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Your price. Image ID:. Standard royalty-free license for commercial use eg. Add extended license. Image information. Image Specification:. All attempts to observe the size and shape of objects are limited by the wavelength of the probe. Sonar and medical ultrasound are limited by the wavelength of sound they employ. We shall see that this is also true in electron microscopy, since electrons have a wavelength.

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The most obvious method of obtaining better detail is to utilize shorter wavelengths. Ultraviolet UV microscopes have been constructed with special lenses that transmit UV rays and utilize photographic or electronic techniques to record images. The shorter UV wavelengths allow somewhat greater detail to be observed, but drawbacks, such as the hazard of UV to living tissue and the need for special detection devices and lenses which tend to be dispersive in the UV , severely limit the use of UV microscopes.

Elsewhere, we will explore practical uses of very short wavelength EM waves, such as x rays, and other short-wavelength probes, such as electrons in electron microscopes, to detect small details. Another difficulty in microscopy is the fact that many microscopic objects do not absorb much of the light passing through them. The lack of contrast makes image interpretation very difficult. Contrast is the difference in intensity between objects and the background on which they are observed.

Stains such as dyes, fluorophores, etc. More general wave interference techniques can be used to produce contrast. Since the indices of refraction differ, the number of wavelengths in the paths differs.


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Light emerging from the object is thus out of phase with light from the background and will interfere differently, producing enhanced contrast, especially if the light is coherent and monochromatic -- as in laser light. Inference microscopes enhance contrast between objects and background by superimposing a reference beam of light upon the light emerging from the sample.


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Since light from the background and objects differ in phase, there will be different amounts of constructive and destructive interference, producing the desired contrast in final intensity. Parallel rays of light from a source are split into two beams by a half-silvered mirror. These beams are called the object and reference beams. Each beam passes through identical optical elements, except that the object beam passes through the object we wish to observe microscopically.

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The light beams are recombined by another half-silvered mirror and interfere.