5400 Grain Dissolver and MTF impact?

F

Fernando

Very interesting shots. For some reason the digital ones seem to be
oversharpened compared to the film. There is a noticeable fringe
on either side of the roofline in the first image, for example.
I don't think this alters your conclusions, but it would be nice
to know if this degree of sharpening is something you did or is
inherent in the digital camera output.

Thanks for your contribution.

This is what I did:

1) RAW conversion via ACR 2.3, selecting the largest possible image
size (something like 6000x4000) because in previous tests, I found
that the resizing algorythm of ACR is better than any other I tried.
2) White balance fine-tuning within Photoshop CS, working at 48bpp
3) Upsampling with Bicubic Smoother to match final scan size (about 36
megapixels or so)
4) Sharpen using the excellent FocalBlade 1.03 plug-in, with low
radius (first pass at 0.5 pixels, second pass at 1.0 pixel) and high
halo suppression (115 on both White Halo and Black Halo), plus halo
compensation on both Edge Sharpening and Texture Sharpening.
This was a due pass, for the image was terribly soft after the
interpolation. Digital loyalist would have killed me! :D

The strange fringings (that in some cases seem to "double" the edges)
were already present before the FocalBlade sharpening pass (that of
course made them more evident), and that was the *only* sharpening
pass I did... I think they were somehow introduced by the heavy
upsampling, but it's only my opinion of course.
They visually prefer the lack of grain, and the enhanced edge contrast
gives the impression of more detail than is actually present.

Yes, I agree!
But on some subjects (landscapes and macro, for example), I asked some
untrained friends to compare digital prints (13x18" Lightjet prints,
under good light) from scanned Provia and digital capture, and the
majority of them selected the film-originated shots: "they seem more
real and the grass/flowers/trees are more sharp here!".

Anyway, my test was not about final pleasentness, it was about
ultimate resolution power: I was tired of reading sillyness like "6mp
DSLR shots are now as detailed as film shots in any situation".
It just isn't true. I think you have to shoot with a 1Ds to actually
match scanned film resolution power, grain and pleasentness apart.
And I'm now more convinced in my decision to shoot film for landscapes
and such, and shoot digital for high ISO situations, portraits and
commercials. So, tests are useful sometimes. :)

Please let me know if you are interested in having the original RAW
file, I have no problems in sharing it for further testings.

Thanks,

Fernando
 
W

Wilfred

Robert said:
I think what you have illustrated so clearly is why many people find
digital images equal or better than film under normal magnifications.
They visually prefer the lack of grain, and the enhanced edge contrast
gives the impression of more detail than is actually present.
In many situations (like portraits, for example) there is very little
fine detail (except for eyelashes and stray hair). The enhanced edge
contrast makes this look "sharp" and the lack of grain makes the skin
look smoother. Thus the image is deemed to be "better".

Yes, and I think that's especially true for images displayed on
monitors, where the light source is in the image itself and the image is
pixelated. The 'pixelation' also tends to emphasize the grain (another
case of grain aliasing, I think; even with downsampling it's hard to get
rid of all the grain). It's my impression that in printed images, the
grain is much less conspicious.
After all, it's what the viewer likes that makes the sale.

.... and then we have to consider that more and more images are sold
based on a first impression from a monitor.
 
W

Wilfred

Fernando said:
Anyway, my test was not about final pleasentness, it was about
ultimate resolution power: I was tired of reading sillyness like "6mp
DSLR shots are now as detailed as film shots in any situation".
It just isn't true. I think you have to shoot with a 1Ds to actually
match scanned film resolution power, grain and pleasentness apart.
And I'm now more convinced in my decision to shoot film for landscapes
and such, and shoot digital for high ISO situations, portraits and
commercials. So, tests are useful sometimes. :)

It would also be interesting to downsample the film scan to 6MP, perhaps
after using NeatImage to get rid of the grain, then upsampling it again
to its original resolution. It wouldn't surprise me if it would be
undistinguishable from the upsampled digital picture.
 
F

Fernando

It would also be interesting to downsample the film scan to 6MP, perhaps
after using NeatImage to get rid of the grain, then upsampling it again
to its original resolution. It wouldn't surprise me if it would be
undistinguishable from the upsampled digital picture.

It would be absolutely obvious, to me. When you downsample the scan to
6mp, of course you lose details, limiting them to those that can be
resolved in a 6mp image: that is quite what the 6mp DSLR already
does... so I don't see much point here (film scan has more details
precisely because can offer more actual resolution).

But maybe I misinterpred your statement...?

Fernando
 
W

Wilfred

Fernando said:
It would be absolutely obvious, to me. When you downsample the scan to
6mp, of course you lose details, limiting them to those that can be
resolved in a 6mp image: that is quite what the 6mp DSLR already
does... so I don't see much point here (film scan has more details
precisely because can offer more actual resolution).

But maybe I misinterpred your statement...?

I think it would make your statement stronger

<quote> I was tired of reading sillyness like '6mp DSLR shots are now as
detailed as film shots in any situation'. It just isn't true. I think
you have to shoot with a 1Ds to actually match scanned film resolution
power, grain and pleasentness apart </endquote>.

