- Fluorescence microscope
A fluorescence microscope is an optical microscope used to study properties of organic or inorganic substances using the phenomena of fluorescence and phosphorescence instead of, or in addition to, reflection and absorption. The "fluorescence microscope" refers to any microscope that uses fluorescence to generate an image, whether it is a more simple set up like an epifluorescent microscope, or a more complicated design such as a confocal microscope, which uses optical sectioning to get better resolution of the fluorescent image.
All fluorescence microscopy methods share the same principle. A sample is illuminated with light of a wavelength which causes fluorescence in the sample. The light emitted by fluorescence, which is at a different, longer, wavelength than the illumination, is then detected through a microscope objective. Two filters are normally used in this technique; an illumination (or excitation) filter which ensures the illumination is near monochromatic and at the correct wavelength, and a second emission (or detection) filter which ensures none of the excitation light source reaches the detector. Fluorescence microscopy takes a fundamentally different approach to generating a light microscope image compared to transmitted or reflected white light techniques such as phase contrast and differential interference contrast microscopy. These two contrasting optical microscopy methods give very different but complementary data.
- 1 Principle
- 2 Light sources
- 3 Sample preparation
- 4 Limitations
- 5 Improvements and sub-diffraction techniques
- 6 Fluorescence microscope gallery
- 7 Fluorescence micrograph gallery
- 8 See also
- 9 References
- 10 External Links
The specimen is illuminated with light of a specific wavelength (or wavelengths) which is absorbed by the fluorophores, causing them to emit light of longer wavelengths (i.e., of a different color than the absorbed light). The illumination light is separated from the much weaker emitted fluorescence through the use of a spectral emission filter. Typical components of a fluorescence microscope are a light source (xenon arc lamp or mercury-vapor lamp), the excitation filter, the dichroic mirror (or dichroic beamsplitter), and the emission filter (see figure below). The filters and the dichroic are chosen to match the spectral excitation and emission characteristics of the fluorophore used to label the specimen. In this manner, the distribution of a single fluorophore (color) is imaged at a time. Multi-color images of several types of fluorophores must be composed by combining several single-color images.
Most fluorescence microscopes in use are epifluorescence microscopes (i.e., excitation and observation of the fluorescence are from above (epi–) the specimen). These microscopes have become an important part in the field of biology, opening the doors for more advanced microscope designs, such as the confocal microscope and the total internal reflection fluorescence microscope (TIRF).
The majority of fluorescence microscopy, especially in the life sciences, is epifluorescence microscopy. The excitatory light is passed from above (or, for inverted microscopes, from below), through the objective lens and then onto the specimen instead of passing it first through the specimen. The fluorescence in the specimen gives rise to emitted light which is focused to the detector by the same objective that is used for the excitation. Since most of the excitatory light is transmitted through the specimen, only reflected excitatory light reaches the objective together with the emitted light and this method therefore gives an improved signal to noise ratio. An additional dichroic filter between the objective and the detector can filter out the remaining excitation light from fluorescent light.
Fluorescence microscopy requires intense, near-monochromatic, illumination which some widespread light sources, like halogen lamps cannot provide. There are two main types of light source used; xenon arc lamp or mercury-vapor lamps with an excitation filter and lasers. Lasers are most widely used for more complex fluorescence microscopy techniques like confocal microscopy and total internal reflection fluorescence microscopy while xenon and mercury lamps with an excitation filter are commonly used for widefield epifluorescence microscopes.
In order for a sample to be suitable for fluorescence microscopy it must be fluorescent. There are several methods of creating a fluorescent sample; the main techniques are labelling with fluorescent stains or, in the case of biological samples, expression of a fluorescent protein. Alternatively the intrinsic fluorescence of a sample (i.e., autofluorescence) can be used. In the life sciences fluorescence microscopy is a powerful tool which allows the specific and sensitive staining of a specimen in order to detect the distribution of proteins or other molecules of interest. As a result there is a diverse range of techniques for fluorescent staining of biological samples.
