... for those with a technical bent:
http://theory.uchicago.edu/~ejm/pix/20d/te...oise/index.html
Put on your propeller beanies
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Considering the scope and quality of Emil's post, I am quite surprised that there have not been more comments. Perhaps readers need additional time to digest the article. To get discussion started, here are a few observations.
"one might think that read noise is a fixed cost per pixel in recording an image, again assuming that the same quality of circuit elements are employed."
This does appear to be true, but should one measure the cost in terms of noise expressed in data numbers (DN, raw pixel values) or electrons? In [a href=\"http://www.clarkvision.com/imagedetail/digital.sensor.performance.summary/#read_noise]Clark Fig 3[/url] of a post, Roger Clark notes that read noise expressed in electrons is similar in sensors of the same generation but of differing pixel sizes. Read noise varies with ISO, but read noise quoted in manufacturer's spec sheets is typically for unity gain, which complicates the analysis since unity gain is correlated with pixel size.
One can increase signal to noise at the expense of resolution by pixel binning as Emil discusses. The results of binning differ when binning is done in hardware prior to digitization or in software by downsizing. Consider hardware binning in which 4 pixels in a 2 by 2 array are combined and read out together, as described
here. The four pixels are combined into a superpixel, which is read out with the same read noise (in electrons) as for a single small pixel. This implies that when other factors are held constant, read noise is independent of pixel size. If one performed binning in Photoshop after the fact, the resulting superpixel would have incurred 4 read noise contributions, not a single one as with hardware binning.
If the read noise is similar for large and small pixels, the large pixel camera still has an advantage when read noise is measured in DNs rather than electrons. This is because of camera gain as Roger explains in this example:
Clark Table 3. See the text just following table 3.
"The realization from Table 3 is even though the read noise is similar in terms of electrons, the effect on the image is huge because of the gain factor. Thus shadow detail on a small sensor is severely compromised as the gain factor drops."
Seriously, though, fans of this site's disquisition on ETTR might be interested in the analysis on page 3 of the article, among other things.
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Any comments by the resident "experts" who have expounded on the "levels theory", where half the levels are in the brightest f/stop? The improved signal to noise ratio with ETTR is a definite benefit, but how does it scale to human perception? Considering only shot noise, the S:N increases by a factor of sqrt(2) with doubling of the exposure. Looking at Emil's S:N graphic demonstration, I perceive only slight image improvement with a doubling of S:N. Is this a log function or what?
Bill