What about 1DMkIII's Dynamic Range?

Where did you find the blackframe read noise value? Are you sure
that it is read noise and not the read level (the noise being the
square root of the number of detections)? If the 1DII does have
1.26 bits RMS of read noise at ISO 100 the addition of the A-D
converter noise (Q/sqrt(12) RMS for a step size of Q) would yield
sqrt(1.26^2+1/12) or 1.293 RMS as the system noise. Increasing the
ISO setting to 400 would only make a negligible change of noise
level from 1.293 to 1.268 but a much larger change in low light
sensitivity is observed.
There are two samples from the mkIII on the Imaging Resource website. They contain the black-pixel borders if you load them into the current version of IRIS (www.astrosurf.com/buil). Future versions of the program will most likely crop them away.

--
John

 
Thanks, that should be the black level then not the RMS noise which by Poisson statistics is the square root of the number of particles detected as Peter Carmichael explained. See Peter's first post for a good explanation of the system DR issue.
 
No text.
 
By my reckoning, the improvement in shadows from ISO 100 to 400 is
dramatic. This two stop variance in ISO setting would be available
to a single shot with 14 bit conversion. The sensor has had this
capability for a generation already; extra bits at the D/A stage
are now making it possible to access this capability in
post-processing of a single shot.

So. I would assert that 14 bit raw has the potential to add DR
capability. If the full well depth of the 1DmkIII is still of the
same order of magnitude as the 5D and 1DmkII, then the 14 bits will
result in greater DR. The need to swing ISO to access this DR will
reduce. The exact DR will depend critically on exposure.
I agree entirely and I said so a few weeks ago (of course you have
added the full science behind the explanation). Even if the
technical DR has not changed, if you are gaining much less noise in
the shadows and have more tonal values at hand is not the effective
DR improved. It must be by definition IMO. You can now go 1-2 stops
further below middle tone and have the same shadow detail as the
old camera.

Maybe the issue is that the improvements only come at the shadow
end of the range; highlight DR is not affected; the wells are the
same size and cannot hold more charge than before.
But if you have the extra 1-2 stops DR in the shadows can't you "underexpose" by 1-2 stops without sacrificing shadow noise? Thus you will gain 1-2 stops in the highlights without getting any worse shadow noise.

--
Ed Richer
 
But if you have the extra 1-2 stops DR in the shadows can't you
"underexpose" by 1-2 stops without sacrificing shadow noise? Thus
you will gain 1-2 stops in the highlights without getting any worse
shadow noise.
Yes. Dynamic range at capture (i.e. linear values digitized into a raw file) is agnostic of the intended exposure. Mid-gray has no inherent meaning in terms of captured and counted electrons. The downstream processing subsequently produces an output file in a generic colorspace, where mid-gray has a meaning.

In an 8 bit sRGB output file, mid-gray is 117,117,117 with the file allowing 2.5 stops of highlight range. If there are more extended highlights captured and if the photographer wants that highlight information represented in the output file, then the post-processing tone curve must compress any captured highlights into the 2.5 stop headroom available in the colorspace. This is the same whether the camera is a P&S, a Nikon, a Canon or a Fuji S5.
 
DR and noise go hand in hand. Noise is dominated by photon
counting statistics (Poisson's law). The best way to save your
shadows from disappearing into noise is to capture more photons.
That helps, but if there is a lot of read noise, photon shot noise is the least of your problems in the deep shadows. Read noise is the dominant noise at some point in the shadows, and below. The point where read noise dominates is higher in sensor wells with high capacity.

At any given tonal level, the total noise (as measured in electrons or photons) is approximately equal to the square root of the sum of the read noise squared, and the number of photons captured (all in units of electrons).

Most DSLRs are limited in DR at ISO 100 by read noise; collecting more photons will only make the noise in the midtones and highlights slightly better, but they have nothing to do with DR, per se.
This gives you grief with the highlights blowing out, hence the
need for a large full well depth.

The raw capture is digitized as a linear count of the charge
accumulated in each photosite. This is proportional to the number
of electrons stored. The number of electrons stored is
proportional to the number of incident (and captured) photons.

Because the raw capture is a linear count directly related to
incident photons, the dynamic range of the captured image can be
limited by having too few bits available to digitize the available
signal information. 14 bits stores two more stops of sensor data
than 12 bits. Fact. Not fiction. That's just how it is.