Biological fluorescent stains
Many fluorescent stains have been designed for a range of biological molecules. Some of these are small molecules which are intrinsically fluorescent and bind a biological molecule of interest. Major examples of these are nucleic acid stains like DAPI and Hoechst which bind the minor groove of DNA, thus labelling the nuclei of cells. Others are drugs or toxins which bind specific cellular structures and have been derivatised with a fluorescent reporter. A major example of this class of fluorescent stain is fluorescently labelled-phalloidin which is used to stain actin fibres in mammalian cells.
There are many fluorescent reported molecules, called fluorophores such as fluorescein and DyLight 488, which can be chemically linked to a different molecule which binds the target of interest within the sample.
ImmunofluorescenceMain article: Immunofluorescence
Immuofluorescence is an antibody based on technique which uses the highly specific binding of an antibody to its antigen in order to label specific proteins or other molecules within the cell. A sample is treated with a primary antibody specific for the molecule of interest A fluorophore can be directly conjugated to the primary antibody. Alternatively a secondary antibody, conjugated to a fluorophore, which binds specifically to the first antibody can be used. For example a primary antibody raised in a mouse which recognises tubulin combined with a secondary anti-mouse antibody derivatised with a fluorophore could be used to label microtubules in a cell.
Fluorescent proteinsSee also: Fluorescent protein
The modern understanding of genetics and the techniques available for modifying DNA allows scientists to genetically modify proteins to also carry a fluorescent protein reporter. In biological samples this allows a scientist to directly make a protein of interest fluorescent. The protein location can then be directly tracked, including in live cells.
Fluorophores lose their ability to fluoresce as they are illuminated in a process called photobleaching. Photobleaching occurs as the fluorescent molecules accumulate chemical damage from the electrons excited during fluorescence. Photobleaching can severely limit the time over which a sample can be observed by fluorescent microscopy. Several techniques exist to reduce photobleaching such as the use of more robust fluorophores, by minimizing illumination, or by using photoprotective scavenger chemicals.
Fluorescence microscopy with fluorescent reporter proteins has enabled analysis of live cells by fluorescence microscopy, however cells are susceptible to phototoxicity, particularly with short wavelength light. Furthermore fluorescent molecules have a tendency to generate reactive chemical species when under illumination which enhances the phototoxic effect.
Unlike transmitted and reflected light microscopy techniques fluorescence microscopy only allows observation of the specific structures which have been fluorescently labeled. For example observing a tissue sample prepared with a fluorescent DNA stain by fluorescent microscopy only reveals the organisation of the DNA within the cells and reveals nothing else about the cell morphologies.
Improvements and sub-diffraction techniquesSee also: Microscopy#Sub-diffraction techniques
The wave nature of light limits the size of the spot to which light can be focused due to the diffraction limit. This limitation was described in the 19th century by Ernst Abbe and limits an optical microscope's resolution to approximately half of the wavelength of the light used. Fluorescence microscopy is central to many techniques which aim to reach past this limit by specialised optical configurations.
Several improvements in microscopy techniques have been invented in the 20th century and have resulted in increased resolution and contrast to some extent. However they did not overcome the diffraction limit. In 1978 first theoretical ideas have been developed to break this barrier by using a 4Pi microscope as a confocal laser scanning fluorescence microscope where the light is focused ideally from all sides to a common focus which is used to scan the object by 'point-by-point' excitation combined with 'point-by-point' detection. However, the first experimental demonstration of the 4pi microscope took place in 1994. 4Pi microscopy maximizes the amount of available focusing directions by using two opposing objective lenses or Multi-photon microscopy using redshifted light and multi-photon excitation.
The first technique to really achieve a sub-diffraction resolution was STED microscopy, proposed in 1994. This method and all techniques following the RESOLFT concept rely on a strong non-linear interaction between light and fluorescing molecules. The molecules are driven strongly between distinguishable molecular states at each specific location, so that finally light can be emitted at only a small fraction of space, hence an increased resolution.
As well in the 1990s another super resolution microscopy method based on wide field microscopy has been developed. Substantially improved size resolution of cellular nanostructures stained with a fluorescent marker was achieved by development of SPDM localization microscopy and the structured laser illumination (spatially modulated illumination, SMI). Combining the principle of SPDM with SMI resulted in the development of the Vertico SMI microscope. Single molecule detection of normal blinking fluorescent dyes like Green fluorescent protein (GFP) can be achieved by using a further development of SPDM the so-called SPDMphymod technology which makes it possible to detect and count two different fluorescent molecule types at the molecular level (this technology is referred to as 2CLM, 2 Color Localization Microscopy).
