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First published online May 14, 2007
doi: 10.1242/10.1242/jcs.03433
Cell Science at a Glance |
Life Sciences Complex Imaging Facility, Department of Biochemistry, McGill University, Montreal, Canada, H3G 1Y6
e-mail: claire.brown{at}mcgill.ca
| Introduction |
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With the complexity of modern fluorescence microscopes there is an endless number of possible set-ups and image acquisition settings. Here, I highlight common pitfalls encountered when performing fluorescence microscopy and discuss how to avoid them. Interested readers can consult in-depth technical reviews and books on various aspects of fluorescence microscopy for more information (Conchello and Lichtman, 2005
; Goldman and Spector, 2005
; Herman and Tanke, 1998
; Hibbs, 2004
; Lichtman and Conchello, 2005
; Muller, 2005
; Murphy, 2001
; North, 2006
; Pawley, 2006
). Numerous interactive web-based resources are also available; Molecular Expressions (http://micro.magnet.fsu.edu/), Nikon Microscopy U (http://www.microscopyu.com/), and Olympus Microscopy Resource Center (http://www.olympusmicro.com/).
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| Experimental set up |
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Fluorophore saturation
The general belief is that more light produces higher-contrast images. This is true to a point but if laser powers are excessively high essentially all of the fluorophores within the focal volume will be excited, leading to excited-state saturation. Adding additional light does not increase signal intensity in the plane of focus, but more out-of-focus fluorophores will be excited, resulting in poorer z-axis resolution and increased photobleaching/phototoxicity. In general, it is advisable to start at the lowest laser power possible, with a higher photo-multiplier tube (PMT) voltage (>600 V) and gradually increase the laser power as required. Line averaging using faster scan speeds, for example sampling a pixel four times for one-quarter of the time and averaging, generates images with a better signal-to-noise ratio because signal builds while noise averages out.
| Image acquisition |
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Confocal images can have very small pixel sizes (
10 times smaller than CCD cameras), but using high numerical aperture objectives, making pixels smaller does not always add resolution because objects that are smaller than the wavelength of light (e.g. 488 nm) cannot be resolved. At higher zoom settings, pixels are smaller and more data points are collected, making image files larger, but the specimen is oversampled and additional structural information not attained. For visible light and high numerical aperture objectives (>0.8) a pixel size of
0.1-0.2 µm is ideal.
Offsets and detector saturation
Confocal microscopes have a software offset setting and users are trained to set the background of images to `black' (i.e. zero). However, if the background intensity is set too dark, low intensity cellular details can be lost. These features are maintained when correcting high intensity background images post acquisition. Offsets can lead to grave quantitative errors. For example, if there are two points in an image with 200 and 100 intensity units, then one is 100% brighter. However, if the offset is set at 50 then the two points are now at 150 and 50 intensity units and one is 300% brighter. Offset errors will propagate when comparing intensities of multi-labelled samples or calculating image ratios. When imaging no pixel should measure zero intensity; however, it is critical to subtract the average background intensity before performing quantitative analysis.
Similarly, if laser powers, lamps, PMT gains or camera exposures are set too high, detectors can be saturated and features within images can be lost. Most software programs offer a high/low or range finder look-up table (LUT) where blue pixels read zero intensity and red pixels are saturated. The image acquisition parameters should be set so that no detection channel shows pixels reading zero or saturated levels.
Software settings and image display
In general it is best to use the full dynamic range of the detector. This means for an 8-bit detector use all 256 intensity levels (use 4096 for a 12-bit detector). Increasing the brightness of the excitation light (lamp or laser), the detector sensitivity (gain), or the camera exposure time (decreasing scan speeds for LSM) can ensure that the fluorescence signal is bright enough to nearly saturate the detector. However, less excitation light and shorter exposure times (or faster scan speeds) are better for imaging live cells or dim samples because phototoxicity/photobleaching is reduced. A common problem with imaging software is the image display settings default to displaying the full detector dynamic range with a linear relationship between the image and display intensities. For example, using an 8-bit detector there are 256 intensity levels but when imaging a dim sample maybe only 64 of these levels will be used. The data will only occupy the lowest 25% of the display intensities; the rest of the levels will be empty and the image will appear dark. The information required may be present in the image and visualised simply by adjusting the display settings. Other programs default to a `min/max' or `autolevels' display so that dim images appear bright on the screen. This is fine for visualisation but the sample may not be as bright as it appears and samples of very different brightness will appear similar. There is often an `autoexposure' setting in the software that automatically adjusts the exposure time to use the full detector dynamic range. This setting is most useful for fixed cells or as a starting point for live cells. In general it is important to know how the software is displaying the images and to look at the numeric values of the pixel intensities.
