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What compact digicam has the biggest CCD pixels?

Forum Digital Cameras : General Discussion What compact digicam has the biggest CCD pixels?

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Pixel size = CCD size in square microns, divided by total number of pixels.

Nikon D70: CCD = 15 x 22 mm = 330 million sq. microns, divided by 6 MP =
about 50 square microns per pixel, pretty good.

Random compact point and shoot: CCD = 6 x 8 mm = 48 million sq. microns,
divided by 4 mp = 12 square microns per pixel, much noisier.

What I want is a compact P/S with a good 6x8 mm sensor and about 1 MP
-- do they still make those?

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You could get lucky, but I'd say that marketing has dictated that
manufacturers need to cram in as many megapixels as possible in order
to be attractive. Ask any consumer salesperson how to improve image
quality and the answer is inevitably going to be "get the model with
more megapixels." A newly released 1 megapixel compact would
effectively be considered obsolete...

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Paul Rubin wrote:
> Pixel size = CCD size in square microns, divided by total number of pixels.
>
> Nikon D70: CCD = 15 x 22 mm = 330 million sq. microns, divided by 6 MP =
> about 50 square microns per pixel, pretty good.
>
> Random compact point and shoot: CCD = 6 x 8 mm = 48 million sq. microns,
> divided by 4 mp = 12 square microns per pixel, much noisier.
>
> What I want is a compact P/S with a good 6x8 mm sensor and about 1 MP
> -- do they still make those?


The Olympus C3030 has a "half inch" sensor 4:3 ratio (12.7x9.5mm?)
sensor with effective 3.14MP. It cost $800 in the year 2000.

120sq mm (120 million sq. microns?)/3.14MP = 38 square microns per pixel.

It does show purple fringing in backlit trees pretty bad and banding
with long night exposures but with a decent f/2.8 lens it does pretty
well in most lighting. ISO 100 to 400. I can say that when I got a D70
after this I was amazed how much information I could pull out of shadows
compared to the Oly 3030. I haven't compared other P&S's to it.


googlegroups@sensation.net.au wrote:

> You could get lucky, but I'd say that marketing has dictated that
> manufacturers need to cram in as many megapixels as possible in order
> to be attractive. Ask any consumer salesperson how to improve image
> quality and the answer is inevitably going to be "get the model with
> more megapixels." A newly released 1 megapixel compact would
> effectively be considered obsolete...


True but there must be some significant variation in the ratio for
different models. I've not seen such a chart comparing square microns
pixel size (12 to 50+).

Here's the closest I've seen:
http://homepages.ihug.com.au/~pars [...] sors1.html
Unfortunately they don't tell megapixels.

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paul <paul@not.net> writes:
> The Olympus C3030 has a "half inch" sensor 4:3 ratio (12.7x9.5mm?)
> sensor with effective 3.14MP. It cost $800 in the year 2000.

Nah, that "half inch" has somewhat less sensor area than that, like
half that amount. "Half inch" refers to the diameter of vidicon tube
from the tube era that would have had a similar amount of active
imaging area. Good point about the old Olympus though.

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Paul Rubin wrote:

> paul <paul@not.net> writes:
>
>>The Olympus C3030 has a "half inch" sensor 4:3 ratio (12.7x9.5mm?)
>>sensor with effective 3.14MP. It cost $800 in the year 2000.
>
>
> Nah, that "half inch" has somewhat less sensor area than that, like
> half that amount. "Half inch" refers to the diameter of vidicon tube
> from the tube era that would have had a similar amount of active
> imaging area. Good point about the old Olympus though.


ehhh that's why I put it in quotes <grin>.
I don't know, I'd like to see a chart.

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paul <paul@not.net> writes:
> > Nah, that "half inch" has somewhat less sensor area than that, like
> > half that amount. "Half inch" refers to the diameter of vidicon tube
> > from the tube era that would have had a similar amount of active
> > imaging area. Good point about the old Olympus though.
>
> ehhh that's why I put it in quotes <grin>.
> I don't know, I'd like to see a chart.

All you need to do is ask:

http://www.dpreview.com/learn/?/key=Sensor_Sizes

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Paul Rubin wrote:

> paul <paul@not.net> writes:
>
>>The Olympus C3030 has a "half inch" sensor 4:3 ratio (12.7x9.5mm?)
>>sensor with effective 3.14MP. It cost $800 in the year 2000.
>
>
> Nah, that "half inch" has somewhat less sensor area than that, like
> half that amount. "Half inch" refers to the diameter of vidicon tube
> from the tube era that would have had a similar amount of active
> imaging area. Good point about the old Olympus though.


So what does it mean when they state a sensor's size as
"1/1.8-inch CCD" ?

Reply to Paul

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In article <7x1x9334dj.fsf_-_@ruckus.brouhaha.com>,
Paul Rubin <http://phr.cx@NOSPAM.invalid> wrote:

> Pixel size = CCD size in square microns, divided by total number of pixels.
>
> Nikon D70: CCD = 15 x 22 mm = 330 million sq. microns, divided by 6 MP =
> about 50 square microns per pixel, pretty good.
>
> Random compact point and shoot: CCD = 6 x 8 mm = 48 million sq. microns,
> divided by 4 mp = 12 square microns per pixel, much noisier.
>
> What I want is a compact P/S with a good 6x8 mm sensor and about 1 MP
> -- do they still make those?

Forget about the theoretical math. Sensors aren't that good yet.
Factors like production quality, chip design, manufacturing process, and
image processing still dominate the image quality. Read the reviews,
check out some sample pictures, and then try some out.

Your specifications of a good 1MP camera is contradictory. The lack of
resolution would ruin many photos.

Reply to Anonymous

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Kevin McMurtrie <mcmurtri@dslextreme.com> writes:
> Your specifications of a good 1MP camera is contradictory. The lack of
> resolution would ruin many photos.

I don't believe that; for pictorial photos, megapixels are way
overrated. The 2.7MP Nikon D1 still makes better photos than any
compact 5 or 8 megapixel camera. I woke up to megapixel hype when I
saw a 16x20" or so poster print that someone was carrying around in
the street. From 5 feet away it looked great. From up close it
looked soft, but I thought that was because of the printer. I asked
what kind of camera it had been taken with. The answer was it had
been taken with a 320x240 web cam. For a while my only digicam was an
0.75 MP Canon A5 and I felt the photos it took were fine. (It helps
that I don't care about prints very much, and mainly want to view on
screen).

1MP sensors are capable of making 8x10" prints that look as good as
decent 35mm prints (use bicubic interpolation yada yada). The 6.2MP
D70 gets sort of acceptable noise performance for low light shooting
at 1600 ISO. Let's see if this makes sense: the D70 throws away two
thirds of the incoming photons in the RGB filters in front of the
sensor, so a monochrome version could do 4800 ISO. Now lower the
resolution to 1MP (6x the sensor area per pixel) and you're up to
30,000 ISO. With a fast lens (I have a 30 year old 35/1.4 MF Nikkor
that was $200 on Ebay a couple years ago and is now probably worth
almost zilch) you should be able to get good printable monochrome
shots with no flash even in the worst indoor lighting like dimly lit
bars. That's the total fix to red-eye ;-).

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Paul Rubin wrote:

> paul <paul@not.net> writes:
>
>>>Nah, that "half inch" has somewhat less sensor area than that, like
>>>half that amount. "Half inch" refers to the diameter of vidicon tube
>>>from the tube era that would have had a similar amount of active
>>>imaging area. Good point about the old Olympus though.
>>
>>ehhh that's why I put it in quotes <grin>.
>>I don't know, I'd like to see a chart.
>
>
> All you need to do is ask:
>
> http://www.dpreview.com/learn/?/key=Sensor_Sizes


OK so the Oly 1/1.8-inch CCD=
7.15x5.32mm = 38sq mm (38 million sq. microns)
/3.14MP = 12 square microns per pixel.

The examples on that page come out to 6.4 to 7.6sq microns/px so that's
pretty good but not the 60-76sq microns/px of a DSLR.

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Paul Rubin wrote:
>
> ....you should be able to get good printable monochrome
> shots with no flash even in the worst indoor lighting like dimly lit
> bars. That's the total fix to red-eye ;-).


Downsample an underexposed/corrected 6MP image to 1MP in that lighting
and it might look good?

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Paul Rubin wrote:
> Pixel size = CCD size in square microns, divided by total number of
> pixels.
>
> Nikon D70: CCD = 15 x 22 mm = 330 million sq. microns, divided by 6
> MP = about 50 square microns per pixel, pretty good.
>
> Random compact point and shoot: CCD = 6 x 8 mm = 48 million sq.
> microns, divided by 4 mp = 12 square microns per pixel, much noisier.
>
> What I want is a compact P/S with a good 6x8 mm sensor and about 1 MP
> -- do they still make those?

You may be asking the wrong question. Sensor size itself may be more
important than pixel size, as you can downsample to reduce the number of
pixels. Bigger sensors can capture more photons, and produce a better
signal-to-noise ratio. However, as the pixels get smaller, they fraction
of their area which captures light may decrease.

Given all of the above, the 2/3 inch sensor (8.8 x 6.6mm) is perhaps the
largest compact camera sensor, and can be found in the Nikon 5700 (5MP)
and Nikon 8400 and 880 (8MP) cameras.

