CMOS vs. CCD? (Any advantages)

Nobody wrote about the selfheating effects. With long exposures CCD gets (very) noisy whereas CMOS stays relatively cool by its far lower power consumption. IMO it is the reason why CMOS camera's have live view. Regards,
--
WillemB
 
Nobody wrote about the selfheating effects. With long exposures CCD
gets (very) noisy whereas CMOS stays relatively cool by its far lower
power consumption. IMO it is the reason why CMOS camera's have live
view. Regards,
How big a problem is this? CCD sensors require higher voltages, but does this increase power consumption during exposure, or only during read-out?

I can see this will be a problem for rapid frame rates and video, but during long exposures how much electrical activity is there?

Cheers.
--
Alan Robinson
 
Thanks for that link from clarkvision. It will take some study to get
my head around all the graphs. - Will
Clark's stuff is pretty well regarded, but his definition of dynamic range as 'full well capacity / read noise' is a questionable. He uses the read noise measured at high ISO where only a fraction of the full well capacity can be recorded. For most DSLRs the read noise at low ISO is rather higher, and the achievable dynamic range lower than this estimate.

Clark comes from an astrophotography perspective. If you are still looking for bedtime reading after finishing clarkvision, try Emil Martinec's site: http://theory.uchicago.edu/~ejm/pix/20d/tests/noise/index.html

Cheers,
--
Alan Robinson
 
Thanks for that link from clarkvision. It will take some study to get
my head around all the graphs. - Will
Clark's stuff is pretty well regarded, but his definition of dynamic
range as 'full well capacity / read noise' is a questionable. He
uses the read noise measured at high ISO where only a fraction of the
full well capacity can be recorded. For most DSLRs the read noise at
low ISO is rather higher, and the achievable dynamic range lower than
this estimate.
Actually, Clark is reasonably careful in his choice of words to distinguish what he calls 'sensor dynamic range' from 'camera dynamic range'; what he doesn't explain very well is why he can determine those two quantities separately, and why 'sensor DR' is equal to 'full well capacity/high ISO read noise'.

For any camera, of course, the delivered DR at any ISO is the raw saturation level divided by the read noise at that ISO. This is the definition that Clark uses when he reports 'camera dynamic range'; unfortunately, he doesn't record those for more than a handful of cameras, and spends most of his time quoting values for 'sensor dynamic range', which is not what the camera delivers.

So how does he get at this 'sensor DR'? Read noise has two broad classes of contributions -- those upstream of the ISO amplifier and those downstream. The latter don't get amplified proportionally by the ISO setting, while the former do; thus by measuring the read noise at several ISO settings one can determine the upstream and downstream contributions separately, see the table below fig 15 on page 3 of my article

http://theory.uchicago.edu/~ejm/pix/20d/tests/noise/noise-p2.html#read_vs_iso

It turns out that low ISO read noise is dominated by the downstream contributions -- the ISO amplifier itself and the ADC -- while high ISO read noise is almost entirely due to the amplified upstream contribution, which comes from the sensor. If the downstream electronics weren't overwhelming the sensor contribution at low ISO, the delivered DR would be the full well capacity/high ISO read noise (all measured in electrons), which on pro level Canons and Nikons is about 14 stops. It is only the limitations of the amplifier/ADC combination that are preventing the delivery of that DR in current cameras.

I think there are easy technology solutions to get the full sensor DR, I have described them elsewhere:

http://forums.dpreview.com/forums/read.asp?forum=1032&message=28567133

--
emil
--



http://theory.uchicago.edu/~ejm/pix/20d/
 
Actually, Clark is reasonably careful in his choice of words to
distinguish what he calls 'sensor dynamic range' from 'camera dynamic
range'; what he doesn't explain very well is why he can determine
those two quantities separately, and why 'sensor DR' is equal to
'full well capacity/high ISO read noise'.
Good point. I had forgotten about his ISO-dependent dynamic range calculations on individual cameras. It is still potentially misleading if you don't read the entire site.
For any camera, of course, the delivered DR at any ISO is the raw
saturation level divided by the read noise at that ISO. This is the
definition that Clark uses when he reports 'camera dynamic range';
unfortunately, he doesn't record those for more than a handful of
cameras, and spends most of his time quoting values for 'sensor
dynamic range', which is not what the camera delivers.

