Confocal Microscopy
The big idea of a confocal microscope is to illuminate and
image a sample just one spot at a time. A complete two-dimensional
image is then built up by scanning, in other words illuminating
and imaging row upon row of individual spots in a plane. The
resulting image is then a "slice" through the sample,
typically at a distance of a few microns into the sample.
It's possible to get some really clear images this way, and
to use sets (or stacks) of slices at different depths to build
a three-dimensional picture of the sample.
Below is a schematic of how a confocal microscope works:
The
light source that illuminates the sample is the laser at the
top of the picture. The fine laser beam (blue line) travels
to the sample via a beamsplitter, then two scanning mirrors,
and finally the actual microscope lenses. Those scanning mirrors
are a key ingredient. Each mirror twists about its axis very
rapidly, deflecting the laser beam. One mirror is responsible
for scanning the light one way across the sample. The other
mirror scans the light beam at right angles to the first,
so that a complete region of the sample is illuminated.
Light reflected by the illuminated portion of the sample
(green line) passes back through the lenses and mirror, through
the beamsplitter and into the detector. Each sweep of the
sample by the illuminating beam gives a corresponding image
of the sample in the detector. Crucially, the illuminating
light and the image pass through the same microscope optics
- so where the laser is focused on the sample, the imaging
optics (being one and the same) are focused too.
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| Rendered three-dimensional image of an aggregated emulsion |
There are a couple more magic ingredients. Imagine the illuminating
laser beam is focused some way into the sample, as is usually
the case in confocal microscopy. Then although the brightest
illumination is at the focus, regions of the sample immediately
before and after the focus will also be lit up and will also
reflect light. But these regions will not be in focus, and
so would make the final image fuzzy. Light from these regions
needs to be removed, and this task is performed by the pinhole,
shown in the diagram close by the detector.
The pin hole is located such that light from the spot of
interest is focused exactly on the pin hole, so passes through
and on to the detector beyond. However light from a point
deeper into the sample, say, will be focused in front of the
pinhole, and will have begun to spread out again by the time
it reaches the pin hole. Being too spread out by the time
it reaches the pin hole, most will not make it through. A
similar fate befalls light emanating from points not far enough
into the sample. So the pinhole filters out light coming from
points above and below the plane of interest.
The final trick is to use a special dye added to the sample
which, when illuminated by one colour of light, will fluoresce
and emit light of a different colour. For example the dye
Nile Red will give off red light when illuminated with blue
laser light. The illuminating blue laser light enters the
system via a "dichroic beamsplitter", which acts
as a mirror for high frequency light (eg blue) but like a
window for low frequency light (eg red). So the beamsplitter
diverts the laser light into the system, but the red light
returning to it merely passes through and on to the detector.
Confocal microscopes are really useful if you want to look
into a sample instead of at its surface, for creating clear
images, and for building three-dimensional images. They are
widely used in biology, for example. Typically, a confocal
microscope is mounted vertically above the sample, looking
down into it. In our work we are interested in the role of
gravity, so we have arranged our microscope to view the image
sideways on, which is pretty unusual.
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