Cheers,
David

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[A complimentary Cc of this posting was sent to
Paul Rubin
<http://phr.cx@NOSPAM.invalid>], who wrote in article <7x1x9334dj.fsf_-_@ruckus.brouhaha.com>:
> Pixel size = CCD size in square microns, divided by total number of pixels.
>
> Nikon D70: CCD = 15 x 22 mm = 330 million sq. microns, divided by 6 MP =
> about 50 square microns per pixel, pretty good.
>
> Random compact point and shoot: CCD = 6 x 8 mm = 48 million sq. microns,
> divided by 4 mp = 12 square microns per pixel, much noisier.

> What I want is a compact P/S with a good 6x8 mm sensor and about 1 MP
> -- do they still make those?

What for? To save space on your flash card? Do not be ridiculous.

Given an 8MP camera and 1MP camera with the same sensor size, the same
percentage of area which is photo-sensitive, and the same QE, the 8MP
image contains *strictly* more information than 1MP camera. If you
want to extract the 1MP information from 8MP image, just average over
8 cells.

Hope this helps,
Ilya

P.S. Of course, it may be that 8MP camera has slightly lower
percentage of photo-sensitive area (due to non-0 amount of "additional
circuitry" ). However, the cameras of '05 should have higher QE than
those of '00.

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paul <paul@not.net> writes:
> > ....you should be able to get good printable monochrome
> > shots with no flash even in the worst indoor lighting like dimly lit
> > bars. That's the total fix to red-eye ;-).
>
> Downsample an underexposed/corrected 6MP image to 1MP in that lighting
> and it might look good?

I've been wondering about that and I think some improvement might
result, but you don't get the whole factor of six. For example,
almost all consumer video cameras these days have megapixel sensors so
they can double as still cameras. As a result, they have worse low
light performance at normal video resolution (720x480) than the
previous generation of camcorders which only had video resolution
sensors.

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Ilya Zakharevich <nospam-abuse@ilyaz.org> writes:
> Given an 8MP camera and 1MP camera with the same sensor size, the same
> percentage of area which is photo-sensitive, and the same QE, the 8MP
> image contains *strictly* more information than 1MP camera. If you
> want to extract the 1MP information from 8MP image, just average over
> 8 cells.

Given what I see happening in video camcorders (low light performance
at (fixed) video resolution gets worse and worse as they increase the
number of pixels on the ccd), I don't think that averaging approach
works as well as it might sound.

> P.S. Of course, it may be that 8MP camera has slightly lower
> percentage of photo-sensitive area (due to non-0 amount of "additional
> circuitry" ). However, the cameras of '05 should have higher QE than
> those of '00.

Obviously then the answer is a camera made in '05 that still has nice
big pixels.

The other thing missing is a monochrome digicam less exotic than the
Kodak DCS-660M.

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David J Taylor wrote:
> Paul Rubin wrote:
>
>>Pixel size = CCD size in square microns, divided by total number of
>>pixels.
>>
>>Nikon D70: CCD = 15 x 22 mm = 330 million sq. microns, divided by 6
>>MP = about 50 square microns per pixel, pretty good.
>>
>>Random compact point and shoot: CCD = 6 x 8 mm = 48 million sq.
>>microns, divided by 4 mp = 12 square microns per pixel, much noisier.
>>
>>What I want is a compact P/S with a good 6x8 mm sensor and about 1 MP
>>-- do they still make those?
>
>
> You may be asking the wrong question. Sensor size itself may be more
> important than pixel size, as you can downsample to reduce the number of
> pixels. Bigger sensors can capture more photons, and produce a better
> signal-to-noise ratio. However, as the pixels get smaller, they fraction
> of their area which captures light may decrease.


I'm not sure. I think it's the pixel size that overloads when too small.


>
> Given all of the above, the 2/3 inch sensor (8.8 x 6.6mm) is perhaps the
> largest compact camera sensor, and can be found in the Nikon 5700 (5MP)


OK I started a chart:
<http://www.edgehill.net/1/Misc/photography/sensors/excel/sensor-size.htm>
That shows the Nikon 5700 2/3 @ 5MP as 11.6sq microns/px
It is an excel chart saved as html & can be opened with excel.


> and Nikon 8400 and 880 (8MP) cameras.


7.3sq microns/px

Reply to Paul

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In article <7x3btjuzu0.fsf@ruckus.brouhaha.com>,
Paul Rubin <http://phr.cx@NOSPAM.invalid> wrote:

> Kevin McMurtrie <mcmurtri@dslextreme.com> writes:
> > Your specifications of a good 1MP camera is contradictory. The lack of
> > resolution would ruin many photos.
>
> I don't believe that; for pictorial photos, megapixels are way
> overrated. The 2.7MP Nikon D1 still makes better photos than any
> compact 5 or 8 megapixel camera. I woke up to megapixel hype when I
> saw a 16x20" or so poster print that someone was carrying around in
> the street. From 5 feet away it looked great. From up close it
> looked soft, but I thought that was because of the printer. I asked
> what kind of camera it had been taken with. The answer was it had
> been taken with a 320x240 web cam. For a while my only digicam was an
> 0.75 MP Canon A5 and I felt the photos it took were fine. (It helps
> that I don't care about prints very much, and mainly want to view on
> screen).
>
> 1MP sensors are capable of making 8x10" prints that look as good as
> decent 35mm prints (use bicubic interpolation yada yada). The 6.2MP
> D70 gets sort of acceptable noise performance for low light shooting
> at 1600 ISO. Let's see if this makes sense: the D70 throws away two
> thirds of the incoming photons in the RGB filters in front of the
> sensor, so a monochrome version could do 4800 ISO. Now lower the
> resolution to 1MP (6x the sensor area per pixel) and you're up to
> 30,000 ISO. With a fast lens (I have a 30 year old 35/1.4 MF Nikkor
> that was $200 on Ebay a couple years ago and is now probably worth
> almost zilch) you should be able to get good printable monochrome
> shots with no flash even in the worst indoor lighting like dimly lit
> bars. That's the total fix to red-eye ;-).


Modern cameras like the Canon 20D, 300D, and 350D have far less noise
than lower resolution cameras of not long ago. Like I said before, it's
more about the sensor quality. The older CCD chips grabbed lots of
light but they leaked electricity rapidly, bloomed, and the quality from
pixel to pixel was terrible. My Canon 350D has less noise at ISO 800
than my Oly C2000Z, C3030Z, and C4040Z had at ISO 100. When using the
higher pixel count for noise filtering, the Canon 350D is cleaner at ISO
1600 than the Olys were at ISO 100. CCDs are also prone to overheating.
45 minute exposures with my Canon 350D have less noise than 8 second
exposures from older CCD sensors.

Maybe you want an astronomy grade sensor.

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Kevin McMurtrie <mcmurtri@dslextreme.com> wrote:

[snip]

>CCDs are also prone to overheating.
>45 minute exposures with my Canon 350D have less noise than 8 second
>exposures from older CCD sensors.

You can do 45 minute minute exposures? If so, this means these
cameras are like real film cameras. I have a feeling that next years
bonus and tax refund have just been spoken for.

Heading off to dpreview to read the specs.

Wes

--
Reply to:
Whiskey Echo Sierra Sierra AT Alpha Charlie Echo Golf Romeo Oscar Paul dot Charlie Charlie
Lycos address is a spam trap.

Reply to Clutch

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Kevin McMurtrie wrote:

> Modern cameras like the Canon 20D, 300D, and 350D have far less noise
> than lower resolution cameras of not long ago. Like I said before, it's
> more about the sensor quality. The older CCD chips grabbed lots of
> light but they leaked electricity rapidly, bloomed, and the quality from
> pixel to pixel was terrible. My Canon 350D has less noise at ISO 800
> than my Oly C2000Z, C3030Z, and C4040Z had at ISO 100. When using the
> higher pixel count for noise filtering, the Canon 350D is cleaner at ISO
> 1600 than the Olys were at ISO 100. CCDs are also prone to overheating.
> 45 minute exposures with my Canon 350D have less noise than 8 second
> exposures from older CCD sensors.
>

All newer good quality digital cameras are photon + read noise
limited. Further improvements will be very slight, in the sense
that the only things left to improve are: lower read noise
(will affect shadows, no brighter parts of the image),
quantum efficiency, and higher optical transmission
throughput (total =perhaps a 2x gain here). All this will
help large as well as small sensors, so the large sensor
camera will always produce better images. See:

http://www.clarkvision.com/imagede [...] ize.matter

Roger

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paul wrote:

> Paul Rubin wrote:
>
>> paul <paul@not.net> writes:
>>
>>> The Olympus C3030 has a "half inch" sensor 4:3 ratio (12.7x9.5mm?)
>>> sensor with effective 3.14MP. It cost $800 in the year 2000.
>>
>>
>>
>> Nah, that "half inch" has somewhat less sensor area than that, like
>> half that amount. "Half inch" refers to the diameter of vidicon tube
>> from the tube era that would have had a similar amount of active
>> imaging area. Good point about the old Olympus though.
>
>
>
> So what does it mean when they state a sensor's size as
> "1/1.8-inch CCD" ?

