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Interference patterns

Shearography monitors the speckular 2D interference pattern of an unpolished surface illuminated by a coherent light source, and is therefore a metliod that lends itself to the testing of industrial materials. Small surface, or near-surface defects may produce localised strain on... [Pg.678]

When an electron scatters from an atom, its phase is changed so that the reflected wave is not in phase with the incoming wave. This changes the interference pattern and hence the apparent distance between the two atoms. Knowledge of this phase shift is the key to getting precise bond lengths from SEXAFS. Phase shifts depend mainly on which atoms are involved, not on their detailed chemical environment, and should therefore be transferable from a known system to unknown systems. The phase shifts may be obtained ftom theoretical calculations, and there are published tabulations, but practically it is desirable to check the phase shifts using... [Pg.229]

Probability maps typically exhibit striped wave-like interference patterns. It is easy to show why striped i atterns (i.e. patterns for which, at a given time step, the site probabilities alternate between low and high values), emerge for all systems with Sc > /2. Assume that (7j t) 0, At time t -f 1 we then have... [Pg.408]

When a beam of monochromatic radiation is passed through the windows of an infrared cell some reflection occurs on the window surfaces and interference takes place between radiation passing from the internal surface of the first window and that reflected back from the internal surface of the second window. This interference is at a maximum when 2d = (n + 1 /2)k, where d is the distance in yum between the inner surfaces of the two cell windows, X is the wavelength in m, and n is any integral number. If the wavelength k of the monochromatic radiation is varied continuously an interference pattern consisting of a series of waves (Fig. 19.7) is obtained. [Pg.750]

Fig. 19.7 Interference patterns from empty fixed-path-length cell. Reprodnced by permission from R. C. J. Osland, Principles and Practices of Infrared Spectroscopy, 2nd edn, Philips Ltd, 1985. Fig. 19.7 Interference patterns from empty fixed-path-length cell. Reprodnced by permission from R. C. J. Osland, Principles and Practices of Infrared Spectroscopy, 2nd edn, Philips Ltd, 1985.
The application of interference techniques overcomes the limitations exerted by the large optical wavelengths. With commercial phase-measurement interference microscopes (PMIM), a surface resolution of the order of 0.6 nm can be achieved [33, 34]. In a microscope a laser beam is both reflected from the sample surface and from a semitransparent smooth reference surface (Fig. 3). The interference pattern is recorded on an area detector and modulated via the piezo-electric driven reference surface. The modulated interference pattern is fed into a computer to generate a two-dimensional phase map which is converted into a height level contour map of the sample surface. While the lateral resolution (typically of the... [Pg.368]

A nearly perfect diverging wavefront would exit the test plate appearing as though it came from a source 100 m away. A segment would be positioned so that its mean center of curvature was coincident with that virtual source 100 m away. In the worst case in our example, the un-equal air path would be about 4 m rather than 204 m. Interference would take place between the wavefront reflected off the 100 m radius side of the test plate and the segment. The roughly 3 m back to the source and beamsplitter is common path and will not affect the interference pattern. [Pg.101]


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