It would clearly show that the same 'nicer and smoother looking digital
pictures' can also be produced based on the information recorded on
film. Of course you already know but it might a very convincing
illustration for 'the others' :)
 
F

Fernando

It would clearly show that the same 'nicer and smoother looking digital
pictures' can also be produced based on the information recorded on
film. Of course you already know but it might a very convincing
illustration for 'the others' :)

Right! :)
I'll try it tomorrow at home, could be interesting to see what I come
out with. :)

Fernando
 
D

David J. Littleboy

Kennedy McEwen said:
Completely wrong David!

Well, the published MTF curves certainly _predict the response incorrectly_
for low contrast targets.
The MTF still exists at 100cy/mm for 1.6:1 targets but the resulting
contrast in the image has fallen below the noise level. That certainly
does not mean that the MTF is zero, it just means that it requires a
higher contrast original source to measure it or a tedious averaging
method to reduce the noise floor of the measurement medium.

The film is the measurement medium, and it's not responding. You can't
idealize away the noise: it's an inherent property of the medium. If a
section of your photograph has detail with 1.6:1 contrast _as projected on
the film_, then you won't see that detail.
MTF is a measurement of the optical component or system, it is
completely independent of the illumination levels used in the test -
although that may well restrict how much of the unit's performance can
be assessed.

Again, the complaint is that for the images I'm taking, I need low-contrast
performance. The theoretical MTF in response to a contrast 500 times more
than what I've got doesn't tell me what the film does in my images. The
signal that I get off the film has noise in it, and I don't have the option
of ignoring that noise.
Note the difference between zero *contrast* in the resulting image and
zero *MTF* for the medium - they are *NOT* the same thing!

??? I thought that the MTF was the contrast of the thing being measured. If
I'm measuring the medium, that's what I want to measure.
No! No! No!
Absolutely not!

Measuring MTF with a low contrast signal is like measuring the
dimensions of CCD pixels with a foot rule! Sure, you can do it - but
you have to understand the limits of your measurement technique and make
sure that the results you get are not just a consequence of the method.

I didn't mean to say measure the MTF only for low-contrast images, I meant
to say also report the MTF for low-contrast images.

Most of the signals we record on slide films in actual photography are areas
that fall in a fairly narrow range of zones. So the response that we
actually use and need to render our subjects (not just the edges) is the low
contrast response.
Your assessment of a 1.6:1 contrast resolution limit as an upper limit
of the MTF curve is just such a limitation - and the Fuji data sheet you
linked to actually says as much! *Nowhere* on that data sheet does it
state that the MTF is measured with a particular contrast signal -
because MTF is *independent* of the source contrast. It is a transfer
function of the medium - that is why it is called Modulation Transfer
Function. The resolution limit of the film is given on the data sheet
for two different contrasts, because these are the contrasts which, when
transformed by the MTF of the film, result in a signal which is
detectable with a defined (but not stated) signal to noise ratio. The
noise in this case being the film grain.

Talking about the performance of a system abstracted away from the noise
seems very much the wrong thing.
And the shadows? That is where the contrast with the fully lit sky was
well in excess of 1000:1.

I doubt it. The shadows are lit by full open sky. That's a lot of light.
Bart discussed this here before: it's really quite hard to create a 1000:1
contrast.

This argument is problematic because I don't really mean to say never: I
mean to say rare. Since low contrast is far more common, it's the low
contast performance of the film that I need to model.
The contrast between the highlights on the
transformer and the sky was certainly much lower, but that wasn't the
parts of the image I suggested were in high contrast.

If none of your images ever exceed 1000:1 contrast, why bother with
quality film?

Now you're being silly.
You can probably make reversal emulsions which have a
Dmax of 3 in your kitchen sink, let alone the crap, fogged and badly
stored films you can buy down the average flea market! Your argument
basically boils down to a statement that even the worst film available
commercially has far more latitude and dynamic range than you ever
encounter in you photographic exercises.

Ah, I see the reason for the silliness: you've misunderstood what I'm trying
to say.
Sorry, but I don't believe
that you are that limited, David - remember, I have seen some of your
work!

http://www.pbase.com/davidjl/image/21864044/large

Detail at: http://www.pbase.com/davidjl/image/21867927/original

(This shot is not as sharp as I'd like.)

If I want to resolve the texture in the trees in a distant forrest, then the
contrast isn't a whole lot over 1.6:1. Even the rice in the foreground is
fairly low contrast. If one does the standard landscape on Velvia with
polarizer bit (that shot is Provia without), one doesn't get the contrast
from the specular reflections, and is left dealing with much lower
contrasts. It's the 1.6:1 performance that imposes the practical limits on
what I can get out of my film.

And I don't think my photography is particularly unique/perverse. Boring and
plodding I'm sure come more to mind.
Indeed that is often the case, but not with high quality optics.