It's a scam to fool you from knowing how small it really
is! See:
http://www.dpreview.com/learn/?/Gl [...] zes_01.htm

Roger

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Paul Rubin wrote:

> Ilya Zakharevich <nospam-abuse@ilyaz.org> writes:
>
>>Given an 8MP camera and 1MP camera with the same sensor size, the same
>>percentage of area which is photo-sensitive, and the same QE, the 8MP
>>image contains *strictly* more information than 1MP camera. If you
>>want to extract the 1MP information from 8MP image, just average over
>>8 cells.
>
>
> Given what I see happening in video camcorders (low light performance
> at (fixed) video resolution gets worse and worse as they increase the
> number of pixels on the ccd), I don't think that averaging approach
> works as well as it might sound.
>
>
>>P.S. Of course, it may be that 8MP camera has slightly lower
>>percentage of photo-sensitive area (due to non-0 amount of "additional
>>circuitry" ). However, the cameras of '05 should have higher QE than
>>those of '00.
>
>
> Obviously then the answer is a camera made in '05 that still has nice
> big pixels.

No. Ilya forgot to include read noise. Read noise is currently
approximately the same for all good sensors, somewhere in
the 7-15 electron range. As your signal gets smaller,
e.g. smaller pixels, or shadow areas, read noise becomes
a larger fraction of the total noise from the sensor.
See:
http://www.clarkvision.com/imagede [...] ize.matter

Note too the diffraction spot diameter: for f/2.8 it is
3.2 microns for blue (4700 angstroms) light, 4.1 microns for
red light (6000 angstroms). Pixels smaller than 4 microns
have images that are diffraction limited (many high megapixel
P&S have smaller pixels than this)! Go to f/5.6, which is what
many zoom lenses are, and your at diffraction spot sizes of
6 to 8 microns. Diffraction and numbers of photons are why
large pixel size sensors produce better images. Simple physics
that will not change unless a major, Major, MAJOR, *MAJOR* rewrite
of fundamental physics happens.

Roger

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Kevin McMurtrie <mcmurtri@dslextreme.com> writes:

> Modern cameras like the Canon 20D, 300D, and 350D have far less
> noise than lower resolution cameras of not long ago. Like I said
> before, it's more about the sensor quality. The older CCD chips
> grabbed lots of light but they leaked electricity rapidly, bloomed,
> and the quality from pixel to pixel was terrible.

Do you have data to back up this claim? If it was as you say, then
they simply would not work at all. Even the tiniest leakage of loss in
readout sends the signal to zero. If you wonder about that, try
calculating 0.999^2000 and see how many 9s you need to get a
reasonable answer.

> My Canon 350D has less noise at ISO 800 than my Oly C2000Z, C3030Z,
> and C4040Z had at ISO 100. When using the higher pixel count for
> noise filtering, the Canon 350D is cleaner at ISO 1600 than the Olys
> were at ISO 100. CCDs are also prone to overheating. 45 minute
> exposures with my Canon 350D have less noise than 8 second exposures
> from older CCD sensors.

How do CCDs get hot? They have no electronicss on the chip, unlike CMOS
chips, and rare static during exposure.

--
Paul Repacholi 1 Crescent Rd.,
+61 (08) 9257-1001 Kalamunda.
West Australia 6076
comp.os.vms,- The Older, Grumpier Slashdot
Raw, Cooked or Well-done, it's all half baked.
EPIC, The Architecture of the future, always has been, always will be.

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prep@prep.synonet.com wrote:
> Kevin McMurtrie <mcmurtri@dslextreme.com> writes:
>

>>CCDs are also prone to overheating. 45 minute
>>exposures with my Canon 350D have less noise than 8 second exposures
>>from older CCD sensors.
>
>
> How do CCDs get hot? They have no electronicss on the chip, unlike CMOS
> chips, and rare static during exposure.



I don't know if it's CCD/CMOS dependent but I heard astronomers cool
their sensors with liquid nitrogen.

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Paul Rubin wrote:

> Pixel size = CCD size in square microns, divided by total number of pixels.
>
> Nikon D70: CCD = 15 x 22 mm = 330 million sq. microns, divided by 6 MP =
> about 50 square microns per pixel, pretty good.
>
> Random compact point and shoot: CCD = 6 x 8 mm = 48 million sq. microns,
> divided by 4 mp = 12 square microns per pixel, much noisier.
>
> What I want is a compact P/S with a good 6x8 mm sensor and about 1 MP
> -- do they still make those?


Here are some links:
http://nordicgroup.us/digicam/dslr [...] resolution
-table of DSLR's showing "pixel pitch" of around 8 microns. I don't know
how pitch is calculated, your calc giveas around 50 microns for these
cameras.

http://www.outbackphoto.com/dp_ess [...] essay.html
http://www.outbackphoto.com/dp_ess [...] essay.html
Biased by the author's Foveon connection but otherwise very lucid
discussion of sensor/pixel sizes. Interestingly though, he talks about
Foveon downgrading to average out for better SNR at fewer MP like you
discuss. I'm still not clear this can't be done with a simple
downsampling in photoshop but I don't know.

I think sensor size is one part of the formula but there are large pixel
cameras with bad noise & more pixels really does count for more (within
limits). A table showing actual signal to noise ratio (SNR) would answer
this question. I don't know if SNR is as easily graphed as MTF
(resolution) but still MTF like pixel count is more important than
noise. Dynamic range is the other big factor which probably is closely
tied to pixel size. And the quality of the lens is awfully important
too. That's how MTF is usually used though I suppose the sensor quality
effects MTF. Unfortunately none of these critical factors are spelled
out for the smaller MP cameras. I agree it'd be nice to have a super
quality compact 1 to 3MP but I guess the reality is the smaller cameras
are just not taken seriously in terms of quality control so have poorer
lenses, more noise, etc. and the pixel size is targeted as small as
possible for the day's technology. If it has bigger pixels at the low
end, it's because they can't afford to make better smaller pixels.

Reply to Paul

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paul <paul@not.net> writes:

>prep@prep.synonet.com wrote:
>> How do CCDs get hot? They have no electronicss on the chip, unlike CMOS
>> chips, and rare static during exposure.

>I don't know if it's CCD/CMOS dependent but I heard astronomers cool
>their sensors with liquid nitrogen.

They do, because they want to take very long exposures. CCDs have
leakage currents that *double* for every 8 degree C rise in temperature.
If your exposure time is 1/60 second, the leakage in that time is small
compared to the signal you're trying to measure, so it can be ignored.
For somewhat longer exposures (a few seconds), you can take a dark
exposure and subtract it to eliminate most of the effect of leakage.

But astronomers take exposures that are tens of minutes or hours. At
room temperature, CCD leakage would saturate the CCD wells and you'd get
no image at all. So they cool the CCD as cool as practical to reduce
leakage to almost nothing.

Even some astronomical cameras used by amateurs use Peltier devices to
cool the CCD well below room temperature.

But none of this means that a CCD *heats up* during exposure - it just
remains at whatever temperature it is. As "prep" wrote, the CCD isn't
even clocked during exposure, it just has static voltages on it.

Dave

Reply to Anonymous

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On Sat, 23 Apr 2005 21:33:55 -0700, paul wrote:

> -table of DSLR's showing "pixel pitch" of around 8 microns. I don't
> know how pitch is calculated, your calc giveas around 50 microns for
> these cameras.

I didn't look at the link, and didn't examine any formula, but
simple "mind math" showed that if the former was a linear
measurement and the latter was area, they'd be very close, and this
was proved by a calculator. 4 * 4 * pi == 50.265. Of course this
may just be a coincidence.

Reply to Anonymous

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ASAAR wrote:

> On Sat, 23 Apr 2005 21:33:55 -0700, paul wrote:
>
>
>>-table of DSLR's showing "pixel pitch" of around 8 microns. I don't
>>know how pitch is calculated, your calc giveas around 50 microns for
>>these cameras.
>
>
> I didn't look at the link, and didn't examine any formula, but
> simple "mind math" showed that if the former was a linear
> measurement and the latter was area, they'd be very close, and this
> was proved by a calculator. 4 * 4 * pi == 50.265. Of course this
> may just be a coincidence.
>
Pixel pitch is the linear distance from one pixel to the next.
For example, on the Canon 1D Mark II, the sensor size is
28.7 x 19.1 microns, which have 3504 x 2336 pixels.
Pixels spacing (pitch) = 28.7*1000/3504 = 8.2 microns x
19.1*1000/2336 = 8.2 microns. Assuming a square area,
that would be 8.2x8.2 = 67.4 square microns. Pixels
do not necessarily have to be round. The question is,
what is the fill factor (the percentage of the area that
is sensitive to light)? For smaller sensors, it has to be
less. Probably at least a micron or so is needed between the
sensitive areas to keep the charge from leaking across
pixels. If someone has info on fill factor, please post it.

This site http://www.fast-vision.com/cameras/camerasensor.HTM
claims 75% for their CMOS sensors. If similar to the
1D Mark II, the the Mark II would have about 50 square microns
of sensitivity.

Now a small sensor still needs that wall between pixels, and if CMOS
room for electronics, so efficiency of the active area must drop.

