your signal represents 1014 *tint*QE*pix_size = 15⋅10 3 e-⋅pix-1 . The total dark noise is < 60 e-. Signal to noise ratio is well over 3. Your signal can easily be detected.
These considerations lead us to two questions: when does it become useful to stabilize the temperature of C-RED 3 and when does it become necessary to switch to C-RED 2 Lite (stabilized camera) or C-RED 2 (cooled camera)?
In some specific cases, stabilizing the sensor temperature may be necessary:
First Light Imaging offers the following solution:
C-RED 3 alone is not stabilized, which will result in temperature variations in time. Available with C-RED 3 is a compact water cooling adapter which can be screwed below the camera to stabilize the temperature. A passive or active water chiller must be connected to the bloc. This solution preserves compactness and cost-effectiveness.
C-RED 2 Lite is a stabilized version of the C-RED 3 camera. “Stabilized” means that the camera has the ability to maintain the sensor at a target temperature. This is done via two internal thermoelectric coolers (TEC). First Light Imaging guarantees a temperature difference of 25°C between the outer case and the sensor. Depending on how well the heat is dissipated away from the case, the sensor can be set to lower temperatures. The advantages of this solution over the C-RED 3 with a cooling plate are : higher cooling capability, guaranteed stabilization performance, and less bulkiness.
To choose between a cooled, stabilized or uncooled camera, the question you need to ask yourself is: is your acquisition limited by photon noise or dark current noise?
C-RED 3 readout noise versus framerate (integration time is equal to the inverse of framerate) at 35°C shows that:
Take-home message
There are three effects of temperature on a camera's performances:
However, these effects are not necessarily drawbacks.
C-RED 3 offers high performances at short integration times (below 10 ms).
You should consider regulating or cooling the sensor only for specific applications or if using long integration times.
C-RED 3 is integrated in First Light Vision, the Graphical User Interface (GUI) developed for all C-RED and C-BLUE cameras by First Light Imaging. It is compatible with both USB and CL interfaces and is cross-platform (x86 / ARM, Windows/ Linux). It is user friendly, allowing easy controlling, and offers multiple functionalities for higher end usage. To help programmers develop their own interface for C-RED 3, the Software Development Kit (SDK) provides source codes for short demos in C/C++, Labview, Python and MATLAB. C-RED 3 can also be controlled using Micro Manager.
Several on-the-fly corrections can be applied to C-RED 3 to optimize the raw data. The hardware processing developed by First Light Imaging based on the expertise acquired with the C-RED One and C-RED 2 cameras makes C-RED 3 a high performance camera.
A bad pixel map is built in the camera during the manufacturing. This map can be edited by the user to add and/or remove bad pixels.
Dark Signal Non Uniformity (DSNU) is one source of pattern noise. It results from an offset (bias) resulting from electronic disparity, and dark current. DSNU correction is usually fixed by subtracting a dark frame from the useful image.
Date: April 2022
Author: Cecile Brun
Category: Application Note