Emil,
When calculating the DR at full well, why do you use the read noise for ISO 1600? Or is the read noise at base ISO that low?
Bill
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I used to think this was goofy, but now I know better (and finally understand what Roger Clark has been trying to say for a long time). The read noise in absolute terms (eg in photoelectron equivalents) is much higher at base ISO, but this fact is due to the electronics downstream of the sensor (the variable gain amplifier that implements ISO, and the ADC) rather than the noise of the sensor capture itself. One can see that from the plots of read noise vs ISO at
[a href=\"http://theory.uchicago.edu/~ejm/pix/20d/tests/noise/noise-p2.html#read_vs_iso]http://theory.uchicago.edu/~ejm/pix/20d/te...tml#read_vs_iso[/url]
See in particular the little table below fig 15. The sensor noise is amplified by the ISO amplification, which is why high ISO read noise is large in ADU, but low when referred back to photoelectrons. The low ISO read noise is small in ADU, but large when referred back to photoelectrons; the amplifier/ADC noise is independent of ISO when denominated in ADU. So the dominant contribution to read noise at low ISO comes from the ISO amplifier and ADC, while at high ISO it is almost entirely due to the photosite electronics. What this means is that the read noise at low ISO is being limited by the amplifier/ADC components, since if they contributed less than the sensor itself, one would get the full DR of the sensor.
This is why Roger Clark is careful to distinguish what he calls "sensor DR" from "camera DR". The former is about 14 stops, while the latter is a bit under 12 stops for the 1D3/1Ds3. The difference is due to the quality/capability of the electronics downstream of the sensor in Canon cameras (and also the D3/D300, I should add).
One then might ask, so what? Won't the electronics downstream of the sensor always limit the DR in this way? I don't think so. In principle one could take the sensor output and run it through two parallel signal processing routes -- one set to ISO 100 and the other set to ISO 1600 (think of it as "in-camera HDR"). The low ISO path captures the highlights, but has four times the read noise in electrons. The high ISO path has the highlights clipped, but that's OK we're going to take those from the other path anyway; instead, the high ISO path captures the shadows with much lower read noise in electrons. After digitisation, the two paths can be combined in much the same way one combines two exposures in HDR, one for highlights and the other for shadows. It would be trivial to code this, the only cost is the extra hardware for the dual amplifications. And since one is always capturing the full DR that the sensor can deliver, there is no reason whatsoever to have variable gain; ISO can be implemented as it is in many MFDB's, as a metadata tag for the raw converter to apply. The difference is that one would actually have about 14 stops of DR and high bit depth would actually be justified for a change.