So how does he get at this 'sensor DR'? Read noise has two broad
classes of contributions -- those upstream of the ISO amplifier and
those downstream. The latter don't get amplified proportionally by
the ISO setting, while the former do; thus by measuring the read
noise at several ISO settings one can determine the upstream and
downstream contributions separately, see the table below fig 15 on
page 3 of my article

http://theory.uchicago.edu/~ejm/pix/20d/tests/noise/noise-p2.html#read_vs_iso

It turns out that low ISO read noise is dominated by the downstream
contributions -- the ISO amplifier itself and the ADC -- while high
ISO read noise is almost entirely due to the amplified upstream
contribution, which comes from the sensor. If the downstream
electronics weren't overwhelming the sensor contribution at low ISO,
the delivered DR would be the full well capacity/high ISO read
noise (all measured in electrons), which on pro level Canons and
Nikons is about 14 stops. It is only the limitations of the
amplifier/ADC combination that are preventing the delivery of that DR
in current cameras.
That all makes sense. Are you convinced there is no per-pixel variable amplification? That seems logical, in terms of system complexity, and scope for scaling errors causing gain-dependent pattern noise, but I don't know enough about the internals of these sensors to be sure.
I think there are easy technology solutions to get the full sensor
DR, I have described them elsewhere:
http://forums.dpreview.com/forums/read.asp?forum=1032&message=28567133
I can see that working. You might have slew rate problems on the high gain amplifiers as they exceed the ADC range and potentially saturate. That should be fixable by substituting the base ISO output for one or two pixels after the high gain output comes back into range. We would have a halo of higher absolute noise levels at such light/dark transitions, but I believe the subjective impact would be minimal.

I am assuming that all this is done in-camera. Another option would be to dump both ADC streams into the raw file, giving the option of smarter processing off-line.

It all seems practicable - especially for the higher end cameras. It would certainly put more pressure on the medium format market.

Regards,
Alan
--
Alan Robinson
 
I take it you are interested in low ISO performance. According to
the data on Roger Clark's site
The Nikon D200 (CCD) had better dynamic range than the Canon 40D
(CMOS) at low ISO, in spite of lower well capacity in the CCD sensor.
However, the CMOS read noise was much lower at high ISO.
The newer Nikon D300 CMOS sensor has comparable high ISO noise and
well capacity to the 40D, and better low ISO noise than both D200 and
40D.
It was pointed out to Roger a couple of years ago that the software/method he was using was grossly underestimating Nikon D200 read noise, but he hasn't corrected the values. The D200 starts out just like the 10D 20D and 5D, with about 2 12-bit ADU of read noise at base ISO, when I measured it a couple opf years ago. Unlike these Canons, though, the noise scales nearly linearly with ISO.

--
John

 
Thanks for that link from clarkvision. It will take some study to get
my head around all the graphs. - Will
Clark's stuff is pretty well regarded, but his definition of dynamic
range as 'full well capacity / read noise' is a questionable. He
uses the read noise measured at high ISO where only a fraction of the
full well capacity can be recorded. For most DSLRs the read noise at
low ISO is rather higher, and the achievable dynamic range lower than
this estimate.
Actually, Clark is reasonably careful in his choice of words to
distinguish what he calls 'sensor dynamic range' from 'camera dynamic
range'; what he doesn't explain very well is why he can determine
those two quantities separately, and why 'sensor DR' is equal to
'full well capacity/high ISO read noise'.
Well, he's explained it to me like this; he's interested only in the noise that occurs at the photosite or the first read, and that everything afterward is ADC noise, and irrelevant for the discussion.
For any camera, of course, the delivered DR at any ISO is the raw
saturation level divided by the read noise at that ISO. This is the
definition that Clark uses when he reports 'camera dynamic range';
unfortunately, he doesn't record those for more than a handful of
cameras, and spends most of his time quoting values for 'sensor
dynamic range', which is not what the camera delivers.
Well, he is one of the pillars of pixel-centric thought, and he is obsessed with the dream of humongous pixels with only shot noise, and DR of the pixel being equal to its maximum electron count. I dream of pure shot noise, too, but in shot glasses, not soup bowls!
So how does he get at this 'sensor DR'? Read noise has two broad
classes of contributions -- those upstream of the ISO amplifier and
those downstream. The latter don't get amplified proportionally by
the ISO setting, while the former do; thus by measuring the read
noise at several ISO settings one can determine the upstream and
downstream contributions separately, see the table below fig 15 on
page 3 of my article