I've tested all my Mamiya and Fuji 645 lenses, and even for my relatively
high contrast test scenes, I don't see any differences (observing with a 60x
microscope) from one stop down from wide open to f/16. As I've said before,
I can maybe persuade myself that f/22 is a tad softer.
The basic rule for the diffractive optical cut-off of a lens is 1/(W.f)
where W is the mean wavelength of the light (in the case of the visible
spectrum around 0.55um) and f is the f/# of the lens. However it
requires a very precise surface form to achieve the diffraction limit
and this becomes more difficult at large apertures, low f/#s, for two
reasons:
1. The diffractive limit is higher
2. The diameter of the optical aperture and the incident angle due to
the curvature of the lens surfaces are greater over that aperture.

In short, not only do you have to maintain precision over a greater area
of glass, but the level of precision required increases. That is why
you will often find lenses produce a "sweet spot" in resolution terms
around f/4-f/5.6 - where the diffraction limit actually reduces the
resolution more than residual design and manufacturing aberrations. A
good measure of the intrinsic quality of the lens is the f/# that sweet
spot occurs at - the lower the f/# the better the lens. Even budget
lenses manage sweet spots around f/8.

I'm quite aware of all that.
You need to measure the performance a lot better - the diffraction
limits of f/16 are clearly visible on most film.

My 60x microscope doesn't show that. With Provia 100F for real-life images.

However much I provide higher contrast targets for testing, real photographs
won't show any difference between f/11 and f/16. And certainly no difference
that's useful for imaging.
f/22 certainly is worse - I have already had this discussion several
times, including one poster on another forum who went so far as to buy
some Provia and post scans of his results to demonstrate I was wrong,
but then changed his argument to "not too much worse". I don't know if
his images are still available, I'll have a search and if they are I
will post the link in an update, but this was almost a decade ago.

Another issue is how does MTF change as one moves away from the plane of
focus. I suspect that what's going on here is that what we use for our
practical photography really isn't much over 30 lp/mm most of the time. Off
axis, normal to wide angle lenses crap out pretty badly even at 30 lp/mm and
f/8, and we actually use the off axis areas. And regions away from the plane
of perfect focus are obviously less contrasty as well.
You responded to my post about aliasing on scanned film - which
intrinsically includes the aliasing of the emulsions characteristics.

The post I thought I was responding to was, I thought, only concerned with
image content. And I tried to limit my comments to that. Again, I thought
the issue of concern was aliasing of image detail on the film, and that
still strikes me as a seriously unlikely problem.
In
my subsequent response to that I already agreed that in most, but not
all, cases your comments were correct in terms of the image content but
that was not the whole story because grain plays a significant effect
and its spatial frequencies certainly do alias.

OK. Fine. I get the content bit and you get the grain bit<g>.

It sounds, though, that including an antialiasing filter on the scanner CCD
would be a good idea.

But I bet most scanner users would scream bloody murder if mfrs started
doing that said:
Exactly, but that doesn't mean those frequencies which would alias have
been eliminated, merely reduce by the MTF of the total system.

Not total system: lens + film<g>. One problem with my counting pixels in
edges _in the scan_ is that that includes the scanner MTF.

But I thought I tried to hedge my comments concern only _visually
significant_ aliasing. I may be wrong here, but aliasing a component that's
been grossly attenuated* should be on the order of the noise. For aliasing
of image content to occur, on my scanner I'd have to have content at 80
lp/mm, and both lenses and film have rather painfully low MTFs at 80 lp/mm.
That goes up to 100 lp/mm for the Minolta.

*: The high-frequency components in the Fourier transform (of an edge) are
lower magnitude than the fundamental, they're attenuated by the lens, and
they're attenuated by the film. That's getting to be a lot of attenuation.
And optics, in fact almost all imaging processes, but again, unless the
MTF is actually zero (which does happen with optics, even ideal optics)
all frequencies are reproduced at some level. If some of these none
zero frequencies are above the Nyquist limit then they will alias - even
though the edge smears over several pixels.

Yes. But they are so grossly attenuated that they differ insignificantly
from the case were they not there.

Again, this is my basic rant: worrying about image detail at sky high (note
the informal term said:
For an explanation, read the text I wrote again!

You have to remember that when I write "no detail" I mean "no significant
detail". Sorry for the sloppiness.
This comes down to which spatial frequencies are present in an edge
transition and how well they are reproduced. Unless all of the spatial
frequencies are reproduced with the same response, the edge will change
its shape - reduce only mid spatial frequencies and the edge will ring,
reduce only low spatial frequencies and the edge will overshoot, remove
the fundamental frequency and the edge will have the same intensity on
either side, reducing all spatial frequencies as a function of the
frequency and the edge will smear. A smeared edge does not mean that
all spatial frequencies that could alias have been eliminated, it only
means that they have been attenuated more that the low frequencies.

Yes. But if you look at the amplitudes of the upper frequency components
(before attenuation) in the fourier series for an edge or square wave,
you'll note that they are of a far lower magnitude than the fundamental.
It's these lower magnitude signals, that are attenuated fist by the lens and
second by the film, that need to be present.
Unless those high frequencies have been eliminated then they will alias.