In the least significant bits, quantization errors add noise. With
bigger signals the digitization noise is insignificant compared to
the inherent photon noise in the signal. At each signal level,
there is a determinable photon shot signal to noise ratio. There
is a measurable camera/digitization noise floor. There is a
cut-off point at low signal levels after which the camera's readout
noise swamps the signal.

The sensors in the last generation of big pixel Canon dSLRs (1DmkII
and 5D) have large full well capacity at ~ 80000 electrons. If
you are utilising the full well depth (ISO 100 typically for 5D and
a bit less for the 1DmkII ref. PIXSurgeon), then the least
significant bit of a 12bit RAW file reflects the charge of 20
electrons. This lowest level of information is subject to dither
(intentionally added digital noise) to avoid artifacts. The photon
shot noise at 20 electrons signal is equivalent to a bit less than
5 electrons. In other words, the digitization itself is
introducing worse noise than the noise inherent in the original
signal. Having 1 or 2 more bits available to the D/A conversion
would add useful dynamic range in the capture.


I assert that 12 bit D/A holds back the 5D and the 1DmkII. I have
an experiment that shows this.

This sensor-native DR capability on previous generation cameras is
made available by use of the ISO setting, which alters the analogue
amplification of the output signal. I have taken an "HDR" set of
images with altered ISO setting (100,400,1600), but constant Tv and
Av. I have an example HDR image here:
http://www.seeminglyabsent.co.uk/2007_03_18_hdr/htmls/0000.html
(Gallery of all shots is here:
http://www.seeminglyabsent.co.uk/2007_03_18/htmls/IMG_8766.html

I have equalized the three contributing shots for brightness in
post-processing, but look at the shadow noise in the dark window
reflection and the highlights on the tiles on the right (gallery
for shadows is here:
http://www.seeminglyabsent.co.uk/2007_03_18_shadows/htmls/0000.html
; gallery for highlights is here:
http://www.seeminglyabsent.co.uk/2007_03_18_highlights/htmls/0003.html )

Crops for shadows (ISO 100 -> 400 -> 1600)







Crops for highlights (ISO 100 -> 400 -> 1600)







By my reckoning, the improvement in shadows from ISO 100 to 400 is
dramatic. This two stop variance in ISO setting would be available
to a single shot with 14 bit conversion. The sensor has had this
capability for a generation already; extra bits at the D/A stage
are now making it possible to access this capability in
post-processing of a single shot.

So. I would assert that 14 bit raw has the potential to add DR
capability. If the full well depth of the 1DmkIII is still of the
same order of magnitude as the 5D and 1DmkII, then the 14 bits will
result in greater DR. The need to swing ISO to access this DR will
reduce. The exact DR will depend critically on exposure.
--
John

 
...I read the whole thing, and I will provide some specific feedback/questions later, tonight, when I get some time for it... :-)

--

TIP: If you do not like this post, simply press the 'COMPLAINT' button. Mommy/Daddy are just one click away.
 
I assert that 12 bit D/A holds back the 5D and the 1DmkII. I have
an experiment that shows this.
That's what I concluded a couple of years ago after doing similar experiments, however, I now have a completely different conclusion.
By my reckoning, the improvement in shadows from ISO 100 to 400 is
dramatic. This two stop variance in ISO setting would be available
to a single shot with 14 bit conversion.
That does not really follow; your experiment (and the ones I did with my 20D) show clearly that there are small-signal details in the sensor wells that are not captured well in the RAW files at ISO 100. However, more bit depth will not really help, because it isn't the problem. The problem is analog read noise. Most of the read noise in the ISO 100 shadows occurs somewhere between the on-pixel amplification, and the digitization in the ADC. The characteristic of the noise floor is not quantization noise; it is horizontal and vertical banding, mixed with 2-D random noise. The standard deviation of ISO 100 blackframes from current Canons range between 1.26 ADUs and 2.07 ADUs. Even with trace amounts of analog noise, quantization noise will not give a standard deviation of more than about 0.2 or 0.3. There are ways to prove that the noise is not mainly quantization; when I did my tests like yours, I did everything in the RAW state, without any converters per se, and had the opportunity to do simple arithmetic on the RAW data. I took two identical photos, one at ISO 100, and one at ISO 1600, both under-exposed so that they were actually pushes to ISO 10,000. Both had the same manual exposure, same Av and Tv values, but the ISOs differed. In the ISO 100, 20 RAW levels represented the full DR in the push, and in the ISO 1600, 320 levels did (a factor of 16, as you would expect). The ISO 100, as you would guess, is much noisier. To determine if it was quantization, I quantized the ISO 1600 to only 20 levels also by dividing the RAW values by 16, and then using 20 RAW values also for the full push. The result was shocking (at the time; logical to me now); the quantized ISO 1600 looked almost indistinguishable from the non-quantized 1600, and still far better than the ISO 100. Conclusion: bit depth is not a/the problem; analog read noise is.
So. I would assert that 14 bit raw has the potential to add DR
capability. If the full well depth of the 1DmkIII is still of the
same order of magnitude as the 5D and 1DmkII, then the 14 bits will
result in greater DR.
Unfortunately, the noise and DR of a pixel in a mkIII is exactly the same as the mkII, at least at ISO 100. The 2 extra bits made the read noise quadruple in ADUs, and not much else. For all intents and purposes, those extra two bits are just a waste of CF storage. Unless, of course, with these extra two bits comes a reduction of banding noise (especially at high ISOs). I haven't had a chance to examine high-ISO RAWs from the mkIII, only ISO 100.