http://theory.uchicago.edu/~ejm/pix/20d/tests/noise/noise-p2.html#read_vs_iso

It turns out that low ISO read noise is dominated by the downstream
contributions -- the ISO amplifier itself and the ADC -- while high
ISO read noise is almost entirely due to the amplified upstream
contribution, which comes from the sensor. If the downstream
electronics weren't overwhelming the sensor contribution at low ISO,
the delivered DR would be the full well capacity/high ISO read
noise (all measured in electrons), which on pro level Canons and
Nikons is about 14 stops. It is only the limitations of the
amplifier/ADC combination that are preventing the delivery of that DR
in current cameras.
Well, I agree with you on many things, but I have to take exception to this. I believe that the transistors at the photosites make the sensor read noise different at different ISOs. I know you have an equation that makes it work for the in-between ISOs, but you can make an equation to fit any curve. I consider the practicalities, and I can not imagine any design scenario where Canon would introduce 1/3-stop ISOs through variable gain at a stage later than where it does the K*(2^N) gains ... why not do them there, too, and get consistently smooth ISO vs read noise curves? It just doesn't make any sense to me. Also, there is the issue that line noises are greatest, relative to absolute signal at base ISOs in Canons. That means that they have a difference that should be occurring on the sensor - more difficulty black-leveling each line when there is less gain. I don't think any of the later stages would have any issues that relate to individual lines; individual lines distinguish themselves only on the sensor, I would think.

--
John

 
Interesting article, thanks. I see you noted that Nikons clip the
black point; I attempted to convince someone else once but he didn't
listen (he also got some other strange results about the new canons).
It seems like everyone except Canon clips the blackpoints, and many clip it higher than mean black. My estimates re-distributing D3 blacks suggest that the D3 clips black at what should be 9 14-bit ADUs above black.

I determined this by taking a blackframe from a high-ISO file, and making a histogram and importing it into Excel. I looked at the curve from 1 to the highest RAW value in the black area, and estimated what the population would be from the next lower value below the non-zero part of the histogram, and added 1 to the values and inserted the new population. I did this until the amount of 0 vales and positive values made sense for a true mean black clip, and I had added 9 populations before this happened. I did it at high ISO because the curve is shallower, simpler, and easier to predict than base ISO.

--
John

 
I take it you are interested in low ISO performance. According to
the data on Roger Clark's site
The Nikon D200 (CCD) had better dynamic range than the Canon 40D
(CMOS) at low ISO, in spite of lower well capacity in the CCD sensor.
However, the CMOS read noise was much lower at high ISO.
The newer Nikon D300 CMOS sensor has comparable high ISO noise and
well capacity to the 40D, and better low ISO noise than both D200 and
40D.
It was pointed out to Roger a couple of years ago that the
software/method he was using was grossly underestimating Nikon D200
read noise, but he hasn't corrected the values. The D200 starts out
just like the 10D 20D and 5D, with about 2 12-bit ADU of read noise
at base ISO, when I measured it a couple opf years ago. Unlike these
Canons, though, the noise scales nearly linearly with ISO.
Thanks for the correction John.

Is this the black level clipping problem? Unfortunately, Roger's values are conveniently tabulated and easy to find. Perhaps I should have used Gordon's analysis of the Pentax K10D sensor for my example of good CCD dynamic range at low ISO. http://daystarvisions.com/Docs/Rvws/K20D/pg3.html

This is what comes of getting sucked into internet discussions. The intent in my original post was to say "Here's an interesting presentation by Eric Fossum. Draw your own conclusions".

Enjoy the rest of the day.

Alan

--
Alan Robinson
 
Interesting article, thanks. I see you noted that Nikons clip the
black point; I attempted to convince someone else once but he didn't
listen (he also got some other strange results about the new canons).
It seems like everyone except Canon clips the blackpoints, and many
clip it higher than mean black. My estimates re-distributing D3
blacks suggest that the D3 clips black at what should be 9 14-bit
ADUs above black.