Sure. But alias so that they are significant? I've not seen it. Have you
been able to demonstrate image aliasing in the Minolta scanner? It should be
more of a problem in the Nikon 8000, but I haven't seen it. A lot of dSLRs
(D70, 1Ds) have inadequate antialiasing filters, and that is sometimes a
problem, but only in response to patterns that have a fundamental frequency
at or above Nyquist.
They may be less than the low frequencies (and certainly will be) due to
the MTF of the system, resulting in edge smearing, but that does not
mean that they have been eliminated. Unfortunately, high contrast, high
spatial frequency signals occur naturally all over the place - any
specular reflection you have ever seen is an example.

That's why landscape wannabes use polarizing filters. Which themselves are
another source of reduced MTF.
A low, but
non-zero, MTF at high frequencies will result in such image content
being reproduced on film and subsequently aliased by the scanning
system.

Sorry David, but that is simply BS. Random dots, by definition, have
*all* spatial frequencies present

Note that the "random dots" I'm talking about are dots _IN THE SCANNED IMAGE
NOT THE FILM_.
and thus contain out of band signals which certainly do alias.

Well, they would alias if you scanned the scan<g>.

David J. Littleboy
Tokyo, Japan
 
O

Ole-Hjalmar Kristensen

<lots of misconceptions about MTF snipped>

DJL> The post I thought I was responding to was, I thought, only concerned with
DJL> image content. And I tried to limit my comments to that. Again, I thought
DJL> the issue of concern was aliasing of image detail on the film, and that
DJL> still strikes me as a seriously unlikely problem.

I assume you were responding to my posting about fundamental problems
with film scanning. In the original post, I did not say anything about
whether the high-frequncy signal came from image content or grain
noise. In a follow-up, I made it completely clear that the higher
frquencies will be dominated by noise. But the source of this
high-frequency energy is irrelevant, it will reappear lower down in
the frequency spectrum thanks to the sampling process, unless you
filter ita away optically *before* the sampling. As steep optical
filters are hard to realize, you will either have to accept that your
4000 dpi scanner wil *not* have a flat MTF up to 4000 dpi, or you have
to accept aliasing. This design tradeoff has been done by the scanner
manufacturer, and unless you modify the optical path (like with the
Scanhancer or Grain Dissolver), you cannot do much about it.

DJL> OK. Fine. I get the content bit and you get the grain bit<g>.

DJL> It sounds, though, that including an antialiasing filter on the scanner CCD
DJL> would be a good idea.

DJL> But I bet most scanner users would scream bloody murder if mfrs started

DJL> Not total system: lens + film<g>. One problem with my counting pixels in
DJL> edges _in the scan_ is that that includes the scanner MTF.

DJL> But I thought I tried to hedge my comments concern only _visually
DJL> significant_ aliasing. I may be wrong here, but aliasing a component that's
DJL> been grossly attenuated* should be on the order of the noise. For aliasing
DJL> of image content to occur, on my scanner I'd have to have content at 80
DJL> lp/mm, and both lenses and film have rather painfully low MTFs at 80 lp/mm.
DJL> That goes up to 100 lp/mm for the Minolta.

As you can see through any microscope, there is plenty of signal
coming from grain boundaries at those frequencies. Whether you see
aliasing or not depends on the optical system of your scanner.

<snip>

DJL> David J. Littleboy
DJL> Tokyo, Japan
 
K

Kennedy McEwen

David J. Littleboy said:
Well, the published MTF curves certainly _predict the response incorrectly_
for low contrast targets.
No they don't - they present the MTF and that is independent of the
signal contrast. How you choose to interpret, or mis-interpret, the NTF
curve for your own use is your problem. Learn how to use the tool
before criticising it, I say!
The film is the measurement medium, and it's not responding. You can't
idealize away the noise: it's an inherent property of the medium. If a
section of your photograph has detail with 1.6:1 contrast _as projected on
the film_, then you won't see that detail.
Exactly, and I am not disputing that, although I do dispute your
suggestion that you are only concerned with source contrast in that
region. Your own results show final contrasts outside of that region
so, allowing for the MTF losses already identified, the source contrast
must have been significantly greater than you suggest.
Again, the complaint is that for the images I'm taking, I need low-contrast
performance. The theoretical MTF in response to a contrast 500 times more
than what I've got doesn't tell me what the film does in my images. The
signal that I get off the film has noise in it, and I don't have the option
of ignoring that noise.

And I am not suggesting anything different - every condition sets
limits, but understanding what those limits are and what secondary
effects they impose is just as significant. If, as you suggest (even
though I dispute it), that all of your source material is 1.6:1 contrast
and less then granular is, and always will be, your biggest enemy - and
that enemy will alias *very* significantly with both 2700ppi and 4000ppi
scanners.