Alternatively, the advent of photoactivated localization microscopy could achieve similar results by relying on blinking or switching of single molecules, where the fraction of fluorescing molecules is very small at each time. This stochastic response of molecules on the applied light corresponds also to a highly nonlinear interaction, leading to subdiffraction resolution.
Fluorescence microscope gallery
Fluorescence micrograph gallery
Epifluorescent imaging of the three components in a dividing human cancer cell. DNA is stained blue, a protein called INCENP is green, and the microtubules are red. Each fluorophore is imaged separately using a different combination of excitation and emission filters, and the images are captured sequentially using a digital CCD camera, then overlaid to give a complete image.
Human lymphocyte nucleus stained with DAPI with chromosome 13 (green) and 21 (red) centromere probes hybridized (Fluorescent in situ hybridization (FISH))
Fluorescence microscopy of DNA Expression in the Human Wild-Type and P239S Mutant Palladin.
- ^ a b c d Spring KR, Davidson MW. "Introduction to Fluorescence Microscopy". Nikon MicroscopyU. http://www.microscopyu.com/articles/fluorescence/fluorescenceintro.html. Retrieved 2008-09-28.
- ^ "The Fluorescence Microscope". Microscopes—Help Scientists Explore Hidden Worlds. The Nobel Foundation. http://nobelprize.org/educational_games/physics/microscopes/fluorescence/. Retrieved 2008-09-28.
- ^ Considerations on a laser-scanning-microscope with high resolution and depth of field: C. Cremer and T. Cremer in M1CROSCOPICA ACTA VOL. 81 NUMBER 1 September,pp. 31—44 (1978)
- ^ S.W. Hell, E.H.K. Stelzer, S. Lindek, C. Cremer (1994). "Confocal microscopy with an increased detection aperture: type-B 4Pi confocal microscopy". Optics Letters 19 (3): 222–224. Bibcode 1994OptL...19..222H. doi:10.1364/OL.19.000222. PMID 19829598. http://www.opticsinfobase.org/viewmedia.cfm?uri=ol-19-3-222&seq=0.
- ^ M. Hausmann, B. Schneider, J. Bradl, C. Cremer (1997): High-precision distance microscopy of 3D-nanostructures by a spatially modulated excitation fluorescence microscope. In: Optical Biopsies and Microscopic Techniques II (Edts Bigio IJ, Schneckenburger H, Slavik J, Svanberg K, Viallet PM), Proc. SPIE 3197: 217-222
- ^ High precision structural analysis of subnuclear complexes in fixed and live cells via Spatially Modulated Illumination (SMI) microscopy: J. Reymann, D. Baddeley, P. Lemmer, W. Stadter, T. Jegou, K. Rippe, C. Cremer, U. Birk in CHROMOSOME RESEARCH, Vol. 16, pp. 367 –382 (2008)
- ^ Nano-structure analysis using Spatially Modulated Illumination microscopy: D. Baddeley, C. Batram, Y. Weiland, C. Cremer, U.J. Birk in NATURE PROTOCOLS, Vol 2, pp. 2640–2646 (2007)
- ^ Manuel Gunkel, Fabian Erdel, Karsten Rippe, Paul Lemmer, Rainer Kaufmann, Christoph Hörmann, Roman Amberger and Christoph Cremer: Dual color localization microscopy of cellular nanostructures. In: Biotechnology Journal, 2009, 4, 927-938. ISSN 1860-6768
Fluorescence methodsFluorescence microscopy · Confocal microscopy · Two-photon excitation microscopy · Multiphoton microscopy · Image deconvolution · Total internal reflection fluorescence microscopy (TIRF) Sub-diffraction
limit techniquesDiffraction limit · Stimulated emission depletion (STED) · Photo-activated localization microscopy (PALM) · Near-field (NSOM/SNOM)Categories:
- Cell imaging
- Laboratory equipment
Wikimedia Foundation. 2010.