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Dark-field microscopy

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Laboratory technique
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Red blood cells as seen by dark-field microscopy

Dark-field microscopy, also calleddark-ground microscopy, describesmicroscopy methods, in bothlight andelectron microscopy, which exclude the unscattered beam from the image. Consequently, the field around the specimen (i.e., where there is no specimen toscatter the beam) is generally dark.

In optical microscopes a darkfieldcondenser lens must be used, which directs a cone of light away from the objective lens. To maximize the scattered light-gathering power of the objective lens, oil immersion is used and thenumerical aperture (NA) of the objective lens must be less than 1.0. Objective lenses with a higher NA can be used but only if they have an adjustable diaphragm, which reduces the NA. Often these objective lenses have a NA that is variable from 0.7 to 1.25.[1]

Light microscopy applications

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A cross-section of anematode, photographed with an oil dark field condenser with anumerical aperture of 1.40

Inoptical microscopy, dark-field describes anillumination technique used to enhance thecontrast in unstainedsamples. It works by illuminating the sample with light that will not be collected by the objective lens and thus will not form part of the image. This produces the classic appearance of a dark, almost black, background with bright objects on it. Optical dark fields usually done with ancondenser that features a central light-stop in front of the light source to prevent direct illumination of the focal plane, and at highernumerical apertures may require oil or water between the condenser and the specimen slide to provide an optimalrefractive index.[2][3]

The light's path

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Diagram illustrating the light path through a dark-field microscope

The steps are illustrated in the figure where aninverted microscope is used.

  1. Light enters themicroscope for illumination of the sample.
  2. A specially sized disc, thepatch stop (see figure), blocks some light from the light source, leaving an outer ring of illumination. A wide phase annulus can also be reasonably substituted at low magnification.
  3. Thecondenser lens focuses the light towards the sample.
  4. The light enters the sample. Most is directly transmitted, while some is scattered from the sample.
  5. Thescattered light enters the objective lens, while thedirectly transmitted light simply misses the lens and is not collected due to adirect-illumination block (see figure).
  6. Only the scattered light goes on to produce the image, while the directly transmitted light is omitted.

Advantages and disadvantages

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Dark-field microscopy produces an image with a dark background
Operating principles of dark-field andphase-contrast microscopies

Dark-field microscopy is a very simple yet effective technique and well suited for uses involving live andunstained biological samples, such as a smear from a tissue culture or individual, water-borne, single-celled organisms.[4] Considering the simplicity of the setup, the quality of images obtained from this technique is impressive.

One limitation of dark-field microscopy is the low light levels seen in the final image. This means that the sample must be very strongly illuminated, which can cause damage to the sample.

Dark-field microscopy techniques are almost entirely free of halo or relief-style artifacts typical ofdifferential interference contrast microscopy. This comes at the expense of sensitivity to phase information.

The interpretation of dark-field images must be done with great care, as common dark features ofbright-field microscopy images may be invisible, and vice versa. In general the dark-field image lacks the lowspatial frequencies associated with the bright-field image, making the image ahigh-passed version of the underlying structure.

While the dark-field image may first appear to be a negative of the bright-field image, different effects are visible in each. In bright-field microscopy, features are visible where either a shadow is cast on the surface by the incident light or a part of the surface is less reflective, possibly by the presence of pits or scratches. Raised features that are too smooth to cast shadows will not appear in bright-field images, but the light that reflects off the sides of the feature will be visible in the dark-field images.

  • Comparison of transillumination techniques used to generate contrast in a sample oftissue paper (1.559 μm/pixel when viewed at full resolution)
  • Dark-field illumination, sample contrast comes from light scattered by the sample
    Dark-field illumination, sample contrast comes from lightscattered by the sample
  • Bright-field illumination, sample contrast comes from attenuation of light in the sample
    Bright-field illumination, sample contrast comes fromattenuation of light in the sample
  • Cross-polarized light illumination, sample contrast comes from rotation of polarized light through the sample
    Cross-polarized light illumination, sample contrast comes from rotation ofpolarized light through the sample
  • Phase-contrast illumination, sample contrast comes from interference of different path lengths of light through the sample
    Phase-contrast illumination, sample contrast comes frominterference of different path lengths of light through the sample

Use in computing

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Dark-field microscopy has recently been applied incomputer mouse pointing devices to allow the mouse to work on transparent glass by imaging microscopic flaws and dust on the glass's surface.