I started by conceding you the image content, whilst pointing out that
the grain was also important - you seem to be intent in arguing that the
image is actually worth a lot less than my starting position on this.
;-)
??? I thought that the MTF was the contrast of the thing being measured. If
I'm measuring the medium, that's what I want to measure.
No - the MTF is the *relative* contrast between input and output (ie.
the *ratio* of output contrast to input contrast) of the medium, or
system comprising several media. MTF is *NOT* contrast, hence my
reference to the difference between the two in the previous quote! The
medium itself has no contrast - whether you wish to measure it or not.
Most of the signals we record on slide films in actual photography are areas
that fall in a fairly narrow range of zones. So the response that we
actually use and need to render our subjects (not just the edges) is the low
contrast response.
So why, if we are only interested in low contrast response, reduced even
further by lens MTF and film MTF, do we need scanners with 16-bit ADCs?
The contrast of the now obsolete 10-bit films scanner is 1000:1, and
with MTFs of camera lens, film, scanner lens, and scanner CCD summing up
to less than 5% for a significant part of the spatial frequency range,
that obsolete capability became saturated with 20,000:1 scenes!
Talking about the performance of a system abstracted away from the noise
seems very much the wrong thing.
Not at all - MTF is useful to determine the signal. The noise can be
determined from other parameters. It is quite common in sensor system
modelling to compute signal and noise completely independently and
combing them to create a signal to noise ratio - in fact I know of no
reputable analysis which does otherwise!
I doubt it. The shadows are lit by full open sky. That's a lot of light.

Shadows lit by open sky can only exist on the top of the units - the
shadows in your image have a significant range of levels. The higher
contrast in the digital image suggests that some of these are well below
1/1000th of the white levels after monitor gamma is taken account of.
Bart discussed this here before: it's really quite hard to create a 1000:1
contrast.
As I previously pointed out, if it was so difficult then we certainly
would not need the equipment, either film or scanner, that we do.
This argument is problematic because I don't really mean to say never: I
mean to say rare. Since low contrast is far more common, it's the low
contast performance of the film that I need to model.

I disagree - you need a film that copes with the extremes that you are
likely to throw at it. Any old muck can cope with the mundane - its the
stuff that copes better with the exceptions that gets the reputation for
performing.
Ah, I see the reason for the silliness: you've misunderstood what I'm trying
to say.
I don't think so - I see you repeating it several times in your
response!
Detail selected being low contrast, but still higher than your nominal
reference. The foreground detail, like all short range material, has
much less atmospheric attenuation and this much higher contrast.

Just in case you weren't aware, the atmospheric transmission attenuates
the highlights and elevates the shadows by scattering the available
illumination, such as ambient daylight.

For reference - two adjacent pixels in the foreground read RGB values of
189,195, 144 and 21,35,0. Combining these RGB values with a relativel
crude 1,2,1 weighting gives a gamma compensated contrast in excess of
8:1, and a linear contrast of over 40:1. Given the MTF of the system
components used, a source contrast approaching 1000:1 is not too far off
being present there in the example image that you chose to offer!
If I want to resolve the texture in the trees in a distant forrest, then the
contrast isn't a whole lot over 1.6:1. Even the rice in the foreground is
fairly low contrast.

Actually, from the figures presented above, it is close to and probably
even exceeds the figures that you claim never to encounter!
If one does the standard landscape on Velvia with
polarizer bit (that shot is Provia without), one doesn't get the contrast
from the specular reflections, and is left dealing with much lower
contrasts. It's the 1.6:1 performance that imposes the practical limits on
what I can get out of my film.
No it isn't - it is the MTF applied to all of the contrast present in
your image, not just those you care to assess.
I've tested all my Mamiya and Fuji 645 lenses, and even for my relatively
high contrast test scenes, I don't see any differences (observing with a 60x
microscope) from one stop down from wide open to f/16. As I've said before,
I can maybe persuade myself that f/22 is a tad softer.
Converse to conventional wisdom, large format lenses tend to be lower
performance than small format lenses. This happens for two key reasons.
Firstly, because they can get away with it, given the lower levels of
magnification of the film. Secondly because it is much harder to
maintain performance across the field, and it is generally preferable to
have a slightly inferior cross field performance than a cracking on axis
and poor edge performance. Your Mamiya lenses may well have sweet spots
down in the f/16 region - never getting any better with smaller f/#s -
however you will find 35mm optics considerably better, albeit over a
smaller area, and digital camera optics often even better still over an
even smaller area.
My 60x microscope doesn't show that. With Provia 100F for real-life images.
As mentioned earlier, you are looking at lens trade-offs which take
advantage of the larger format. Diffraction limit f/16 is only 10% at
100cy/mm, but f/11 is 33% and f/8 is 50%. If you see no difference then
clearly your lenses may be good as mid format optics, but they are
relatively poor in terms of 35mm and next to useless for small format
(3um pixel) digital media - where the small formats demand higher
performance, and would never have become acceptable without it.
Another issue is how does MTF change as one moves away from the plane of
focus.

