Fluorescence, confocal and related techniques

About this technique


Fluorescence microscopy

Fluorescence microscopy illuminates the sample through the objective lens, with short wavelength light, which will excite a fluorescent dye, or fluorochrome. The fluorochrome will emit light at a longer wavelength and a wavelength-selective dichroic mirror in the optical path will let this light travel to the eyepieces or camera. Typically excitation is with near-ultraviolet, blue or green light, and emission is respectively in the blue, green or red. Some samples are naturally fluorescent but most will need to be stained. There are three approaches to fluorescent staining:

Confocal microscopy

A confocal microscope scans the sample with a spot of light in a regular ‘raster’ pattern and so acquires an image point by point. The end result, on this basis, is no different from the image given by a regular microscope. But because only one point is acquired at a time, we can place a pinhole where the spot is imaged, and so eliminate out of focus light. Light that is in focus will be a small spot and will pass through the pinhole, but out of focus light will be a fuzzy blob and will mostly be blocked. This enables true three-dimensional imaging. To get enough light in one point, a laser is usually the illumination source. 

Confocal microscopes can be operated in reflection mode – typically for surface profiling, but in the life sciences they are more often used in fluorescence mode, where out of focus glare can be a major problem. Typically, one uses a confocal microscope either to collect a three-dimensional set of slice images, or to image a single layer in cases where strong surrounding fluorescence would spoil the image in a conventional fluorescence microscope. 

In confocal microscopy one needs to bear in mind that there are only a few, discrete, laser lines for illumination and the stain must be chosen to suit. Excitation (except in some special cases) is only in the visible range, with 405 nm (deep violet) the shortest wavelength available. Also, correct matching of mounting medium, coverslip and objective becomes critically important for 3-D imaging. Specific techniques such as FRET, FRAP, FLIM, FCS/RICS and TIRF are available to address more defined questions and are dealt with separeately

Multiphoton microscopy

Multiphoton microscopy is essentially an extension of confocal imaging. Very short, intense pulses of light in the near infrared are used for illumination and fluorescence is excited when two photons hit the fluorochrome molecule simultaneously, and behave as one photon of half the wavelength. The intensity of a single pulse is very high, but the spaces are much longer than the pulses, so that averaged over time the irradiation is comparable to confocal microscopy. Since two-photon events will only take place at the focus of the excitation spot, optical sectioning is automatic without any confocal pinhole. This means that detection can be made more efficient, particularly in a scattering sample, and it also means that that there will be no bleaching above and below the focal plane.

The longer wavelengths used in multiphoton imaging penetrate better into thick samples, and are also less damaging to living cells, than the wavelengths used for conventional fluorescence. Other key benefits are the ability to excite fluorochromes such as DAPI and calcium ratio dyes which would normally require near UV, and a wide wavelength selection since the lasers used can be tuned through the range 700–1000 nm. 

Second harmonic generation

Certain substances have the ability, when excited by strong pulses of light, to generate the second harmonic – that is, light of twice the frequency (hence half the wavelength). Typically these are molecules with no centre of symmetry, and the more highly crystalline they are the stronger the effect. In biological samples collagen, starch and myosin are all candidates. This means that they can be imaged without any staining or labelling, and since it is a purely physical process there is no fading. The microscope setup is just as for multiphoton imaging, and both can be done at once.

References

Output examples

[confocal_01_TF.jpg]
Confocal image of cancer cells stained by using three different labels.
[confocal_02_TF.jpg]
Confocal image of cancer cells in a collagen matrix.
[SHG_01_TF.jpg]
Second harmonic image of starch (blue) in living moss leaf combined with two-photon fluorescence imaging of chlorophyll (red) and phenolics (green).


Contact an expert

The University of Sydney
Ms Ellie Kable
T: 02 9351 7566
E: eleanor.kable@sydney.edu.au

The University of Western Australia
Mr John Murphy
T: 08 6488 8070
E: john.murphy@uwa.edu.au

The Australian National University
Mr Daryl Webb
T: 0427 553 182
E: webb@rsbs.anu.edu.au

James Cook University
Dr Kevin Blake
T: 07 4781 4864
E: kevin.blake@jcu.edu.au

CSIRO
Dr Adam Costin
T: 03 5227 5209
E: adam.costin@csiro.au

UTS
A/Prof. Louise Cole
T: 02 9514 3149
E: Louise.Cole@uts.edu.au

SARF – Flinders University
Mrs Pat Vilimas
T: 08 82044858
E: pat.vilimas@flinders.edu.au

SARF – The University of Adelaide
Dr Jane Sibbons
T: 08 8313 5207
E: jane.sibbons@adelaide.edu.au