Most sensitive and quantitative scientific detectors are monochromatic and multi-colour images are generated using filters to separate various colours. Monochromatic images are then pseudo-coloured by the imaging or post-acquisition software. The colour coding of images is defined by a LUT that defines what display colour a given intensity will correspond to. Grey-scale images are displayed from black to white over 256 (8-bit display) grey levels. In turn, images could be displayed from black to green (or any colour) with 256 green levels. It is best to display images in grey scale whenever possible, but if colour is used keep in mind that the human eye is most sensitive to green light; so green images reveal more detail than blue or red. In addition, the eye only distinguishes up to about 100 grey levels even if 256 levels are displayed. Rainbow or spectrum look up tables show even higher contrast by using multiple colours to represent different intensity values (0-25 intensity units could be shades of purple, then 26-50 intensity unit shades of blue etc.). 3D plots of images are available in many software packages and can reveal more subtle differences in intensity, but can be difficult to fully interpret. For colocalisation figures it is best to show each image in grey scale with indicators pointing out common features and only show overlays in colour.
Dim features, such as the lamellipodia or cell edge, can be enhanced by modifying the display to a non-linear LUT using the gamma factor. Changing image brightness or contrast alone is not as effective because bright structures will be saturated when trying to emphasise dim ones. Display settings do not change the underlying data, however, these manipulations should be mentioned in figure captions. Finally, as always, care must be taken with any image manipulation that the data are not being misrepresented (Rossner and Yamada, 2004
) and see the JCS instructions for authors (http://www.biologists.com/web/submissions/jcs_information.html).
| Acknowledgments |
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| References |
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Bolte, S. and Cordelieres, F. P. (2006). A guided tour into subcellular colocalization analysis in light microscopy. J. Microsc. 224, 213-32.[Medline]
Comeau, J. W., Costantino, S. and Wiseman, P. W. (2006). A guide to accurate fluorescence microscopy colocalization measurements. Biophys. J. 91, 4611-4622.[CrossRef][Medline]
Conchello, J. A. and Lichtman, J. W. (2005). Optical sectioning microscopy. Nat. Methods 2, 920-931.[CrossRef][Medline]
Goldman, R. D. and Spector, D. L. (2005). Live Cell Imaging: A Laboratory Manual. New York: Cold Spring Harbor Laboratory Press.
Graf, R., Rietdorf, J. and Zimmermann, T. (2005). Live cell spinning disk microscopy. Adv. Biochem. Eng. Biotechnol. 95, 57-75.[Medline]
Hanley, Q. S., Verveer, P. J., Gemkow, M. J., Arndt-Jovin, D. and Jovin, T. M. (1999). An optical sectioning programmable array microscope implemented with a digital micromirror device. J. Microsc. 196, 317-331.[Medline]
Helmchen, F. and Denk, W. (2005). Deep tissue two-photon microscopy. Nat. Methods 2, 932-940.[CrossRef][Medline]
Herman, B. and Tanke, H. (1998). Fluorescence Microscopy: Springer.
Hibbs, A. (2004). Confocal Microscopy for Biologists: Springer.
Lichtman, J. W. and Conchello, J. A. (2005). Fluorescence microscopy. Nat. Methods 2, 910-919.[CrossRef][Medline]
Muller, M. (2005). Introduction to Confocal Fluorescence Microscopy: Spie Press.
Murphy, D. (2001). Fundamentals of Light Microscopy and Electronic Imaging: John Wiley & Sons Canada, Ltd.
North, A. J. (2006). Seeing is believing? A beginners' guide to practical pitfalls in image acquisition. J. Cell Biol. 172, 9-18.
Pawley, J. (2006). Handbook of Biological Confocal Microscopy: Springer.
Rossner, M. and Yamada, K. M. (2004). What's in a picture? The temptation of image manipulation. J. Cell Biol. 166, 11-15.
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