Dark-field microscopy combined with hyperspectral imaging

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When coupled tohyperspectral imaging, dark-field microscopy becomes a powerful tool for the characterization ofnanomaterials embedded in cells. In a recent publication, Patskovsky et al. used this technique to study the attachment of goldnanoparticles (AuNPs) targetingCD44+ cancer cells.[5]

Transmission electron microscope applications

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Main article:transmission electron microscopy
Weak-beam DF of strain aroundnuclear track cores

Dark-field studies in transmission electron microscopy play a powerful role in the study of crystals and crystal defects, as well as in the imaging of individual atoms.

Conventional dark-field imaging

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Briefly, imaging[6] involves tilting the incident illumination until a diffracted, rather than the incident, beam passes through a small objective aperture in the objective lens back focal plane. Dark-field images, under these conditions, allow one to map the diffracted intensity coming from a single collection of diffracting planes as a function of projected position on the specimen and as a function of specimen tilt.

In single-crystal specimens, single-reflection dark-field images of a specimen tilted just off theBragg condition allow one to "light up" only those lattice defects, like dislocations or precipitates, that bend a single set of lattice planes in their neighborhood. Analysis of intensities in such images may then be used to estimate the amount of that bending. In polycrystalline specimens, on the other hand, dark-field images serve to light up only that subset of crystals that are Bragg-reflecting at a given orientation.

Animation: dark-field imaging of crystals
Digital dark-field simulation of 2 nm metal particles on a nano-cylinder
This animation illustrates movement of an aperture (centered in the orange figure at left) over the power spectrum (a digital substitute for the back focal-plane's optical diffraction pattern) shown with the DC peak (or unscattered beam) below center. Only nanocrystals with projected periodicities that diffract into the aperture light up in the dark-field image at right. The aperture is moving by 1.25° increments around the ring associated with diffraction from gold 2.3 Å (111) lattice spacings.

Weak-beam imaging

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Digital dark-field image of internal twins

Weak-beam imaging involves optics similar to conventional dark-field, but uses a diffracted beamharmonic rather than the diffracted beam itself. In this way, much higher resolution of strained regions around defects can be obtained.

Low- and high-angle annular dark-field imaging

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Annular dark-field imaging requires one to form images with electrons diffracted into an annular aperture centered on, but not including, the unscattered beam. For large scattering angles in ascanning transmission electron microscope, this is sometimes calledZ-contrast imaging because of the enhanced scattering from high-atomic-number atoms.

Digital dark-field analysis

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This a mathematical technique intermediate between direct and reciprocal (Fourier-transform) space for exploring images with well-defined periodicities, like electron microscope lattice-fringe images. As with analog dark-field imaging in a transmission electron microscope, it allows one to "light up" those objects in the field of view where periodicities of interest reside. Unlike analog dark-field imaging it may also allow one to map theFourier-phase of periodicities, and hence phase gradients, which provide quantitative information on vector lattice strain.

See also

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Footnotes

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  1. ^Nikon: Darkfield Illumination
  2. ^Abramowitz, Mortimer; Davidson, Michael W."Specialized Microscopy Techniques - Darkfield Illumination".Microscopy Resource Center. Olympus LS. Retrieved24 October 2024.
  3. ^Murray, R. G. E.; Robinow, Carl F. (30 April 2014)."Light Microscopy"(PDF).Methods for General and Molecular Microbiology:15–16.doi:10.1128/9781555817497.ch1. Retrieved24 October 2024.
  4. ^"Darkfield Illumination".evidentscientific.com. Retrieved2025-01-10.
  5. ^S. Patskovsky; et al. (2014). "Wide-field hyperspectral 3D imaging of functionalized gold nanoparticles targeting cancer cells by reflected light microscopy".Journal of Biophotonics.8 (5):1–7.doi:10.1002/jbio.201400025.PMID 24961507.
  6. ^P. Hirsch, A. Howie, R. Nicholson, D. W. Pashley and M. J. Whelan (1965/1977)Electron microscopy of thin crystals (Butterworths/Krieger, London/Malabar FL)ISBN 0-88275-376-2.

External links

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