JMZawodny said:
tron said:
PureClassA said:
If they can generate the ISO1600 noise levels at ISO 3200 and/or 6400, that would be a good win. When I use the 1DX, I'm never below ISO 1600 and 75%+ as ISO 3200 - 6400.
tron said:
I do not believe that it will have 15 stops of DR. I will be satisfied though if it will come very close to 14.
OK, that's High ISO performance but I am interested in it too. I use my 5D3 for landscape astrophotography and I have to use it up to ISO 10000. So, I would welcome a serious improvement in high ISO too....
Also, the fact that 1DxII will be 22Mp it will make it look like a super charged 5D3!
You should always shoot Astro at the ISO setting that provides the gain to digitize 1 electron as one count. Typically that ISO is near 800. Anything less and you begin to lose information for the sake of increased dynamic range. More than that and you lose dynamic range. Shooting at 10000 simply reduces the dynamic range with absolutely nothing in return. Your ISO 10000 histograms very likely look like a comb.
To address this more directly. There is always noise in the conversion. It actually is not possible to always convert 1 electron to 1 ADU because noise will usually mean you get 0 ADU, or >1 ADU.
Technically speaking, it is better to sample every electron as finely as possible. That means you want a gain (in terms of e-/ADU) of LESS than 1. Nyquist would dictate a gain of 0.5e-/ADU, however that only really works for something like an audio signal, however because of the various noise terms that play a role with digital imaging (including read noise and PRNU) and because we usually stack, a gain of 0.3e-/ADU is better, and higher is certainly not bad, especially with very faint signals. There is certainly a balancing act here...too high of an ISO and you will throw away too much dynamic range...and in the case of a Canon DSLR, too low of an ISO and read noise will increase to ridiculous levels (anything over 10e- and you have to start wondering why your bothering...the 5D III has ~35e- RN @ ISO 100...square that, you add 1225e- noise in your noise term when calculating SNR!!!)
There is a caveat here. Outside of the >10e- read noise scenario...read noise usually barely matters! This is because for most imagers, there are other sources of noise that are more significant. Dark current is one, which can add as much as 1500e- signal or around there, which is 30e- noise. Another significant source of noise is light pollution, which can add anywhere from 200 to 2000e- additional signal outside of a nice dark site (yellow through white zones on the bortle scale). With minimal dark current and no light pollution, an SNR calculation might look like this (assuming 50e- signal from space in say a 120 second exposure ):
Code:
50e-/SQRT(50e- + 10e-^2) = 4.1:1
At high ISO, where your better sampling each and every electron, your read noise (in relative terms) is smaller:
Code:
50e-/SQRT(50e- + 3e-^2) = 6.5:1
An improvement of almost 60%. Quite significant. However it's never that simple. Add in dark current at say 10e-/s/px @ 20C (i.e. 5D II):
Code:
50e-/SQRT(50e- + (10*120) + 3e-^2) = 50e-/SQRT(50e- + 1200e- + 9e-) = 1.41:1
That dark current totally decimated our SNR. Increasing read noise to 10e- really doesn't matter much at that point:
Code:
50e-/SQRT(50e- + (10*120) + 10e-^2) = 50e-/SQRT(50e- + 1200e- + 100e-) = 1.36:1
Less than a 4% difference here. Read noise matters even less when we factor in light pollution (say deep in a red zone, suburbia central):
Code:
50e-/SQRT(50e- + 1500e- + (10e-/s*120s) + 10e-^2) = 50e-/SQRT(50e- + 1500e- + 1200e- + 100e-) = 0.94:1
Even if you had a mere 1e- read noise, it wouldn't matter:
Code:
50e-/SQRT(50e- + 1500e- + (10e-/s*120s) + 1e-^2) = 50e-/SQRT(50e- + 1500e- + 1200e- + 1e-) = 0.95:1
It really doesn't matter if you image at ISO 400, 800, or 1600...in the end, the amount of read noise barely affects the results. Dark current and light pollution dominate by such a significant margin. That changes if you can regulate your sensor temp, and find dark skies, though:
Code:
50e-/SQRT(50e- + 30e- + (0.02e-/s*120s) + 3e-^2) = 5.23:1
Bump read noise up to 10e-:
Code:
50e-/SQRT(50e- + 30e- + (0.02e-/s*120s) + 10e-^2) = 3.7:1
Read noise becomes a more significant factor when your imaging under pristine dark skies (i.e. 21.5mag/sq" or better, deep blue zone, gray zone, black zone) with very low dark current. Dark current itself could easily be the single most devastating noise term you may have to deal with (i.e. dark sky...in the summer):
Code:
50e-/SQRT(50e- + 30e- + (5e-/s*120s) + 3e-^2) = 1.9:1
50e-/SQRT(50e- + 30e- + (10e-/s*120s) + 3e-^2) = 1.4:1