Simple to compute - multiply the MTF with the FT of the circle of
confusion. That's the way MTFs work.
I suspect that what's going on here is that what we use for our
practical photography really isn't much over 30 lp/mm most of the time. Off
axis, normal to wide angle lenses crap out pretty badly even at 30 lp/mm and
f/8, and we actually use the off axis areas. And regions away from the plane
of perfect focus are obviously less contrasty as well.
A 30lp/mm upper limit would be abysmal on a 35mm format - even a flatbed
scanner would be able to discern the limitation of 1500ppi, so again yo
do tend to be considering the effect of mid format again, where the
larger sizes involved mean that depth of field is much more restricted
that the equivalent field of view small format lens. I have an 18mm
f/3.5 that is pretty extreme FoV on 35mm and certainly produces much
more than 30cy/mm on film. In fact, it is probably one of the sharpest
lenses I own at the upper and lower frame edge and although side edge
and corners do have noticeable fall-off, even they have significant MTF
at 30cy/mm.
OK. Fine. I get the content bit and you get the grain bit<g>.

It sounds, though, that including an antialiasing filter on the scanner CCD
would be a good idea.

But I bet most scanner users would scream bloody murder if mfrs started
doing that, though<g>.
I don't hear many Minolta 5400 owners screaming bloody murder about the
grain dissolver, which is just that, if a less than perfect example. I
accept that many flatbed users do scream about poor performance of their
units which incorporate anti-alias hyperCCDs, but I have yet to be
convinced that is not just cheap optics and a lack of understnading on
the user's part of what a properly sampled image looks like under
magnification. The whole point is that you don't see individual pixel
sized objects, but that is what the masses seem to expect, so they
complain that their scanners are poorly focussed.
Not total system: lens + film<g>. One problem with my counting pixels in
edges _in the scan_ is that that includes the scanner MTF.
It is the total system MTF that determines whether the image information
will alias, not just the lens + film.
The high-frequency components in the Fourier transform (of an edge) are
lower magnitude than the fundamental, they're attenuated by the lens, and
they're attenuated by the film. That's getting to be a lot of attenuation.
Their original amplitude is unimportant in terms of how they affect the
edge being smeared out, that comes down to how well they are reproduced
by the system.
Yes. But they are so grossly attenuated that they differ insignificantly
from the case were they not there.
Sadly that isn't always the case. I wish you were right, but it just
doesn't happen that much.
Again, this is my basic rant: worrying about image detail at sky high (note
the informal term<g>) lp/mm levels is barking up the wrong tree.
As stated right at the start of our debate, for image detail that is
often, but not always, the case - however image data isn't the full
story. Grain, drives you to higher resolutions to avoid aliasing issues
with very high source and final contrasts and, quite frankly, unless you
control grain at source before the image even reaches the sampling
sensor, that drives you to submicron sampling to ensure that all of the
potential aliasing signal is completely attenuated by the optical MTF.
Sure. But alias so that they are significant? I've not seen it. Have you
been able to demonstrate image aliasing in the Minolta scanner?

It is no secret that I don't have a Minolta scanner. ;-)
However I have produced aliasing on the Nikon LS-4000 in a couple of
real images. As I said some time ago though, it was the reduction in
grain aliasing that persuaded me to move to the higher 4000ppi
resolution from earlier Nikon scanners, rather than a marginal increase
in image resolution.
Note that the "random dots" I'm talking about are dots _IN THE SCANNED IMAGE
NOT THE FILM_.
In which case their fundamentals are not out of band, they are an
in-band alias of the originally out of band fundamental of the random
dots ON THE FILM! Nevertheless, depending on how you display the
scanned image, those final dots will have a certain amount of out of
band information too - otherwise they would not appear as dots, but
fuzzy splodges. ;-)
 
W

WD

What is the physical explanation for a diffuse light source acting as
a low pass filter? (as compared to a collimated light source)?

As an aside, it is interesting to note that the latest Imacon
'top of the line' scanner boasts a diffuse light source.


W
 
K

Kennedy McEwen

WD said:
What is the physical explanation for a diffuse light source acting as
a low pass filter? (as compared to a collimated light source)?
Basically, it comes down to how 'ordered' the rays incident on the
optical system are, meaning that the MTF of the lens is different when
measured under different illumination sources.

Collimated light acts as a partially coherent light source, the smaller
the source the more coherent it becomes, so collimated light from a
point source can be very coherent indeed - and before the days of
lasers, most coherent light sources were produced by collimating a point
source, which limited the available light intensity.

With a coherent source, the MTF of the lens is flat up to the optical
cut-off whilst, with an incoherent source, the optical cut-off doubles
but the MTF reduces almost linearly towards it, depending on the exact
shape of the optical pupil. For a square pupil, this reduction is
perfectly linear, for a circular pupil it reduces slightly faster but
then gradually flattens out just before reaching cut-off. Basically,
the shape of the MTF curve with an incoherent source is just the overlap
area as two pupils scan past each other.

Thus a collimated source illumination system has half of the limiting
resolution of an un-collimated one, but the contrast of any spatial
frequency reproduced within that band is much higher. At the optical
cut-off with coherent illumination, the perfect incoherent system would
have a lens MTF of less than 50%.