Roger

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[A complimentary Cc of this posting was sent to

<prep@prep.synonet.com>], who wrote in article <87r7h1qks7.fsf@prep.synonet.com>:
> readout sends the signal to zero. If you wonder about that, try
> calculating 0.999^2000 and see how many 9s you need to get a
> reasonable answer.

???

perl -wle "print 0.999**2000"
0.135199925397499

Comparing the camera of 2000 and cameras of today are comparing days
and night. The sensors of today are within an order of magnitude of
theoretical limits. If you take large sensors (those used in dSLRs)
then they are within 7x or 8x of theoretical limits.

Cameras of 2000 were a pure junk comparing to what is available today
(at least compacts; I did not have my hands on a dSLR then).

Hope this helps,
Ilya

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[A complimentary Cc of this posting was sent to
Roger N. Clark (change username to rnclark)
<username@qwest.net>], who wrote in article <426A927B.1070300@qwest.net>:

> No. Ilya forgot to include read noise. Read noise is currently
> approximately the same for all good sensors, somewhere in
> the 7-15 electron range. As your signal gets smaller,
> e.g. smaller pixels, or shadow areas, read noise becomes
> a larger fraction of the total noise from the sensor.

You mean "smaller pixels with the same exposition"; but this is not
necessarily how cameras are used. If you increase exposition to
compensate for smaller pixels, you get the same contribution of read
noise. Example:

a) 8 microns square pixel; you expose it as ISO1600; you get (e.g.)
2500 electrons for white; noise of white is 50 electons; read noise
is (e.g.) 12 electrons; total noise is 51 electron;

b) 2 microns square pixel; you expose it as ISO100; you get the same
2500 electrons for white; noise of white is 50 electons; read noise
is (e.g.) 12 electrons; total noise is the same 51 electron.

Of course, cheaper cameras come with lousier sensors (even when the
performance is rescaled for the size); probably, the read noise is
worse too. E.g., with the same throughput QE a 2/3'' sensor should
perform as 8 times less sensitive than half-frame sensor; however, in
my measurements, 50ISO with 2/3'' sensors is only marginally better
than 800ISO with haolf-frame (with the same QE it should behave as
400ISO).

> Note too the diffraction spot diameter: for f/2.8 it is
> 3.2 microns for blue (4700 angstroms) light, 4.1 microns for
> red light (6000 angstroms). Pixels smaller than 4 microns
> have images that are diffraction limited (many high megapixel
> P&S have smaller pixels than this)!

What planet are you on? Today's 2/3'' can produce "throughput" 75%
MTF at 150 lp/mm (with Adobe demosaicer and sharpening mild enough to
not introduce visual artefacts with line art images [no artefacts at
least when viewed on CRT; I did not check yet on LCD]). See the
thread on "MTF of monitors" for an example.

Hope this helps,
Ilya

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Ilya Zakharevich <nospam-abuse@ilyaz.org> writes:

>You mean "smaller pixels with the same exposition"; but this is not
>necessarily how cameras are used. If you increase exposition to
>compensate for smaller pixels, you get the same contribution of read
>noise. Example:

> a) 8 microns square pixel; you expose it as ISO1600; you get (e.g.)
> 2500 electrons for white; noise of white is 50 electons; read noise
> is (e.g.) 12 electrons; total noise is 51 electron;

> b) 2 microns square pixel; you expose it as ISO100; you get the same
> 2500 electrons for white; noise of white is 50 electons; read noise
> is (e.g.) 12 electrons; total noise is the same 51 electron.

True enough. But the difference is that ISO 1600 is near the top end of
the useful ISO range for the DSLR. You can choose to expose at ISO 800,
400, 200, and perhaps 100. Each halving of ISO doubles the number of
electrons per pixel, improving the signal to noise by sqrt(2), and
giving more dynamic range to boot.

On the other hand, ISO 100 is at or near the *bottom* of the ISO range
available in a small-sensor camera. You can't reduce it much without
saturating the sensor, since you're already close to the full-well
capacity of the tiny sensor elements. You can select higher ISOs, with
even noisier results.

So your example shows that the read noise of a DSLR at just about its
worst ISO (in terms of image noise) is equal to a small-sensor P&S
camera operating at or near its best.

Dave

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Dave Martindale wrote:
[]
> So your example shows that the read noise of a DSLR at just about its
> worst ISO (in terms of image noise) is equal to a small-sensor P&S
> camera operating at or near its best.

This is part of how I see the P&S versus DSLR trade-off. Bigger, more
inconvenient and heavy package but with the advantages of higher
sensitivity, lower noise and interchangeable lenses. Decide what you want
to do, pay your money and take your choice.

Cheers,
David

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Ilya Zakharevich wrote:

> Roger N. Clark (change username to rnclark)
> <username@qwest.net>], who wrote in article <426A927B.1070300@qwest.net>:

> You mean "smaller pixels with the same exposition"; but this is not
> necessarily how cameras are used. If you increase exposition to
> compensate for smaller pixels, you get the same contribution of read
> noise.

Yes, if you want to compare iso 1600 images to iso 100 images,
which is hardly a fair comparison. Compare the same ISO and
the smaller pixels then read noise dominates more and more as the
pixel size drops. And the effect is worse in the darker
portions of the image.

> Of course, cheaper cameras come with lousier sensors (even when the
> performance is rescaled for the size); probably, the read noise is
> worse too. E.g., with the same throughput QE a 2/3'' sensor should
> perform as 8 times less sensitive than half-frame sensor; however, in
> my measurements, 50ISO with 2/3'' sensors is only marginally better
> than 800ISO with haolf-frame (with the same QE it should behave as
> 400ISO).

1) Sensor size is irrelevant. It is pixel size that matters.
2) I've shown that modern P&S cameras, like the S60 are photon
noise limited. It is a fundamental property of scaling
pixel size that no matter what the camera throughput and
quantum efficiency of the sensor, larger pixels will
produce higher signal-to-noise images.
3) Your 8 to 10x numbers are based on flawed calculations.
Improvements can come by 2 methods: improving the
transmission of the optics (lens, blur filter, color filters
over the pixels), and sensor quantum efficiency.
Both of these are unlikely to change unless a radical new
detector comes out, and then it is likely only a factor
of 2 better for small as well as large sensors. Transmission
is already high and is unlikely to change. Fill factors
are already effectively 100% from what I'm reading.
Here is a page listing quantum efficiency:
http://www.britastro.org/vss/ccdtable.html
(see spectral response rows). Here is a page
showing fill factor:
http://www.fillfactory.com/htm/tec [...] h_fill.htm

>>Note too the diffraction spot diameter: for f/2.8 it is
>>3.2 microns for blue (4700 angstroms) light, 4.1 microns for
>>red light (6000 angstroms). Pixels smaller than 4 microns
>>have images that are diffraction limited (many high megapixel
>>P&S have smaller pixels than this)!
>
> What planet are you on? Today's 2/3'' can produce "throughput" 75%
> MTF at 150 lp/mm (with Adobe demosaicer and sharpening mild enough to
> not introduce visual artefacts with line art images [no artefacts at
> least when viewed on CRT; I did not check yet on LCD]). See the
> thread on "MTF of monitors" for an example.

I'm in the real world with real physics. You are in the
world of fake math. Look up the diffraction spot size of
a lens.
Diffraction spot diameter = 2.44 * w * f_ratio,
where w = wavelength, and f_ratio is the f/ratio
of the optical system.

Here is a table from:
http://clarkvision.com/imagedetail [...] ize.matter

================================================
red= Green= Blue=
0.6 0.53 0.47
micron micron micron
================================================
f/ratio diffraction spot diameter in microns
================================================
2 2.9 2.6 2.3
2.8 4.1 3.6 3.2
4 5.9 5.2 4.6
5.6 8.2 7.2 6.4
8 11.7 10.3 9.2
11 16.1 14.2 12.6
16 23.4 20.7 18.3
19 27.8 24.6 21.8
22 32.2 28.5 25.2
32 46.8 41.4 36.7
45 65.9 58.2 51.6
64 93.7 82.8 73.4
================================================

For decent photography where you want some control over depth of
field, you want to get to f/8 (and even that is not much depth
of field in many situations), diffraction strongly influences
image quality, and it should be obvious that diffraction is
less of a problem with a larger pixel.

The diffraction limit for an f/2.8 lens at 5000 angstrom (green)
wavelength is: 585 lines/mm = Rayleigh Resolution Criterion,
which is ~9% MTF. That requires pixel spacing if 585*2/1000
= 1.2 microns. But that is only 9% MTF! Yes, you could
see lines on a test target, but that does not make for a
clean sharp image. The 0% MTF is the Dawes limit, which
for a diffraction limited f/2.8 lens is only 550 lines
per mm for 6500 angstrom light (red). So pixels spacing
less than this will show now detail at all. Yet you say
on your web page that the optimum pixel size is less than
a micron.

Do you know of ANY diffraction limited f/2.8 lens on a P&S
camera (diffraction limited over the whole field of view)?
I do not.

>
> Hope this helps,

No it doesn't. You are providing more confusion.
Here is the problem. You cite a number that you pull from
somewhere without consideration of other factors. For example
deriving optimum pixel size that derives quantum efficiencies
10 times less than manufacturer's specifications, and ignore
diffraction. I have honestly tried to help you pointing
out some of these things. You reject them all and then
declare your erroneous result again. This is becoming
no different than the film versus digital religious wars.