I determined this by taking a blackframe from a high-ISO file, and
making a histogram and importing it into Excel. I looked at the
curve from 1 to the highest RAW value in the black area, and
estimated what the population would be from the next lower value
below the non-zero part of the histogram, and added 1 to the values
and inserted the new population. I did this until the amount of 0
vales and positive values made sense for a true mean black clip, and
I had added 9 populations before this happened. I did it at high ISO
because the curve is shallower, simpler, and easier to predict than
base ISO.
Assuming the read noise histogram is well approximated by a Gaussian distribution, one can simply use the error function (the integral of a gaussian up to some point). Ask what percentage of pixels have nonzero levels, double it (since the gaussian distribution is symmetric about the mean, while the error function integrates only above the mean), and find the argument of the error function which yields this number. This gives the number of standard deviations above the mean where the signal has been clipped; multiply by the read noise and you have the number of ADU above black at which the signal has been clipped.

Doing this exercise for the D300 gave 5ADU above true black for the clipping point at base ISO (200).

--
emil
--



http://theory.uchicago.edu/~ejm/pix/20d/
 
Actually, Clark is reasonably careful in his choice of words to
distinguish what he calls 'sensor dynamic range' from 'camera dynamic
range'; what he doesn't explain very well is why he can determine
those two quantities separately, and why 'sensor DR' is equal to
'full well capacity/high ISO read noise'.
Well, he's explained it to me like this; he's interested only in the
noise that occurs at the photosite or the first read, and that
everything afterward is ADC noise, and irrelevant for the discussion.
The downstream noise is quite relevant for current designs, since it limits the low ISO DR that the cameras deliver.
Well, he is one of the pillars of pixel-centric thought, and he is
obsessed with the dream of humongous pixels with only shot noise, and
DR of the pixel being equal to its maximum electron count. I dream
of pure shot noise, too, but in shot glasses, not soup bowls!
Whether sensor DR goes up or down with pixel size depends crucially on having the right model for read noise, and understanding how that scales with pixel size. If the low ISO read noise is dominated by VGA/ADC noise that is not at the photosite, then this number is largely irrelevant for determining how read noise scales with pixel size. If the high ISO read noise is determined by the photosite properties, then one should be using that noise to do one's scaling analysis. If that noise, referred to electrons, doesn't shrink as the pixel pitch, then larger pixels indeed have more per area DR and less per area read noise. One should worry given the 4-5 electrons of high ISO read noise of current CMOS DSLR's with 6-8µ pixels, vs the 3-4 electrons of read noise of current CCD digicams with 2µ pixels.
So how does he get at this 'sensor DR'? Read noise has two broad
classes of contributions -- those upstream of the ISO amplifier and
those downstream. The latter don't get amplified proportionally by
the ISO setting, while the former do; thus by measuring the read
noise at several ISO settings one can determine the upstream and
downstream contributions separately, see the table below fig 15 on
page 3 of my article

http://theory.uchicago.edu/~ejm/pix/20d/tests/noise/noise-p2.html#read_vs_iso

It turns out that low ISO read noise is dominated by the downstream
contributions -- the ISO amplifier itself and the ADC -- while high
ISO read noise is almost entirely due to the amplified upstream
contribution, which comes from the sensor. If the downstream
electronics weren't overwhelming the sensor contribution at low ISO,
the delivered DR would be the full well capacity/high ISO read
noise (all measured in electrons), which on pro level Canons and
Nikons is about 14 stops. It is only the limitations of the
amplifier/ADC combination that are preventing the delivery of that DR
in current cameras.
Well, I agree with you on many things, but I have to take exception
to this. I believe that the transistors at the photosites make the
sensor read noise different at different ISOs.
What is the evidence for this? Most explanations I have seen of the transistors at the photosite, eg
http://en.wikipedia.org/wiki/Active_pixel_sensor

give them only the job of holding the charge, or switching the output among rows/columns, which would mean that ISO amplification happens after the signal leaves the photosite. But this is rapidly getting far beyond my level of electronics expertise. Some input from experts would help.

