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Electronic Imaging & Signal Processing

Measuring random sensor noise in cameras

A modified method enables fast and accurate measurement of temporal noise in photo and video camera sensors using a remarkably small number of reference frames.
12 May 2015, SPIE Newsroom. DOI: 10.1117/2.1201505.005974

Photo and video cameras are popular tools among both scientists and consumers. Sensor noise, which can be divided into random and pattern components, represents one of the main factors limiting the amount of data that a camera can produce.1 Temporal noise varies randomly, whereas spatial noise has a pattern that arises due to sensor non-uniformities. Spatial noise is usually several magnitudes lower than temporal, to the extent that it can be neglected at first approximation. Knowledge of temporal noise is required in a number of optical digital systems, including wavefront coding for imaging (for aberration correction, extended depth of field, pattern recognition, and optical encryption), digital holography, image forensics, and increasing camera signal-to-noise ratio.

Purchase SPIE Field Guide to Image ProcessingCamera sensor noise can be measured using a variety of techniques. The most widely used among these is EMVA Standard 1288,2 which allows accurate dark and light temporal noise measurement but can be technically difficult to implement. Additionally, if the dependency of the temporal noise on signal value is required in detail, thousands of shots are necessary, making such measurement extremely time-consuming. Analysis of existing temporal noise measurement methods proves that noise measurement by automatic segmentation of non-uniform targets represents one of the fastest and simplest techniques.3 This technique suffers from several significant drawbacks, however, such as an inability to measure noise over the full signal range and a failure to divide full temporal noise into light and dark components. Furthermore, researchers have failed to provide estimates of measurement errors, making its accuracy unknown.

We have proposed a modification of this method4 that provides an unbiased estimation of the temporal noise, faster processing speeds, and separate measurements of dark and light temporal noise. Using our method, just two frames are required for noise measurement.

Our modification consists of two experimental measurement steps and three pure signal processing steps. Using our procedure, we first create a scene (fixed target) with two simple constraints: the brightness dynamic range of a scene must exceed the dynamic range of a studied camera sensor; and the non-uniformity of scene brightness must provide (in registered frames) the presence of all possible signal values within the dynamic range of the sensor.

These constraints enable us to obtain the dependency of temporal noise on signal value for all possible values within the photosensor dynamic range. This makes it possible to find not only full temporal noise, but also dark temporal noise and the dependency of light temporal noise on signal value. To achieve the best possible measurement accuracy, the intensity histogram of registered images should be close to uniform. To accomplish this, we used a defocused image of a binary transparency with a contrast ratio exceeding the dynamic range of the camera. An additional grayscale transparency located nearby allows the histogram of the registered image to be equalized. These binary and grayscale transparencies form the test scene. We then register several shots of this scene and subsequently calculate the pointwise averaged image. The array of squared standard deviations in the signals of each pixel is also calculated, giving the array of variances. From this array, pixels with equivalent signal value from the averaged image are chosen and their mean value is calculated. The temporal noise estimation for this signal value is the square root of the mean variance.

These procedures are performed for all signals within the dynamic range of the sensor and can be calculated very fast (1–20s) using a standard computer. Figure 1 shows the scheme of temporal noise measurement.

Figure 1. A scheme of our proposed technique for temporal noise measurement. A non-uniform test scene is illuminated and registered by the camera. The frames that are obtained are averaged in one array, and the squared standard deviations of the signals of each pixel are used as the second array. Pixels corresponding to the equal signal value from the first array are then chosen from the second array, and their mean value is calculated. The temporal noise estimation for the signal value is the square root of the mean variance.

To demonstrate our proposed modification, we chose four cameras of different types: a consumer photo camera (Canon EOS 400D: CMOS; 10.1MP; 12-bit analog-to-digital converter, ADC); a scientific camera (MegaPlus II ES11000: CCD; 10.7MP; 12-bit ADC); an industrial camera (PixeLink PL-B781F: CMOS; 6.6MP; 10-bit ADC); and a video-surveillance camera (Watec LCL-902C: CCD; 0.47MP; external 8-bit ADC). Figure 2 shows the experimental dependencies of full temporal noise on signal value,5 obtained using averaging over 64 frames. The fitted curves of full temporal noise, based on a Poisson distribution of the quantity of photons falling on the photosensor, are also shown. The experimental and calculated dependencies are in good agreement with each other, excluding areas near saturation, where temporal noise decreases.

Figure 2. Experimental and calculated dependencies of temporal noise on signal value for a variety of cameras: (a) Canon EOS 400D; (b) MegaPlus II ES11000; (c) PixeLink PL-B781F; and (d) Watec LCL-902C.