Theory is fine when it includes all components in the real world.
Then there is the real world.....

Roger

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paul <paul@not.net> writes:
>> Pixel pitch is the linear distance from one pixel to the next.

>Ah! I doubt all pixels are square & they need some space between. I
>wonder how much that efficiency of packing them tighter has changed.

Most still camera sensors have a pixel grid that's square or very close
to it. If not, you simply have separate horizontal and vertical pitch
numbers.

Also, some CCDs use lenslet arrays in front of the sensor. These
collect virtually all incoming light and focus it onto the
light-sensitve portion of each pixel, giving an effective fill factor of
nearly 100% even though the silicon itself (without the lenses) has a
much lower fill factor.

>I also doubt one could easily find the actual pixel size of consumer
>digicams for a comparison.

My Canon cameras put the pixel pitch values in the EXIF data of every
image they shoot. Even without that, it's not hard to get an estimate:

The size of sensors is usually expressed as one over some number in
inches, for example 1/1.8". This is an odd notation, but what it does
tell you is that the actual image capture area diagonal is about
16/1.8 = 8.9 mm. From that and the sensor aspect ratio (usually 1.33,
but sometimes 1.5) you can calculate the horizontal and vertical size.
In our example, it's about 7.1 x 5.3 mm.

Then divide those numbers by the image size in pixels to get the pixel
pitch. If it's a 4 megapixel camera with 2272 x 1704 images, then the
pixel pitch is 7.1e-3 / 2272 = 3.1e-6, or 3.1 micron.

The example numbers above are for a Canon G2. The actual sensor
resolution from the EXIF data is 8114.29 pixels/inch, which is 319.46
pixels/mm or a pixel pitch of 3.1303 microns.

Dave

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"David J Taylor" <david-taylor@blueyonder.co.not-this-bit.nor-this-part.uk> writes:
> This is part of how I see the P&S versus DSLR trade-off. Bigger, more
> inconvenient and heavy package but with the advantages of higher
> sensitivity, lower noise and interchangeable lenses. Decide what you want
> to do, pay your money and take your choice.

There have been millions of relatively inexpensive compact full frame
35mm point-and-shoot cameras made with high quality lenses, sometimes
even zooms. I don't see why compact digicams can't be made with large
sensors. It must just be a cost thing.

Reply to Anonymous

Archived from groups: rec.photo.digital (More info?)

 

On 25 Apr 2005 09:27:34 -0700, Paul Rubin
<http://phr.cx@NOSPAM.invalid> wrote:

>"David J Taylor" <david-taylor@blueyonder.co.not-this-bit.nor-this-part.uk> writes:
>> This is part of how I see the P&S versus DSLR trade-off. Bigger, more
>> inconvenient and heavy package but with the advantages of higher
>> sensitivity, lower noise and interchangeable lenses. Decide what you want
>> to do, pay your money and take your choice.
>
>There have been millions of relatively inexpensive compact full frame
>35mm point-and-shoot cameras made with high quality lenses, sometimes
>even zooms. I don't see why compact digicams can't be made with large
>sensors. It must just be a cost thing.

It would seem to me that the lenses used on compact, small-CCD cameras
are made specifically to fit eh CCD size used. Many are about 1/3"
diagonal. The lenses are smaller, because they only need to cover that
small CCD.
Putting a full 35mm size CCD in the same camera body will require a
much larger lens (and all incidental hardware). This *will* cost more.
There's no way around it.
Plus, the compact cameras aren't empty; there's 'stuff' already in the
nooks and crannies that exist. To make room fro the larger CCD and
lens, the 'stuff' would need to go somewhere; if miniaturization is
used to reduce the size of the 'stuff', that also increases cost. If
not, it increases size.
At least that's how I see it.

--
Bill Funk
Change "g" to "a"

Reply to Anonymous

Archived from groups: rec.photo.digital (More info?)

 

On Mon, 25 Apr 2005 16:05:11 +0000 (UTC), davem@cs.ubc.ca (Dave
Martindale) wrote:

>The size of sensors is usually expressed as one over some number in
>inches, for example 1/1.8". This is an odd notation, but what it does
>tell you is that the actual image capture area diagonal is about
>16/1.8 = 8.9 mm. From that and the sensor aspect ratio (usually 1.33,
>but sometimes 1.5) you can calculate the horizontal and vertical size.
>In our example, it's about 7.1 x 5.3 mm.

Almost.

From:
http://www.dpreview.com/learn/?/Gl [...] zes_01.htm

"Sensors are often referred to with a "type" designation using
imperial fractions such as 1/1.8" or 2/3" which are larger than the
actual sensor diameters. The type designation harks back to a set of
standard sizes given to TV camera tubes in the 50's. These sizes were
typically 1/2", 2/3" etc. The size designation does not define the
diagonal of the sensor area but rather the outer diameter of the long
glass envelope of the tube. Engineers soon discovered that for various
reasons the usable area of this imaging plane was approximately two
thirds of the designated size. This designation has clearly stuck
(although it should have been thrown out long ago). There appears to
be no specific mathematical relationship between the diameter of the
imaging circle and the sensor size, although it is always roughly two
thirds."


--
Bill Funk
Change "g" to "a"

Reply to Anonymous

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Big Bill <bill@pipping.com> writes:
> It would seem to me that the lenses used on compact, small-CCD cameras
> are made specifically to fit eh CCD size used. Many are about 1/3"
> diagonal. The lenses are smaller, because they only need to cover that
> small CCD.

Correct.

> Putting a full 35mm size CCD in the same camera body will require a
> much larger lens (and all incidental hardware). This *will* cost more.
> There's no way around it.

Well, larger, I don't know about "much larger". The lenses in small
35mm P/S cameras are not that large.

> Plus, the compact cameras aren't empty; there's 'stuff' already in the
> nooks and crannies that exist. To make room fro the larger CCD and
> lens, the 'stuff' would need to go somewhere; if miniaturization is
> used to reduce the size of the 'stuff', that also increases cost. If
> not, it increases size.
> At least that's how I see it.

Take a small P/S digicam like a Canon SD200. That clearly contains
all the stuff in those nooks and crannies. Now take a small 35mm P/S
like an Olympus Stylus. That clearly contains a full frame "sensor"
(film frame) plus a lens capable of covering the sensor. (It also
contains space for the film cartridge and takeup spool). Now imagine
a digicam the size of the SD200 and Olympus Stylus put together. The
result is still a pretty small camera, maybe the size of a Canon A70.
But it clearly has space for a full frame sensor and the associated
electronics. Yes it would cost a lot, but I'm not even sure that's
prohibitive. High end 35mm P/S cameras like the Contax T cost more
tha low end DSLR's of today, so people are willing to pay that much
for compact cameras.

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On 26 Apr 2005 10:58:12 -0700, Paul Rubin
<http://phr.cx@NOSPAM.invalid> wrote:

>Big Bill <bill@pipping.com> writes:
>> It would seem to me that the lenses used on compact, small-CCD cameras
>> are made specifically to fit eh CCD size used. Many are about 1/3"
>> diagonal. The lenses are smaller, because they only need to cover that
>> small CCD.
>
>Correct.
>
>> Putting a full 35mm size CCD in the same camera body will require a
>> much larger lens (and all incidental hardware). This *will* cost more.
>> There's no way around it.
>
>Well, larger, I don't know about "much larger". The lenses in small
>35mm P/S cameras are not that large.
>
>> Plus, the compact cameras aren't empty; there's 'stuff' already in the
>> nooks and crannies that exist. To make room fro the larger CCD and
>> lens, the 'stuff' would need to go somewhere; if miniaturization is
>> used to reduce the size of the 'stuff', that also increases cost. If
>> not, it increases size.
>> At least that's how I see it.
>
>Take a small P/S digicam like a Canon SD200. That clearly contains
>all the stuff in those nooks and crannies. Now take a small 35mm P/S
>like an Olympus Stylus. That clearly contains a full frame "sensor"
>(film frame) plus a lens capable of covering the sensor. (It also
>contains space for the film cartridge and takeup spool). Now imagine
>a digicam the size of the SD200 and Olympus Stylus put together. The
>result is still a pretty small camera, maybe the size of a Canon A70.
>But it clearly has space for a full frame sensor and the associated
>electronics. Yes it would cost a lot, but I'm not even sure that's
>prohibitive. High end 35mm P/S cameras like the Contax T cost more
>tha low end DSLR's of today, so people are willing to pay that much
>for compact cameras.

I'm not so sure that you can compare the innards of a film camera with
that of a digital camera.
The film camera needs the cannister/takeup reels, but the digital
needs the extra electronics to process the image,and of course, a card
to hold the image files (with some pretty amazing things done to the
smaller cards, so that hey are easier to lose! :-) ).
Well, OK, maybe the same volume.
I still wonder why, if it's so possible for the same price, it's not
being done. I think the above has somewhat to do with it.

--
Bill Funk
Change "g" to "a"

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Big Bill <bill@pipping.com> writes:
> The film camera needs the cannister/takeup reels, but the digital
> needs the extra electronics to process the image,and of course, a card
> to hold the image files (with some pretty amazing things done to the
> smaller cards, so that hey are easier to lose! :-) ).
> Well, OK, maybe the same volume.