Eric?
I know you have an
equation that makes it work for the in-between ISOs, but you can make
an equation to fit any curve.
Yes, but it is harder to get a highly accurate fit to 13 or 16 data points using three parameters; moreover, there is a sound theoretical underpinning to the functional form of the fit.
I consider the practicalities, and I
can not imagine any design scenario where Canon would introduce
1/3-stop ISOs through variable gain at a stage later than where it
does the K*(2^N) gains ... why not do them there, too, and get
consistently smooth ISO vs read noise curves? It just doesn't make
any sense to me.
Well, I find it puzzling too. Perhaps it's a legacy design, where intermediate ISO's were added as an afterthought. Nikon, designing from the ground up, has no glitches in its read noise vs ISO behavior.
Also, there is the issue that line noises are
greatest, relative to absolute signal at base ISOs in Canons. That
means that they have a difference that should be occurring on the
sensor - more difficulty black-leveling each line when there is less
gain. I don't think any of the later stages would have any issues
that relate to individual lines; individual lines distinguish
themselves only on the sensor, I would think.
Whether line noise is more or less apparent at low or high ISO would depend on where in the signal chain they get their biggest contribution. If they are biggest at base ISO, the pre/post-amplification noise model suggests that they are being predominantly introduced by the VGA/ADC part of the pipeline, post-amplification. Why can't these components have RF noises at some characteristic temporal frequency, that would translate as the pixels are processed sequentially into linear streaks in the datastream of pixel values? But note, as I said, I have little idea how the circuitry actually works. One can imagine lots of scenarios. Some input from experts would help.

Eric?

--
emil
--



http://theory.uchicago.edu/~ejm/pix/20d/
 
I asked this in another thread, but I realized it filled up with my post:
Can you please post a link to the analysis showing the advantage of
small pixels? Was the measurement done at maximum ISO gain? I think
John Sheehy did some measurements but I don't have a link to them.
I don't have a link either, but some sample pixel read noises at base
ISO:

Canon 1mk2 and mk3 series, D3 - 1.25 to 1.35 ADU in 12-bit normalization

Canon 10D, 20D, 30D, 5D - 1.9 to 2.1 ADU (12-bit)

D2X and CCD Nikons - 2.0 to 4.0 ADU

6MP Fuji P&S sensor - 3.2 ADU

10MP Panasonic FZ50 sensor - 2.8 ADU

12MP Canon G9 - 4.0 ADU

So, you can see that the correlation between pixel density and pixel
read noise is very weak, and the addition of smaller pixels in
quadrature (either mathematically, or visually) yields lower read
noise, relative to maximum signal. On top of that, the quantum
efficiencies are generally almost a stop better on the P&S cameras,
so the base ISOs are really up to double what the cameras say, by
DSLR standards. Therefore, DSLR sensors with no high-ISO
optimization (like the D2X and most CCD sensors) give far more read
noise on an area basis than something like the FZ50 pixels, even at
ISO 1600 and any pushes beyond.
Do you have the corresponding figures for ISO 800 or 1600? That may be a more telling figure as far as the sensor capabilities are concerned. Low ISO read noise mostly tells you about the VGA/ADC noise, according to the model, while it's high ISO read noise that is governed by pixel properties.
--
emil
--



http://theory.uchicago.edu/~ejm/pix/20d/
 
Can you please post a link to the analysis showing the advantage of
small pixels? Was the measurement done at maximum ISO gain? I think
John Sheehy did some measurements but I don't have a link to them.
I don't have a link either, but some sample pixel read noises at base
ISO:

Canon 1mk2 and mk3 series, D3 - 1.25 to 1.35 ADU in 12-bit normalization

Canon 10D, 20D, 30D, 5D - 1.9 to 2.1 ADU (12-bit)

D2X and CCD Nikons - 2.0 to 4.0 ADU

6MP Fuji P&S sensor - 3.2 ADU

10MP Panasonic FZ50 sensor - 2.8 ADU

12MP Canon G9 - 4.0 ADU
Do you have the corresponding figures for ISO 800 or 1600? That may
be a more telling figure as far as the sensor capabilities are
concerned. Low ISO read noise mostly tells you about the VGA/ADC
noise, according to the model, while it's high ISO read noise that is
governed by pixel properties.
There are two trends; the CCD and nMOS compact sensors and the older CCD Sony DSLR sensors all have about 15x to 16x the read noise of ISO 100 at ISO 1600, and the D3 and the Canon DSLRs generally have 2.25 to 4x as much read noise at 1600 vs 100. The K20D and the 450D compress the difference even further, less than 2x IIRC (but that's because of bad base ISO read noise).