Consequently it isn't actually true that the diffuser acts as a low pass
filter, but in the range of spatial frequencies we are interested in it
does. This also explains why a highly collimated illumination system
from a small source such as an LED, has such a problem with grain
aliasing, reproducing the grain that is many times greater than the
Nyquist limit with minimal attenuation. High MTF isn't always a good
thing. ;-)
 
F

Fernando

With a coherent source, the MTF of the lens is flat up to the optical
cut-off whilst, with an incoherent source, the optical cut-off doubles
but the MTF reduces almost linearly towards it, depending on the exact
shape of the optical pupil. For a square pupil, this reduction is
perfectly linear, for a circular pupil it reduces slightly faster but
then gradually flattens out just before reaching cut-off. Basically,
the shape of the MTF curve with an incoherent source is just the overlap
area as two pupils scan past each other.

Kennedy, you should write a book on physics, optics and electronic of
digital imaging.
I stopped just 2 tests before graduating in electronic engineering and
now I write software for 2D barcode scanning, so I should have this
stuff very clear in my mind; still, the clarity of your expositions
really is outstanding.

Fernando
 
J

justintime

Fernando said:
Kennedy, you should write a book on physics, optics and electronic of
digital imaging.

Bad idea if he should decide to sell such a book. Money corrupts, just
look at how Ed treats his Vuescan customers.
 
K

Kennedy McEwen

Fernando said:
Kennedy, you should write a book on physics, optics and electronic of
digital imaging.
I stopped just 2 tests before graduating in electronic engineering and
now I write software for 2D barcode scanning, so I should have this
stuff very clear in my mind; still, the clarity of your expositions
really is outstanding.
Maybe one day I'll get a round tuit but, as I have said before, a book
has to be much more general than just specific points and issues.
Answering questions correctly is a lot easier than asking the right
questions to answer. I doubt anyone would pay for my muses. ;-)
 
W

WD

Kennedy McEwen said:
Basically, it comes down to how 'ordered' the rays incident on the
optical system are, meaning that the MTF of the lens is different when
measured under different illumination sources.

Collimated light acts as a partially coherent light source, the smaller
the source the more coherent it becomes, so collimated light from a
point source can be very coherent indeed - and before the days of
lasers, most coherent light sources were produced by collimating a point
source, which limited the available light intensity.

With a coherent source, the MTF of the lens is flat up to the optical
cut-off whilst, with an incoherent source, the optical cut-off doubles
but the MTF reduces almost linearly towards it, depending on the exact
shape of the optical pupil.
For a square pupil, this reduction is
perfectly linear, for a circular pupil it reduces slightly faster but
then gradually flattens out just before reaching cut-off. Basically,
the shape of the MTF curve with an incoherent source is just the overlap
area as two pupils scan past each other.

Thus a collimated source illumination system has half of the limiting
resolution of an un-collimated one, but the contrast of any spatial
frequency reproduced within that band is much higher. At the optical
cut-off with coherent illumination, the perfect incoherent system would
have a lens MTF of less than 50%.

Consequently it isn't actually true that the diffuser acts as a low pass
filter, but in the range of spatial frequencies we are interested in it
does. This also explains why a highly collimated illumination system
from a small source such as an LED, has such a problem with grain
aliasing, reproducing the grain that is many times greater than the
Nyquist limit with minimal attenuation. High MTF isn't always a good
thing. ;-)


So you are saying in fact that with an incoherent source the MTF
cutoff
actually is at a higher spatial frequency than with a coherent source,
but in the 'region of interest'
(spatial frequencies above Nyquist cutoff of CCD array)
there is an attenuation of spatial frequencies.

Another related question I have regards scattering effects.
For example the Callier effect, small trapped air bubbles
(peppergrain),
etc. Your above discussion made no differentiation regarding
scattering
vs. pure transmission/absorption. For example if there was an element
(say grain or tiny bubble), which corresponded to spatial frequencies
beyond the Nyquist freq. of the CCD array, your above explantion
compares
the effect of collimated vs. non-collimated light sources whether or
not
these elements absorb or scatter the light. How does this play into
the picture? Is it merely a matter of the resultant amplitude of the
nasty
spatial frequencies in question? (scattering element vs.
non-scattering element)


This is all very interesting. I have been playing around with a
diffuser
with a coolscan 5000 and have found in certain cases dramatic
improvements.
What surprises me is that scanner vendors are so slow to catch on.
Nikon seems not yet to have caught on, Minolta presumably has with the
5400,
Imacon in their latest and greatest top of the line scanner is touting
its diffuse light source.
I would guess that the increase in scan times from a marketing
perspective
explains part of it, but with such potential improvement (in certain
cases),
it still surprises me.
 
B

Bart van der Wolf

WD said:
Hi,

Wondering if anyone out there has done an MTF measurement with the Minolta
5400 both with and without the 'grain dissolver' enabled?