As explained, a camera the size of a small 35mm AND a small digital
PUT TOGETHER, should be able to hold everything that's in both of them,
and still be a fairly small camera.

> I still wonder why, if it's so possible for the same price, it's not
> being done. I think the above has somewhat to do with it.

It couldn't be done at the same price as today's compact digicams.
But it could probably be done at the price of today's entry level
DSLR's. It's an open question whether anyone would pay that much for
a compact digicam with a large sensor. People still seem to want
gimmick features like extreme pixel counts.

Reply to Anonymous

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On 26 Apr 2005 13:05:25 -0700, in rec.photo.digital , Paul Rubin
<http://phr.cx@NOSPAM.invalid> in <7xis29nw1m.fsf@ruckus.brouhaha.com>
wrote:

>Big Bill <bill@pipping.com> writes:
>> The film camera needs the cannister/takeup reels, but the digital
>> needs the extra electronics to process the image,and of course, a card
>> to hold the image files (with some pretty amazing things done to the
>> smaller cards, so that hey are easier to lose! :-) ).
>> Well, OK, maybe the same volume.
>
>As explained, a camera the size of a small 35mm AND a small digital
>PUT TOGETHER, should be able to hold everything that's in both of them,
>and still be a fairly small camera.
>
>> I still wonder why, if it's so possible for the same price, it's not
>> being done. I think the above has somewhat to do with it.
>
>It couldn't be done at the same price as today's compact digicams.
>But it could probably be done at the price of today's entry level
>DSLR's. It's an open question whether anyone would pay that much for
>a compact digicam with a large sensor. People still seem to want
>gimmick features like extreme pixel counts.

It is not so much gimmick as explainable with a single number. S/N is
a bit hard to understand, but megapixels/wattage (a la
stereos)/horsepower/etc forms a nice single number. For a camera there
are multiple numbers to track. Not a problem for aficionados, but
difficult for the general public. I suspect that big numbers on the
high end stuff actually helps sell the lower end stuff.

--
Matt Silberstein

All in all, if I could be any animal, I would want to be
a duck or a goose. They can fly, walk, and swim. Plus,
there there is a certain satisfaction knowing that at the
end of your life you will taste good with an orange sauce
or, in the case of a goose, a chestnut stuffing.

Reply to Anonymous

Archived from groups: rec.photo.digital (More info?)

 

Big Bill <bill@pipping.com> writes:

>Putting a full 35mm size CCD in the same camera body will require a
>much larger lens (and all incidental hardware). This *will* cost more.
>There's no way around it.

It will certainly require more glass, and be bigger and heavier. On the
other hand, the machining and mechanical assembly tolerances get looser
at the same time, so you'd save some money there. It's not obvious how
much more the larger lens would cost, particularly if the camera could
use a long-proven lens design from a film P&S camera.

The *bit* extra-cost item is the sensor. Going from current digicam
sensors to full-frame 35 is an increase in dimensions by a factor of 5
or 6. The larger sensor would have at least 5^2 = 25 times as much
silicon area, but the sensor would cost much more than 25 times as much
per unit because of the way yield scales with chip size.


Dave

Reply to Anonymous

Archived from groups: rec.photo.digital (More info?)

 

>On Mon, 25 Apr 2005 16:05:11 +0000 (UTC), davem@cs.ubc.ca (Dave
>Martindale) wrote:
>
>>The size of sensors is usually expressed as one over some number in
>>inches, for example 1/1.8". This is an odd notation, but what it does
>>tell you is that the actual image capture area diagonal is about
>>16/1.8 = 8.9 mm.

Big Bill <bill@pipping.com> writes:
>Almost.

>"Sensors are often referred to with a "type" designation using
>imperial fractions such as 1/1.8" or 2/3" which are larger than the
>actual sensor diameters. The type designation harks back to a set of
>standard sizes given to TV camera tubes in the 50's. These sizes were
>typically 1/2", 2/3" etc. The size designation does not define the
>diagonal of the sensor area but rather the outer diameter of the long
>glass envelope of the tube. Engineers soon discovered that for various
>reasons the usable area of this imaging plane was approximately two
>thirds of the designated size. This designation has clearly stuck
>(although it should have been thrown out long ago). There appears to
>be no specific mathematical relationship between the diameter of the
>imaging circle and the sensor size, although it is always roughly two
>thirds."

I'm afraid I don't see where your "almost" comes from.

The quote above suggests that you take the "type" and multiply by 2/3
to convert from "nominal tube diameter" to the diagonal of the image
area. 2/3 of one inch (25.4 mm) is 16.9 mm. What I wrote suggested
starting with 16 mm instead of 16.9. There's no disagreement between
the two quotes above, because one says "about" 16 and the other says
"roughly" 16.9 mm (from 2/3 inch).

On the other hand, what I wrote gave an example of how to take the magic
number 1/1.8, plus the aspect ratio of the image and the pixel count of
the sensor, and calculate an actual pixel pitch. The result will be
approximate because the 16 mm value is approximate and "1.8" doesn't
have many significant figures. But it works pretty well in practice.

Dave

Reply to Anonymous

Archived from groups: rec.photo.digital (More info?)

 

Hi Roger & Ilya,
>
> Diffraction spot diameter = 2.44 * w * f_ratio,
> where w = wavelength, and f_ratio is the f/ratio
> of the optical system.
<snip useful table>
> For decent photography where you want some control over depth of
> field, you want to get to f/8 (and even that is not much depth
> of field in many situations), diffraction strongly influences
> image quality, and it should be obvious that diffraction is
> less of a problem with a larger pixel.
>
> The diffraction limit for an f/2.8 lens at 5000 angstrom (green)
> wavelength is: 585 lines/mm = Rayleigh Resolution Criterion,
> which is ~9% MTF. That requires pixel spacing if 585*2/1000
On the danger of being pedantic:
According to my text book on optics the original Rayleigh criterion is about
two-line resolution in spectroscopes: the lines can be said to be 'just
resolved' when the maximum of the image of one coincides with the minimum of
the other.
This was extended to two-point resolution by coinciding the maximum of one
with the minimum of the Airy disk diffraction pattern of the other:
R = 0.61 lambda/sin(half_aperture) (for aperture << 1, circular aperture,
incoherent light)
For small apertures sin(half_aperture) ~ 1/(2f_number) so:
R = 0.61 * lambda * 2 * f_number
To detect the minimum between the maxima you need two pixels per Rayleigh
distance so the 'Rayleigh pixel size' is 2.44 * lambda * f_number.
So this rediscovers Rayleigh's work from 1879!
> = 1.2 microns. But that is only 9% MTF! Yes, you could
> see lines on a test target, but that does not make for a
> clean sharp image. The 0% MTF is the Dawes limit, which
> for a diffraction limited f/2.8 lens is only 550 lines
> per mm for 6500 angstrom light (red). So pixels spacing
> less than this will show now detail at all. Yet you say
> on your web page that the optimum pixel size is less than
> a micron.
However, if we take the blue 470 nm light then the critical sampling rate is:
delta_x = lambda/(4 * sin(half_aperture) ~ lambda * f_number/2
so for 470nm the sampling distance is ~.66 micron. To capture all information
passed by the lens this is the pixel spacing you need. It could very well be
that readout noise problems and the like make it not feasible, but that is
something else.
>
> Do you know of ANY diffraction limited f/2.8 lens on a P&S
> camera (diffraction limited over the whole field of view)?
I get the impression spherical aberration is so strong in these P&S lenses
that all rays above say f/8 are 'lost'. With that the whole computation above
goes to pieces. Add chromatic aberration and you end up with a 640x480 image
at best.
Quite likely such lenses can be made though, especially for smaller focal
lengths, and using the space where the mirror is in a (d)SLR. But high
quality camera makers have a hard time at the moment.

-- Hans

Reply to Anonymous

Archived from groups: rec.photo.digital (More info?)

 

[A complimentary Cc of this posting was sent to
Roger N. Clark (change username to rnclark)
<username@qwest.net>], who wrote in article <426CF488.5030905@qwest.net>:
> > You mean "smaller pixels with the same exposition"; but this is not
> > necessarily how cameras are used. If you increase exposition to
> > compensate for smaller pixels, you get the same contribution of read
> > noise.

> Yes, if you want to compare iso 1600 images to iso 100 images,

Almost right. Comparing half-frame to 2/3'' sensors (with same pixel
count), it is 8x smaller area; so with the same throughput QE, it is
comparing ISO800 with ISO100. (Although, as I said, the assumption of
the same throughput QE does not currently hold.)

> which is hardly a fair comparison.

Actually, it may be quite fair. Depends on the situation. E.g., you
need 3 f-stops larger aperture to get the same depth of field with
2/3''; this exactly compensates for the difference in sensibility.

[Of course, this assumes that in both situations the lenses perform
similarly good (with goodness measured w.r.t. diffraction-bound
lens of the same f-stop). This is not always true, the zoom lenses used
with current 2/3'' are only 2 f-stops "better in optical quality"
than fixed-focal-length lenses used with film; do not know about
new lenses designed for half-frames.]