All things considered, I get the impression that one of the biggest technological obstacles is reading a large photon count accurately, in a short period of time, and Canon has not conquered this problem at all between the mkII and the mkIII.

--
John

 
Thanks, that should be the black level then not the RMS noise which
by Poisson statistics is the square root of the number of particles
detected as Peter Carmichael explained. See Peter's first post for
a good explanation of the system DR issue.
There really isn't that much room for improvement in "shot noise". It's not a contamination of the actual scene; shot noise is what is really there in the real world light; we only call it noise because we don't like to see it. In real life, shot noise is buffered from the user by the brain. When photons are rarely striking individual rods and cones on your retina, your brain maintains a semi-fabricated "noise-reduced" image that is only changed locally as new samples are integrated. In a photograph; our brains take shot noise literally, as part of the texture of the medium, not as a quality of light, so it is not buffered from our perception.

Quantum efficiency can only get so good; sensors can only get so big and still be practical; read noise can still improve drastically, and is most of the noise in the deepest shadows, especially in cameras that collect a lot of light.

--
John

 
"DR and noise go hand in hand" is true when we think how far the DR
extend to dark shades. But its possible also to improve the dynamic
range in how far you get usable shades in high-lights - today this
is about 3.5-4 stops over the mid-gray.
That's only a semantic, relativistic issue, though. The bottom line is that the RAW data at any given ISO clips at a certain level, and a signal with what you consider the "lowest usable S/N ratio" lies a certain number of stops below that point; that is all that determines dynamic range. It is irrelevant and arbitrary where the middle-grey point is; it is only a frame of reference for metering.

The same sensor with the same amplification could have an ISO 100 with 4 stops of highlights above middle grey, or it can be considered ISO 200 with 5 stops, or ISO 50 with 3 stops.

--
John

 
..I only understand about one word in three of the debate between you and Peter, but most firms are keen to claim any increase if they have managed one! ;-)
--
Regards,
DaveMart

'Just a wildebeest on the plain of life'
Please see profile for equipment
 
I previously posted to this thread trying to briefly say what you
have summarized much more clearly in your post (I guess I should
have read it before posting myself). One item is that you have
neglected is the pre-amplifier noise. That noise is normally
reported in RMS terms and I have seen reports that it is less than
the 5 e- RMS equivalent that you list for the Poisson noise so the
combination would be 7 e- or less which would still be much less
than the 20 e- step size.
5 is in the range of the best cases. Canon DSLRs generally have only about 3 to 6 electrons of read noise at the highest ISO, and A small ZLR like my FZ50 has a read noise of 2.7 electrons at ISO 100 (similar photon count, btw). At ISO 100, and 50, however, read noises on Canon DSLRs can be as high as 36 electrons. My FZ50 rises to 3.34 electrons at ISO 1600, in the opposite direction than the Canon DSLRs; the Canons are optimal at high ISOs, and the FZ50 is optimal at ISO 100 (because the ISO-gain amplifier is basically garbage in the FZ50; pushing gives better results).

