Format Article
without images
with images
MODERN MICROSCOPY JOURNAL
Pixel Array Size Needed to Replace Photomicrographs on Film
Ted Clarke, Scientific Photographer and Instrument Maker
Sunday, February 01, 2004
INTRODUCTION
Some of you may have read previous articles by me
in “Microscopy Today” and know that I am a strong proponent of digital
imaging for photomicrographs and photomacrographs. I require that the
digital images match the resolution and field size of traditional film
images, with the 4X5 Polaroid film most commonly used in metallurgical
laboratories where I worked before early retirement. My development of
an affordable universal student microscope for home microscopy resulted
in a need for color digital images that would meet my requirements at
a reasonable cost. This need was met by recording on 35 mm film with subsequent
scanning of selected film images to a Kodak Master Photo CD. More recently
I purchased a CanoScan FS2710 film scanner for digitizing my family’s
collection of slides and negatives for saving on CD’s. This article will
review how I arrived at my requirements and how well they were met by
digital cameras and by film scanning.
MICROSCOPE RESOLUTION
The definition of the spatial resolution of the microscope
begins with the diffraction pattern image of two nearly adjacent point
sources of light formed through a circular aperture. The point sources
are separated in object space so that the first minimum of one pattern
coincides with the central maximum of the other diffraction pattern.
This is the Rayleigh criterion of resolution. The image of these two point
sources is the sum of the two pattern intensities as shown in Figure
1.
Recording a straight line series of overlapping Airy discs at the
Rayleigh limit with a CCD would require at least two pixels per Airy disk
with the pixels centered on the central maximum and first minimum corresponding
to a pixel size of one fourth the Airy disc diameter. The delta Y separation
in the image can be related back to the separation of the point sources
in object space through the application of Abbe’s sine condition for a
lens free of spherical aberration; this is the objective lens resolution
given in Figure 2.
FIELD SIZE
The recording of photomicrographs requires consideration
of the field size limitations of the microscope. The compound microscope
optics produce an intermediate image which was conventionally enlarged
for viewing with a 10X eyepiece and projected with 10X enlargement for
recording on 4X5 film or with 2.5X enlargement for recording on 35mm film.
Until recently the intermediate field size was limited to about 18mm.
Modern research microscopes may now have an intermediate field size as
large as 26mm in diameter as shown in Figure 3. The
size of the rectangle in the intermediate image enlarged to form the photomicrograph
is important in determining the physical size of the CCD array and relay
lens magnification for digital recording. The intermediate field size
traditionally recorded on 4X5 film is an 8.9X11.4mm rectangle as shown
in Figure 3. Recording a 17.8X17.8mm square format image
from the 26mm intermediate image diameter would make good use of the modern
optics when necessary.
FINAL PRINT RESOLUTION
Resolution of the final photomicrograph is rarely
mentioned in quantitative terms. The viewing and recording optics of
the light microscope have been consistant with Abbe’s definition of usefull
magnification, which is related to the resolving ability of normal vision
when the photomicrograph is viewed from 250mm. Images from the lower
power objectives generally meet an Abbe magnification criterion of 500X
the NA of the objective. An Abbe criterion of 1000X the NA is commonly
used with the highest power objectives so that the finest detail resolvable
by the objective can be easily seen when higher NA is not available.
Images from the lower power objectives place more demand on the resolution
of the film or CCD, as indicated in the analysis given in Figure
4. Assuming a traditional 10X enlargement of the intermediate
image to achieve photomicrograph resolution of between 6 and 3 line pairs
per mm, the intermediate image resolution ranges between a corresponding
60 and 30 line pairs per mm.
PIXEL ARRAY SIZE REQUIREMENT
A minimum pixel array size that is needed to achieve
6 line pairs per mm resolution in the image area of a 4X5 Polaroid film
print is derived in Figure 5. The calculation agrees
well with the now widespread use of 1280X1024 through 1600X1200 pixel
CCD cameras for scientific imaging. The calculation assumes that the
three-color values for each pixel are not interpolated as with consumer
product cameras having a color mosaic filter pattern over the pixels,
which reduces spatial resolution by at least 30%. Non-interpolated pixel
values can be obtained by many approaches. The most common non-interpolated
color capture is by sequential capture of red, green and blue images using
a color filter wheel or tunable liquid crystal filter. Film scanners and
some color digital cameras record the image by scanning the optical image
with a red, green and blue filtered trilinear array.
RESOLUTION TEST PATTERNS
Measuring the resolution capability of a digital
camera or film scanner for photomicrographs ideally requires a microscope
resolution test slide. The lowest magnification objective is commonly
a 5X 0.10 NA (4X 0.10 NA used with a 1.25X tube factor in some Zeiss microscopes).
This lens should resolve 300 line pairs per mm in object space forming
an intermediate image with 60 line pairs per mm resolution. A 3X3” chrome
on glass resolution test chart with patterns from ¼ line pair per mm to
600 line pairs per mm is available and quite costly. I previously used
this test chart with a 0.10 NA Zeiss objective and verified the theoretical
resolution with both the MegaPlus 1.6i/AB digital camera and recording
on Polaroid Type 55 film. Low cost test patterns with a small field
size with line patterns covering a range of 300 to 3000 line pairs per
mm could be made by electron lithography but are not available because
of lack of market demand. An alternative test method is to use a high
resolution macro lens on the camera to image a pattern like the NBS Microcopy
Resolution Test Chart in the 89X114 mm field size of a 4X5 Polaroid film
print for a 1280X1024 pixel CCD sensor (89X133 mm field for a 1534X1024
CCD sensor or film scan of 35 mm format) as done for Figures 6
& 7.