In addition, the smaller sensor is easier to motion-compensate; this
may also improve "practical sensitivity" of this sensor.

> 1) Sensor size is irrelevant. It is pixel size that matters.

While correct, this is irrelevant, since current "leaders" have the
same pixel count.

> 2) I've shown that modern P&S cameras, like the S60 are photon
> noise limited.

a) You mean electron noise here, not photon noise; but let keep this
discussion in one thread, not in many;

b) This is very strange data for S60: with 8 times smaller sensor
you quote 2.5 times smaller full well. Are you sure the data is
for 100ISO?

> It is a fundamental property of scaling
> pixel size that no matter what the camera throughput and
> quantum efficiency of the sensor, larger pixels will
> produce higher signal-to-noise images.

This is manifestly wrong. What matters is product of throughput QE
and the area.

Or do you mean "with the same technology for both sensors"? Then of
course it is true. So with (imminent) 6x improvement in throughput
you can get 10000ISO from large sensors vs 1200IS for small ones. The
people who *need* 10000ISO will have a clear choice. But the people
who do not need more than 1000ISO (with practically no noise) will
*also* have a clear choice.

> 3) Your 8 to 10x numbers are based on flawed calculations.

I think 8x is theoretical, with practical about 6x; but let us keep it
in a separate thread.

> >>Note too the diffraction spot diameter: for f/2.8 it is
> >>3.2 microns for blue (4700 angstroms) light, 4.1 microns for
> >>red light (6000 angstroms). Pixels smaller than 4 microns
> >>have images that are diffraction limited (many high megapixel
> >>P&S have smaller pixels than this)!
> >
> > What planet are you on? Today's 2/3'' can produce "throughput" 75%
> > MTF at 150 lp/mm (with Adobe demosaicer and sharpening mild enough to
> > not introduce visual artefacts with line art images [no artefacts at
> > least when viewed on CRT; I did not check yet on LCD]). See the
> > thread on "MTF of monitors" for an example.
>
> I'm in the real world with real physics. You are in the
> world of fake math. Look up the diffraction spot size of
> a lens.

I see that it is you who are in the world of fake math. Take a test
shot, and see by yourselves. Or look at the example image I provided
(actually, it is not the best possible; when I have time, I will
upload the slightly improved one).

BTW, diffraction spot size is absolutely irrelevant in the age of DSP.
The only important thing is the throughput MTF curve vs throughput
narrow-band noise; it shows what CAN'T be extracted from the image
with DSP.

Hope this helps,
Ilya

Reply to Anonymous

Archived from groups: rec.photo.digital (More info?)

 

[A complimentary Cc of this posting was sent to
HvdV
<nohanz@svi.nl>], who wrote in article <a1990$4270c7bf$3e3aaa83$8037@news.versatel.nl>:
> This was extended to two-point resolution by coinciding the maximum of one
> with the minimum of the Airy disk diffraction pattern of the other:
> R = 0.61 lambda/sin(half_aperture) (for aperture << 1, circular aperture,
> incoherent light)
> For small apertures sin(half_aperture) ~ 1/(2f_number) so:
> R = 0.61 * lambda * 2 * f_number
> To detect the minimum between the maxima you need two pixels per Rayleigh
> distance so the 'Rayleigh pixel size' is 2.44 * lambda * f_number.
> So this rediscovers Rayleigh's work from 1879!

All this is irrelevant in the age of DSP. But I see that your next
paragraph has correct coefficients (ones which no amount of DSP can
improve):

> ... the critical sampling rate is:
> delta_x = lambda/(4 * sin(half_aperture) ~ lambda * f_number/2
> so for 470nm the sampling distance is ~.66 micron. To capture all information
> passed by the lens this is the pixel spacing you need.

> It could very well be
> that readout noise problems and the like make it not feasible, but that is
> something else.

Practical experiments show that with very low readout noise of today,
one should be able to get quite close to this "critical sampling
rate" (at least with higher f-stops).

> I get the impression spherical aberration is so strong in these P&S lenses
> that all rays above say f/8 are 'lost'. With that the whole computation above
> goes to pieces. Add chromatic aberration and you end up with a 640x480 image
> at best.

To the contrary; the lenses for current P&S are *incomparably better*
than those for larger cameras. And this is as it should be: the same
wavelength/40 tolerance is much more demanding if you have a lot of
glass (as you do with a larger lens).

E.g., consider an 8x zoom with sweet spot at f/4... The exact MTF of
the lens is very hard to measure; but as I said, the throughput MTF of
the whole process can be very high (while creating no artefacts and
creating very little "extra" noise). It is practical to have MTF 75%
at 150 lp/mm...

Hope this helps,
Ilya

Reply to Anonymous

Archived from groups: rec.photo.digital (More info?)

 

HvdV wrote:

> Hi Roger & Ilya,
>
>>
>> Diffraction spot diameter = 2.44 * w * f_ratio,
>> where w = wavelength, and f_ratio is the f/ratio
>> of the optical system.
>
> <snip useful table>
>
>> For decent photography where you want some control over depth of
>> field, you want to get to f/8 (and even that is not much depth
>> of field in many situations), diffraction strongly influences
>> image quality, and it should be obvious that diffraction is
>> less of a problem with a larger pixel.
>>
>> The diffraction limit for an f/2.8 lens at 5000 angstrom (green)
>> wavelength is: 585 lines/mm = Rayleigh Resolution Criterion,
>> which is ~9% MTF. That requires pixel spacing if 585*2/1000
>
> On the danger of being pedantic:
> According to my text book on optics the original Rayleigh criterion is
> about
> two-line resolution in spectroscopes: the lines can be said to be 'just
> resolved' when the maximum of the image of one coincides with the
> minimum of
> the other.
> This was extended to two-point resolution by coinciding the maximum of one
> with the minimum of the Airy disk diffraction pattern of the other:
> R = 0.61 lambda/sin(half_aperture) (for aperture << 1, circular aperture,
> incoherent light)
> For small apertures sin(half_aperture) ~ 1/(2f_number) so:
> R = 0.61 * lambda * 2 * f_number
> To detect the minimum between the maxima you need two pixels per Rayleigh
> distance so the 'Rayleigh pixel size' is 2.44 * lambda * f_number.
> So this rediscovers Rayleigh's work from 1879!

HvdV,
Concerning both above and below, it seems your equation differs by a
factor of 2 from that in "Star Testing Astronomical Telescopes,
A Manual for Optical Evaluation and Adjustment" by HR Suiter,
William Bell, Richmond, 1994, page 49, equation 3.5:

S'max = 1/(F*w)

where F = focal ratio, w = wavelength, and S'max is the critical
sampling (0% MTF) in cycles (line pairs) per length (given by the units
of the wavelength). For 0.47 micron wavelength, F=2.8 the
equation gives S'max = 1/(2.8*0.00047 mm) = 760 line pairs/mm.
The Rayleigh limit is at about 82% of the critical limit,
which for 0.47 microns wavelength would be about 620 lp/mm.

In a diffraction limited system, the Rayleigh resolution
criteria occurs when the separation of two objects is precisely
the radius of the theoretical diffraction disk (Suiter, 1994,
page 286). The radius is defined from the maximum to the
first minimum of the diffraction disk. This separation
causes a minimum in the response at the radius, so the
radius is the ideal sampling distance.

The diffraction disk radius, R_airy, is (Suiter, 1994, page 11,
equation 1.1):

R_airy = 1.22*w*f/D

where w = wavelength, f = focal length, and D = aperture
diameter. This reduces to:

R_airy = 1.22*w*F (where F = focal ratio).

For 0.47 micron wavelength, F=2.8 R_airy = 1.22*.47*2.8 = 1.6 microns.

This is the Nyquist sampling interval, meaning one sample at the
peak, one sample at the minimum.

I haven't gone through your equations in detail, but I
suspect you used an equation assuming a diameter and divided
by 2 getting the factor of two smaller sampling, when the
equation was already for radius.

I believe this is correct. It matches examples given in Suiter.
Equation 1.1 is quite well known and far predates Suiter, 1994.
I'm just quoting Suiter as it is an excellent book that brings
a lot of information together into one place.

Roger

>
>> = 1.2 microns. But that is only 9% MTF! Yes, you could
>> see lines on a test target, but that does not make for a
>> clean sharp image. The 0% MTF is the Dawes limit, which
>> for a diffraction limited f/2.8 lens is only 550 lines
>> per mm for 6500 angstrom light (red). So pixels spacing
>> less than this will show now detail at all. Yet you say
>> on your web page that the optimum pixel size is less than
>> a micron.
>
> However, if we take the blue 470 nm light then the critical sampling
> rate is:
> delta_x = lambda/(4 * sin(half_aperture) ~ lambda * f_number/2
> so for 470nm the sampling distance is ~.66 micron. To capture all
> information
> passed by the lens this is the pixel spacing you need. It could very
> well be
> that readout noise problems and the like make it not feasible, but that is
> something else.
>
>>
>> Do you know of ANY diffraction limited f/2.8 lens on a P&S
>> camera (diffraction limited over the whole field of view)?
>
> I get the impression spherical aberration is so strong in these P&S lenses
> that all rays above say f/8 are 'lost'. With that the whole computation
> above
> goes to pieces. Add chromatic aberration and you end up with a 640x480
> image
> at best.
> Quite likely such lenses can be made though, especially for smaller focal
> lengths, and using the space where the mirror is in a (d)SLR. But high
> quality camera makers have a hard time at the moment.
>
> -- Hans

Reply to Anonymous

Archived from groups: rec.photo.digital (More info?)