A somewhat belated response, yes I have.
The following link gives a graphical representation of the best MTF
curves I could produce so far:
http://www.xs4all.nl/~bvdwolf/main/foto/Imatest/SFR_DSE5400_GD.png

Please note that, of the dozens of scans at different focus positions,
a single scan without GD stood out from the rest. The more common
results for both GD and non-GD scans, which showed similar results,
were only slightly lower than the orange (GD) line with a Nyquist
frequency modulation response between 15% and 18%. By the way, this
modulation shows that (grain-)aliasing is a real risk for spatial
frequencies above 106 cy/mm. Of course, the modulation of the film
detail/graininess would need to be more than 55% at those spatial
frequencies to be visible in the combined result.

IMHO the major effect of the more diffuse light-source is a less
pronounced edge definition of dye/grain clusters, due to the more
diffuse shadow/diffraction effects. The Callier effect (Q factor) is
usually quite small (close to 1.0) for dye-based film, but more
important for opaque silver grain. Nevertheless, I find the
'Grain-Dissolver' very useful for both dye- and silver-based film,
with minimal impact or resolution, assuming good focus (which is more
difficult with a diffuse lighting), see:
http://www.xs4all.nl/~bvdwolf/main/foto/scan/se5400/se5400-5.htm .

Bart
 
F

Fernando

important for opaque silver grain. Nevertheless, I find the
'Grain-Dissolver' very useful for both dye- and silver-based film,
with minimal impact or resolution, assuming good focus

Hi Bart!
Seems like GD helps quite a lot with negatives.
I did not find visible improvements with my typical chromes (Velvia
100F, Astia 100F, Sensia-II 400), while I did find a drop in edge
sharpness.
My MTF values lowered with GD when I performed some SETs. In
particular, I see a drop of about 8-10% of MTF50 values, and a drop of
about 25-30% of the MTF @ Nyquist value.
Now I try avoiding GD (and also ICE, unfortunately, being linked
within MSU) whenever possible...
Your results suggest me I should try some tests on BW film (I happen
to scan some TMAX 35mm strips).

Bye!

Fernando
 
B

Bart van der Wolf

SNIP
Well I'll start by saying that I don't have a Minolta scanner
or the Grain Dissolver to test, but the whole principle behind
the grain dissolver is that it reduces the MTF, particularly the
MTF above the Nyquist of the sampling frequency, ie above
about 100cy/mm.

I tend to disagree. IMHO it is the more diffuse shadow of a
three-dimensional dye/grain cluster that reduces its (edge)
visibility. That has also been the goal in traditional darkroom film
processing and enlargement, with the additional effect on density
dependent contrast in silver-based films. The limitation of
frequencies beyond Nyquist is determined by grain(-cluster) size
versus sampling density, a characteristic of scanner+film.
The grain dissolver is *NOT* intended to reduce or eliminate
grain - it is intended to reduce and/or eliminate grain aliasing.
Aliasing occurs because the MTF of the CCD and the optics
are greater than zero above the Nyquist frequency of the
sampling system.

It is required for the combined scanner (lens+CCD) *and* film MTF to
be below 10% response for visibility. That of course implies that
contrast stretching and/or sharpening requires an even lower MTF
response to avoid visibility.

SNIP
One simple way of achieving this is to defocus the lens in the
scanner, ensuring that the MTF above Nyquist is attenuated to
a level where aliasing is eliminated.

Yes, however, it would be more efficient to attenuate spatial
frequencies above Nyquist (before capture), or boost (sharpen)
frequencies below Nyquist (after capture).

SNIP
It still surprises me how many people think a single pixel
standing out from the background indicates a sharp image,
when all it really indicates is a grossly undersampled image
where aliasing abounds.

Indeed, but it requires a Don Quixote kind of approach to educate the
majority,
reporting for duty...

Bart
 
B

Bart van der Wolf

Kennedy McEwen said:
Silhouetted backlit objects can easily exceed contrasts of
1000:1 by several orders of magnitude.

Correct, and that translates to an even higher (film gamma > 1.0)
density difference in slide film (lower film gamma in most negative
films) which is what is presented to the scanner.

SNIP
It's a lot of lines, but still a long way below the diffraction
limit of the optics. At f/8, where all but the cheapest optics
are close to diffraction limited, the MTF is around 20% at
170cy/mm, a quality optic might be diffraction limited at
around f/4 - giving an MTF of 57% at the same resolution.

Quite so, that's why the 'analog imaging based' literature/test
targets of the previous century ;-) allowed to test 250+ lp/mm.
Still, looking at some Reala scans on the disk here, the edge
transitions are on the order of 3 pixels with clearly intermediate
values, which isn't bad and better than the 4 or 5 in 100F
scans. But it's nowhere near aliasing.
Again, you are referring to the *image* content, which may well
have little or no aliasing contribution.

Indeed, the combined performance of lens and film/sensor is important
to notice.

Bart
 
B

Bart van der Wolf

SNIP
My MTF values lowered with GD when I performed some
SETs. In particular, I see a drop of about 8-10% of MTF50
values, and a drop of about 25-30% of the MTF @ Nyquist
value.

Focussing (across the film area) becomes an issue. Focussing on a
small area of film indicates to me that the GD doesn't have enough
impact by itself.

Bart
 

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