Total internal reflection fluorescence microscope

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(Cis-)total internal reflection fluorescence microscope (TIRFM) diagram
  1. Specimen
  2. Evanescent wave range
  3. Cover slip
  4. Immersion oil
  5. Objective
  6. Emission beam (signal)
  7. Excitation beam
(Trans-)total internal reflection fluorescence microscope (TIRFM) diagram
  1. Objective
  2. Emission beam (signal)
  3. Immersion oil
  4. Cover slip
  5. Specimen
  6. Evanescent wave range
  7. Excitation beam
  8. Quartz prism

A total internal reflection fluorescence microscope (TIRFM) is a type of microscope with which a thin region of a specimen, usually less than 200 nm can be observed.

Background[edit]

In cell and molecular biology, a large number of molecular events in cellular surfaces such as cell adhesion, binding of cells by hormones, secretion of neurotransmitters, and membrane dynamics have been studied with conventional fluorescence microscopes. However, fluorophores that are bound to the specimen surface and those in the surrounding medium exist in an equilibrium state. When these molecules are excited and detected with a conventional fluorescence microscope, the resulting fluorescence from those fluorophores bound to the surface is often overwhelmed by the background fluorescence due to the much larger population of non-bound molecules. TIRFM allows for selective excitation of the surface-bound fluorophores, while non-bound molecules are not excited and do not fluoresce. Due to the fact of sub-micron surface selectivity TIRFM has become a method of choice for single molecule detection.

Overview[edit]

The idea of using total internal reflection to illuminate cells contacting the surface of glass was first described by E.J. Ambrose in 1956.[1] This idea was then extended by Daniel Axelrod[2] at the University of Michigan, Ann Arbor in the early 1980s as TIRFM. A TIRFM uses an evanescent wave to selectively illuminate and excite fluorophores in a restricted region of the specimen immediately adjacent to the glass-water interface. The evanescent wave is generated only when the incident light is totally internally reflected at the glass-water interface. The evanescent electromagnetic field decays exponentially from the interface, and thus penetrates to a depth of only approximately 100 nm into the sample medium. Thus the TIRFM enables a selective visualization of surface regions such as the basal plasma membrane (which are about 7.5 nm thick) of cells as shown in the figure above. Note, however, that the region visualised is at least a few hundred nanometers wide, so the cytoplasmic zone immediately beneath the plasma membrane is necessarily visualised in addition to the plasma membrane during TIRF microscopy. The selective visualisation of the plasma membrane renders the features and events on the plasma membrane in living cells with high axial resolution.

TIRF can also be used to observe the fluorescence of a single molecule,[3][4] making it an important tool of biophysics and quantitative biology.

Cis-geometry (through-objective TIRFM) and trans-geometry (prism- and lightguide based TIRFM) have been shown to provide different quality of the effect of total internal reflection. In the case of trans-geometry, the excitation lightpath and the emission channel are separated, while in the case of objective-type TIRFM they share the objective and other optical elements of the microscope. Prism-based geometry was shown to generate clean evanescent wave, which exponential decay is close to theoretically predicted function.[5] In the case of objective-based TIRFM, however, the evanescent wave is contaminated with intense stray light. The intensity of stray light was shown to amount 10-15% of the evanescent wave, which makes it difficult to interpret data obtained by objective-type TIRFM [6][7]

References[edit]

  1. ^ Ambrose, EJ (24 Nov 1956). "A surface contact microscope for the study of cell movements.". Nature. 178 (4543): 1194. Bibcode:1956Natur.178.1194A. doi:10.1038/1781194a0. 
  2. ^ Axelrod, D. (1 April 1981). "Cell-substrate contacts illuminated by total internal reflection fluorescence". The Journal of Cell Biology. 89 (1): 141–145. doi:10.1083/jcb.89.1.141. PMC 2111781free to read. PMID 7014571. 
  3. ^ Yanagida, Toshio; Sako, Yasushi; Minoghchi, Shigeru (10 February 2000). "Single-molecule imaging of EGFR signalling on the surface of living cells". Nature Cell Biology. 2 (3): 168–172. doi:10.1038/35004044. PMID 10707088. 
  4. ^ Andre et al. Cross-correlated tirf/afm reveals asymmetric distribution of forcegenerating heads along self-assembled, synthetic myosin filaments. Biophysical Journal, 96:1952–1960, 2009.
  5. ^ Ambrose, W; et al. (1999). "Single-molecule detection with total internal reflection excitation: comparing signal-to-background and total signals in different geometries. Cytometry". 36(3): 224. 
  6. ^ Mattheyses A. and Axelrod, D. (2006). "Direct measurement of the evanescent field profile produced by objective-based TIRF.". J Biomed Opt. 11: 014006A. 
  7. ^ Brunstein M, Teremetz M, Hérault K, Tourain C, Oheim, M. (2014). "Eliminating unwanted far-field excitation in objectivetype TIRF. Part I.". Biophys J. 106(5): 1020. 

External links[edit]