 

Hi Roger,
>> According to my text book on optics the original Rayleigh criterion is
>> about
>> two-line resolution in spectroscopes: the lines can be said to be 'just
>> resolved' when the maximum of the image of one coincides with the
>> minimum of
>> the other.
>> This was extended to two-point resolution by coinciding the maximum of
>> one
>> with the minimum of the Airy disk diffraction pattern of the other:
>> R = 0.61 lambda/sin(half_aperture) (for aperture << 1, circular aperture,
>> incoherent light)
You can find this relation in various sources, e.g. Born&Wolf, Principles of
Optics. In my 7th ed. on p 468 and others. It is for incoherent light,
paraxial approximation, medium refractive index 1, and two point objects.
>> For small apertures sin(half_aperture) ~ 1/(2f_number) so:
>> R = 0.61 * lambda * 2 * f_number
The approximation I used here is
sin(half_aperture) = sin(arctan(D/2f))~ 1/2F, F the focal ratio.
Good enough for F > 2.8 or so, at F 1.4 the error is 5%.
>
> HvdV,
> Concerning both above and below, it seems your equation differs by a
> factor of 2 from that in "Star Testing Astronomical Telescopes,
> A Manual for Optical Evaluation and Adjustment" by HR Suiter,
> William Bell, Richmond, 1994, page 49, equation 3.5:
>
> S'max = 1/(F*w)
Whereas the two-point Rayleigh distance (using your symbols) is
R ~ 1.22*w*F.
Two-point resolution is different from n-line resolution which might account
for the 22% difference, IIRC lines are a bit easier to resolve than points.
>
> where F = focal ratio, w = wavelength, and S'max is the critical
> sampling (0% MTF) in cycles (line pairs) per length (given by the units

> of the wavelength). For 0.47 micron wavelength, F=2.8 the
> equation gives S'max = 1/(2.8*0.00047 mm) = 760 line pairs/mm.
> The Rayleigh limit is at about 82% of the critical limit,
> which for 0.47 microns wavelength would be about 620 lp/mm.
>
> In a diffraction limited system, the Rayleigh resolution
> criteria occurs when the separation of two objects is precisely
> the radius of the theoretical diffraction disk (Suiter, 1994,
> page 286). The radius is defined from the maximum to the
> first minimum of the diffraction disk. This separation
> causes a minimum in the response at the radius, so the
> radius is the ideal sampling distance.
>
> The diffraction disk radius, R_airy, is (Suiter, 1994, page 11,
> equation 1.1):
>
> R_airy = 1.22*w*f/D
Yes, this matches the approximation above.
>
> where w = wavelength, f = focal length, and D = aperture
> diameter. This reduces to:
>
> R_airy = 1.22*w*F (where F = focal ratio).
>
> For 0.47 micron wavelength, F=2.8 R_airy = 1.22*.47*2.8 = 1.6 microns.
When the two Airy patterns overlap in 'peak on the first dark ring of the
other' fashion, a local minimum in between the peaks 26.5% lower than the
peak results. To sample this configuration you need a (point) sample at the
minimum, so the pseudo Nyquist interval is R_airy/2. In this case .8 microns.
Incidently, the figure of the 26.5% dip is also sometimes referred to as
'Rayleigh criterion'. In practice the value is greatly affected by the degree
of coherency, not mentioning aberrations.
>
> This is the Nyquist sampling interval, meaning one sample at the
> peak, one sample at the minimum.
Yes, the minimum between the two maxima.
>
> I haven't gone through your equations in detail, but I
> suspect you used an equation assuming a diameter and divided
> by 2 getting the factor of two smaller sampling, when the
> equation was already for radius.
It's easy to loose a factor of two somewhere, but I think this solves it.
>
> I believe this is correct. It matches examples given in Suiter.
> Equation 1.1 is quite well known and far predates Suiter, 1994.
> I'm just quoting Suiter as it is an excellent book that brings
> a lot of information together into one place.
I don't know it; is it astronomy oriented?

>> However, if we take the blue 470 nm light then the critical sampling
>> rate is:
>> delta_x = lambda/(4 * sin(half_aperture) ~ lambda * f_number/2
You can find this equation for example in C.J.R Sheppard 'Optical resolution
and the spatial frequency cut-off', Optik 66, 1983 and Optik 72, 1985.
>> so for 470nm the sampling distance is ~.66 micron. To capture all
The fact that this value is different than the Rayleigh value above is no
surprize since the idea behind the Rayleigh criterion is, though practical,
arbitrary. If the Rayleigh criterion would have demanded a 1% dip in an
n-line pattern the values would have been closer. The value of a bandwidth
related criterion is, IMO, that it is independent of aberrations and the
exact shape of the PSF.

-- Hans

Reply to Anonymous

Archived from groups: rec.photo.digital (More info?)

 

Hi Ilya,
>
>
> I see that it is you who are in the world of fake math. Take a test
Ah, but it is a nice world! Unless you mean the math itself is fake ;-)
>
> BTW, diffraction spot size is absolutely irrelevant in the age of DSP.
> The only important thing is the throughput MTF curve vs throughput
> narrow-band noise; it shows what CAN'T be extracted from the image
> with DSP.
Well, you could say the PSF shape is equivalent to the MTF. Of course the
actual PSF hardly ever looks like a diffraction limited PSF, diffraction
limited in the sense of a aberration-free system. The PSF shape and the noise
statistics together are the main ingredients to the image formation, ok.

-- Hans

Reply to Anonymous

Archived from groups: rec.photo.digital (More info?)

 

Hi Ilya,
>>So this rediscovers Rayleigh's work from 1879!
>
>
> All this is irrelevant in the age of DSP. But I see that your next
> paragraph has correct coefficients (ones which no amount of DSP can
> improve):
With a bit of hindsight one could say Rayleigh's and Abbe's work is directly
related to the optical bandwidth problem, so IMO not irrelevant. But I admit,
it is a bit of a hobby horse.
>
>
>>... the critical sampling rate is:
>>delta_x = lambda/(4 * sin(half_aperture) ~ lambda * f_number/2
>>so for 470nm the sampling distance is ~.66 micron. To capture all information
>>passed by the lens this is the pixel spacing you need.

> Practical experiments show that with very low readout noise of today,
> one should be able to get quite close to this "critical sampling
> rate" (at least with higher f-stops).
Nice to hear that; any examples available?
>
>
>>I get the impression spherical aberration is so strong in these P&S lenses
>>that all rays above say f/8 are 'lost'. With that the whole computation above
>>goes to pieces. Add chromatic aberration and you end up with a 640x480 image
>>at best.
>
>
> To the contrary; the lenses for current P&S are *incomparably better*
> than those for larger cameras. And this is as it should be: the same
> wavelength/40 tolerance is much more demanding if you have a lot of
> glass (as you do with a larger lens).
Exactly the point I was trying to make in an earlier thread. What still
baffles me however, is the poor quality of some 'test winning' P&Ss as
compared to the *much* older SLR lenses I have.
This can only be explained by manufacturers only aiming at an as cheap as
possible lens, but with a high zoom number. Understandable from the
manufacturer's standpoint, with the fierce competition survival is #1.
>
> E.g., consider an 8x zoom with sweet spot at f/4... The exact MTF of
> the lens is very hard to measure; but as I said, the throughput MTF of
> the whole process can be very high (while creating no artefacts and
> creating very little "extra" noise). It is practical to have MTF 75%
> at 150 lp/mm...
Which lens is that?

-- Hans

Reply to Anonymous

Archived from groups: rec.photo.digital (More info?)

 

HvdV wrote:

> When the two Airy patterns overlap in 'peak on the first dark ring of
> the other' fashion, a local minimum in between the peaks 26.5% lower
> than the peak results. To sample this configuration you need a (point)
> sample at the minimum, so the pseudo Nyquist interval is R_airy/2. In
> this case .8 microns.
> Incidently, the figure of the 26.5% dip is also sometimes referred to as
> 'Rayleigh criterion'. In practice the value is greatly affected by the
> degree of coherency, not mentioning aberrations.
>
>> This is the Nyquist sampling interval, meaning one sample at the
>> peak, one sample at the minimum.
>
> Yes, the minimum between the two maxima.

HvDv,
This is where we disagree. The minimum occurs at R_airy, not R_airy/2.
The distance between samples is R_airy. You have double Nyquist sampling.
Nyquist sampling occurs at the maxima and minima.

> The fact that this value is different than the Rayleigh value above is
> no surprize since the idea behind the Rayleigh criterion is, though
> practical, arbitrary. If the Rayleigh criterion would have demanded a 1%
> dip in an n-line pattern the values would have been closer. The value of
> a bandwidth related criterion is, IMO, that it is independent of
> aberrations and the exact shape of the PSF.

Yes, I agree completely. The shape of the MTF is a major difference
between film and digital cameras and the major factor in the film versus
digital wars.

Roger

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