Figure 3 shows the obtained experimental dependency of temporal noise on signal value, averaging over two and four frames.4 Only noise measurement errors differ, demonstrating that the proposed method provides unbiased estimation of temporal noise.

Figure 3. Experimental dependencies of temporal noise on signal value for the MegaPlus II ES11000, obtained from (a) two and (b) four frames.
Table 1.Experimental and theoretical relative errors of temporal noise measurement.
Number ofRelative errorRelative error
frames% (mean experimental)% (theoretical)
64 0.190 0.186
32 0.289 0.288
16 0.415 0.415
8 0.607 0.607
4 0.927 0.927
2 1.604 1.605

We have also theoretically and experimentally estimated the measurement errors using this proposed technique. The mean values of errors obtained for signal values in the range 0–3300 are shown in Table 1. The mean relative difference between the corresponding theoretical and experimental values is 0.4%. Using two frames, the error value is 1.6%.

In summary, our modified temporal noise measurement method provides a convenient and accurate way to assess the output of photo and video cameras using a remarkably small number of frames. Over the past few years, we have proposed several techniques for electronic imaging and signal processing. These include measurement of the 2D modulation transfer function,5, 6 increasing the signal-to-noise ratio of registered images by using the light spatial noise portrait of the camera's sensor,7 and increasing the noise-characteristics measurement accuracy for cameras with color filter sensors.8 In future work, we plan to measure the noise and spectral characteristics of other cameras, including web cameras and dashboard cameras. We are also currently developing our technique for the simple measurement of spatial noise in cameras.

Pavel Cheremkhin, Nikolay Evtikhiev, Vitaly Krasnov, Vladislav Rodin, Rostislav Starikov, Sergey Starikov
Department of Laser Physics
National Research Nuclear University MEPhI
(Moscow Engineering Physics Institute)
Moscow, Russia

Pavel Arkadevich Cheremkhin received his PhD in physics in 2013 and is an assistant professor in the Department of Laser Physics. His main research interests are digital holography, camera noise, diffraction optics, wavefront reconstruction, signal processing, and analog optical links. He has more than 70 publications in journals and conferences.

Vitaly Vyacheslavovich Krasnov received his PhD in physics in 2013 and is now an assistant professor in the Department of Laser Physics. His main research interests are optical encryption, diffractive optical element synthesis, wavefront reconstruction, signal processing, and camera noise. He has more than 60 publications in journals and conferences.

1. J. R. Janesick, Scientific Charge-Coupled Devices, SPIE Publications, Bellingham, Washington, 2001.
2. http://www.emva.org/cms/upload/Standards/Stadard_1288/EMVA1288-3.0.pdf EMVA Standard 1288: Standard for Characterization of Image Sensors and Cameras. Accessed 6 April 2015.
3. A. Foi, S. Alenius, V. Katkovnik, K. Egiazarian, Noise measurement for raw-data of digital imaging sensors by automatic segmentation of non-uniform targets, IEEE Sensors J. 7(10), p. 1456-1461, 2007. doi:10.1109/JSEN.2007.904864
4. P. A. Cheremkhin, N. N. Evtikhiev, V. V. Krasnov, V. G. Rodin, S. N. Starikov, Modified temporal noise measurement method with automatic segmentation of non-uniform target, its accuracy estimation, and application to cameras of different types, Opt. Eng. 53(10), p. 102107, 2014. doi:10.1117/1.OE.53.10.102107
5. N. N. Evtikhiev, S. N. Starikov, P. A. Cheryomkhin, V. V. Krasnov, Measurement of noises and modulation transfer function of cameras used in optical-digital correlators, Proc. SPIE 8301, p. 830113, 2012. doi:10.1117/12.908198
6. N. N. Evtikhiev, V. V. Krasnov, S. N. Starikov, A method of generating amplitude masks with a constant power spectra and using them to measure the two-dimensional modulation-transfer functions of optical systems, J. Opt. Technol. 80(5), p. 294-300, 2013. doi:10.1364/JOT.80.000294
7. N. N. Evtikhiev, P. A. Cheremkhin, V. V. Krasnov, V. G. Rodin, S. N. Starikov, Increasing signal-to-noise ratio of registered images by using light spatial noise portrait of camera's photosensor, Proc. SPIE 9025, p. 90250X, 2014. doi:10.1117/12.2037277
8. V. V. Lesnichii, N. V. Petrov, P. A. Cheremkhin, A technique of measuring spectral characteristics of detector arrays in amateur and professional photocameras and their application for problems of digital holography, Opt. Spectrosc. 115(4), p. 557-566, 2013. doi:10.1134/S0030400X13100093