--
John

 
I think the question I have and have had each time CMOS vs CCD
discussions come up is: are the advances in CMOS technology you are
talking about above able to compensate for the inherent difference in
well depth of I think 2 to 1 of the CCD over CMOS in signal to noise.
When you look at images from cameras with pixels of the same pitch,
the noise is discernably larger in the CMOS sensor cameras over the
CCD sensor cameras. There are some clear advantages of CMOS sensors
in that it can use an electronic shutter thus avoiding rolling
shutter time exposure in very high shutter speed, but the noise issue
is unclear to me.
As to well depth, if there were differences of two to one of electron well depth of same photosite density sensors for CCD's over CMOS in the past, there aren't such differences now. For instance the CCD 10 MP APS-C sensor as in the Pentax K10D and the Nikon D80 has about 32,000 electron well cacity at ISO 100 where as the (slightly smaller) 10 MP Canon 40D has over 40,000 electron well capacity at the same ISO 100. The Pentax K20D does even better considering its 14 MP on an APS-C format at something over 35,000 electron well capacity.

As to sensor read noise, again the CMOS sensors typically have half the read noise of the equivalent CCD designs.

However, as others have pointed out, there are other contributions to read noise from other circuitry such as amplifiers and convertor circuits that can confuse the sensor comparisons.

Even discounting those (ie finding cameras where these contributions are the same and/or negligible), one must be careful is drawing broad conclusions from comparisons that "CMOS noise is greater than CCD noise" as there are so many variables in how the images were processed and sharpened. The best comparisons are when both images were shot in identical conditions and exposures and processed from raw with identical conversion parameters.

Regards, GordonBGood
 
I think the question I have and have had each time CMOS vs CCD
discussions come up is: are the advances in CMOS technology you are
talking about above able to compensate for the inherent difference in
well depth of I think 2 to 1 of the CCD over CMOS in signal to noise.
When you look at images from cameras with pixels of the same pitch,
the noise is discernably larger in the CMOS sensor cameras over the
CCD sensor cameras. There are some clear advantages of CMOS sensors
in that it can use an electronic shutter thus avoiding rolling
shutter time exposure in very high shutter speed, but the noise issue
is unclear to me.
As to well depth, if there were differences of two to one of electron
well depth of same photosite density sensors for CCD's over CMOS in
the past, there aren't such differences now. For instance the CCD 10
MP APS-C sensor as in the Pentax K10D and the Nikon D80 has about
32,000 electron well cacity at ISO 100 where as the (slightly
smaller) 10 MP Canon 40D has over 40,000 electron well capacity at
the same ISO 100. The Pentax K20D does even better considering its
14 MP on an APS-C format at something over 35,000 electron well
capacity.

As to sensor read noise, again the CMOS sensors typically have
half the read noise of the equivalent CCD designs.

However, as others have pointed out, there are other contributions to
read noise from other circuitry such as amplifiers and convertor
circuits that can confuse the sensor comparisons.

Even discounting those (ie finding cameras where these contributions
are the same and/or negligible), one must be careful is drawing broad
conclusions from comparisons that "CMOS noise is greater than CCD
noise" as there are so many variables in how the images were
processed and sharpened. The best comparisons are when both images
were shot in identical conditions and exposures and processed from
raw with identical conversion parameters.

Regards, GordonBGood
I suspect (but haven't bothered to find out because I'm lazy ;0) ) that the difference may still exist if we were to compare full frame CCDs rather than their interline counterparts.

Granted the issue becomes a bit academic because they tend not to be used much outside of scientific cameras but for absolute highest image quality, the advantage tends to remain with CCDs. If you're not bothered about lengthy readout times, some of these chips quote read noise levels as low as 1-3e with very large well sizes and high QE (> 90%) for back thinned devices.
 
The new kodak sensor is using 'truesense' technology on a 50MP CCD sensor which flips the pixel upside down to allow a 'bottom up' reception of more light into the well. 6 micron. Wonder how that is going to compare with straight noise readouts. Possible that Phil or another on this site will be able to get a loaner to review?
Will
 
The new kodak sensor is using 'truesense' technology on a 50MP CCD
sensor which flips the pixel upside down to allow a 'bottom up'
reception of more light into the well.
TrueSense (tm) is not back illuminated, it's hole polarity.

--
Seen in a fortune cookie:
Fear is the darkroom where negatives are developed
 
so, i have another reason to use "not almost all" DSLR at work, than sensor type in them.

aside from firt reason to this choice - picture quality, pre-defined(among other things)by sensor type.
 

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