DIGITAL CAMERA AND KODAK PHOTO CD RESOLUTION
The test result for the Mavica camera demonstrates the
significant loss in spatial resolution due to the color mosaic filter over the
CCD sensor when compared with the grayscale capture by the MegaPlus camera.
The pattern results with the MegaPlus camera demonstrate that line patterns
oriented orthogonal to the pixel array are more difficult to record without an
alias line problem. The alias lines are a moiré fringe effect from close
alignment of the pixel spacing with the line patterns in the optical image when
the spatial frequency of the line patterns approach the pixel spacing. The
moiré effect was accentuated with the MegaPlus results because the original
images were high pass filtered to improve the apparent resolution. The
position of the test pattern during imaging was purposely adjusted to avoid
this effect for the orthogonal orientation of the 5.6 line pairs per mm
pattern. The orthogonal patterns from the Photo CD scans show less evidence of
this effect, perhaps mainly because they were not sharpened. The solution to
the alias line problem is to capture the same image with a larger number of
pixels. Since my home microscope and the older Zeiss Universal microscope I
used before retirement have a maximum intermediate image field diameter of 18
mm, a 1534X1024 pixel array meets my requirements for resolution and field
size. The 3000X2000 pixel resolution result indicates that the 35 mm film to
digital method using this Kodak Photo CD file size cropped to 2048X2048 pixels
should be adequate to cover an 18X18 mm portion of a 26 mm intermediate image
field diameter for those fortunate enough to own a modern research microscope.
The 11 line pair per mm pattern just resolved in the 3000X2000 pixel file
corresponds to 40 line pairs per mm in the film image. The blurring effect of
limited film resolution is showing up at this higher spatial frequency.
CANON FILM SCANNER RESOLUTION
Film scanners for use with fast PC’s with 8 megabyte
graphics cards, 1600X1200 pixel monitors and CD writers are now affordable
for home use. I have a large collection of family 35-mm slides and negatives
and wanted to digitize them with storage on CD’s for distribution to the
younger members of the family so their past will not be lost. The cost
savings of owning my own film scanner versus having the film images scanned
to Kodak Master Photo CD’s justified purchase of a Canon CanoScan FS2710
film scanner. A maximum resolution scan for this scanner is 3888X2720
pixels. This pixel array size is not adequate to record the finest spatial
frequencies in very high quality slides and negatives, but should achieve
about 52 line pairs per mm resolution. Some 35 mm film images exceed
63 line pairs per mm resolution. The need to digitize the highest spatial
frequencies on 35 mm film was met by the Kodak Professional Photo CD 6000X4000
pixel scans. Film scanners with this resolution are now available, but
quite expensive for home use. Owning the CanoScan film scanner is a big
advantage for my low budget, home microscopy. I can record on 35 mm color
negative film and use locally available 1 hour processing of the film
prior to scanning it at home. Scanning the negatives rather than photographic
prints from the negatives avoids the problem of variable print quality,
which the mass market probably would not notice. The disadvantage is
that I have to bracket my exposures to be sure of a good film image to
scan. Naturally I have compared the resolution of the Canon scanner,
using the same resolution test slide, with the Kodak Photo CD results
in Figure 6. The finest pattern on the NBS test chart
just resolved on the film is 14 line pairs per mm pattern corresponding
to 51 line pairs per mm on the slide. PhotoShop LE comes with the scanner
software and was used to downsize the large file size to 1940X1360 and
1534X1024 pixel files. A photomontage of the finest patterns in these
files is shown in Figure 7. It is important to note
that the other than 2:1 downsizing used to obtain the 1534X1024 pixel
file introduces noticeable alias line artifacts less evident than in the
Photo CD result shown in Figure 6. The 30% loss in spatial
resolution resulting from use of a CCD camera with a Bayer color mosaic
filter, such as the Nikon Coolpix 995, can be compensated by doubling
the number of pixels used to capture the same image field; this is shown
in Figure 8. The bicubic resampling procedure of PhotoShop
can then be used to maintain the spatial resolution using half the number
of pixels. This step is equivalent to reducing the empty magnification.
SUMMARY
Film-to-digital and direct digital capture, with
a digital camera, can clearly be acceptable methods for obtaining high
quality digital photomicrographs that match the field size and resolution
of traditional photomicrograph prints. Unfortunately there are no national
or international standards dealing with this important transition in technology.
The Photographic and Imaging Manufacturers Association (PIMA) is participating
in an ISO TC42 effort to develop such standards. Their preliminary efforts
concentrate on using a resolution test pattern of their own design and
alias effects are considered. Alias effects are inherent in the digital
capture, but should not be worsened in subsequent image downsizing and
desktop publishing. Understanding the operating principles of the light
microscope and using them to obtain an optimum optical image for recording
is vital for quality digital images. Unfortunately the users who think
software can “fix” the resulting defects in their images do not appreciate
this requirement.
REFERENCE
Clarke, T. M., “Digital
Imaging in the Materials Engineering Laboratory,” THE MICROSCOPE, 1998,
46(2), 85-100.
Clarke, T. M., “Building
an Affordable Universal Student Microscope,” THE MICROSCOPE, 2000, 48(1),
19-39.
K. D. Moller, OPTICS,
University Science Books: Mill Valley, Ca., 1988.
Edwards, Parulski, &
Holm, “Setting Standards--Developing Standards in Electronic Imaging”,
PEI, February 1998, 48-52.
|