--
John

 
..I only understand about one word in three of the debate between
you and Peter,
But I'm up on what the meaning of "is" is,...and I'm right on top of those "and"'s and "the"'s.

I read those things sustained by hope for a layman-decipherable conclusion. ;-)

Larry
 
That's what I concluded a couple of years ago after doing similar
experiments, however, I now have a completely different conclusion.
I know it's always easy to be most influenced by whomever has spoken last, ...but my bottom line of the moment "take" on the Peter/Pix/John input is that the 1DIII has no appreciable "new" DR advantage.

Thanks to all you contributing geeks! :-)

Larry
 
I can't say I followed everything you guys are discussing here, but I did follow enough...

Maybe in this context could you explain what Canon is doing in Highlight-priority mode. It sounded pretty exiting when I first read about it, as I assumed they were referring to a DR improvement in highlights. But then I read their white paper and quickly realized that noise is increased in the shadows in this mode.

So what the heck are they doing? Are they just massaging the digital file in some way or are they in fact reading the sensor differently? Is the result just more meaningful stops aboiv 18% grey...at the expense of less below?
 
5 is in the range of the best cases. Canon DSLRs generally have
only about 3 to 6 electrons of read noise at the highest ISO, and A
small ZLR like my FZ50 has a read noise of 2.7 electrons at ISO 100
(similar photon count, btw). At ISO 100, and 50, however, read
noises on Canon DSLRs can be as high as 36 electrons. My FZ50
rises to 3.34 electrons at ISO 1600, in the opposite direction than
the Canon DSLRs; the Canons are optimal at high ISOs, and the FZ50
is optimal at ISO 100 (because the ISO-gain amplifier is basically
garbage in the FZ50; pushing gives better results).
Can we just be clear that the 36 electrons equivalent readout noise at ISO 100 (say) for a current Canon big pixel 12 bit capture is dominated by quantization noise.

Change the frame of reference.

Describe the same noise in terms of volts, or in terms of bits (digitization of voltages across the A/D input) and it is very clear that noise levels are low at low ISO and high at high ISO. We know this. The noise is confined to the lowest two bits of the raw data on Canon dSLRs until you go beyond "unity ISO" (1600 on the 5D). When you set ISO to lower values, the signal passed from the sensor to the A/D converter is less amplified and each level represented in the digitized output describes a larger count of electrons. The least significant bits of the signal, which are noisy, have high electron equivalence numbers.

"Readout noise" is a terminology for all the noise that isn't photon shot noise (or thermal noise in long exposures). There is no magic way to intervcene and take measurements from the sensor any more accurately than the built in D/A converter. Readout noise is apparent only in the digitized numbers output by the A/D converter and recorded in the raw file and is subject to quantization effects. Quantization noise described in e- terms terms is exactly the quantity that gets divided by a factor when you add bit-depth to your A/D conversion.

If you add 2 bits to your A/D conversion and you add headroom to your analogue amplifcation and you manage not to introduce more noise in the design of the amplifier, then the e- readout noise equivalence drops by close to a factor of 4 for an equivalent full range signal. You digitize more of the sensor's output in one go. It is non-trivial to design such an improved amplification stage and compromise assures that the theoretical factor of four is not achievable, but some improvement will be achieved.

Sensors have been held back by 12 bit A/D conversion. 14 bit is an improvement.
 
I know it's always easy to be most influenced by whomever has
spoken last, ...but my bottom line of the moment "take" on the
Peter/Pix/John input is that the 1DIII has no appreciable "new" DR
advantage.
I think the greatest insight will come from real photographers in real shooting situations, learning the new capabilities of new equipment.

I don't have a 1DmkIII in my hands. My comments are very specific in saying that results will be "implementation dependent". If there is no new capability, then Canon's R&D budget should forthwith be handed over to the marketing department. You've got to hope...
 
I thought ( I know, what with!) that it only applied to JPEG images, effectively putting in a curve?
Maybe in this context could you explain what Canon is doing in
Highlight-priority mode.
Expose to the ... left, with greater sensor + readout DR allowing
the latitude.
--
Regards,
DaveMart

'Just a wildebeest on the plain of life'
Please see profile for equipment
 
Quantization noise described in e- terms
terms is exactly the quantity that gets divided by a factor when
you add bit-depth to your A/D conversion...
...while other components of readout noise will not change magnitude and will be seen as more dominating components in the overall lowered noise level.
 

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