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Michel son-interferometer

In the hrst case, the degree of self coherence depends on the spectral characteristics of the source. The coherence time Tc represents the time scale over which a held remains correlated this hme is inversely proportional to the spectral bandwidth Au) of the detected light. A more quantitative dehnition of quasi-monochromatic conditions is based on the coherence time all relevant delays within the interferometer should be much shorter than the coherence length CTc. A practical way to measure temporal coherence is to use a Michel-son interferometer. As we shall see, in the second case the spatial coherence depends on the apparent extent of a source. [Pg.279]

In detector noise limited spectroscopies such as PAS it is advantageous to enhance the throughput of energy (Jacquinot s advantage) by utilizing a Michel son interferometer. One then Fourier transforms (FTs) the resulting interferogram to yield a PA spectrum that qualitatively resembles an absorption spectrum. [Pg.393]

No beam chopping device is shown in Figure 5. Motion of the moving mirror in the Michel son interferometer is equivalent to beam chopping and the frequency f is given by... [Pg.395]

One type of interferometer which measures changes in position using monochromatic light of a known wavelength is a Michel-son interferometer (Figure 7.18). In this device, monochro-... [Pg.191]

Experimental Techniques. A block diagram of the experimental set-up used for saturated absorption experiments is shown in Figure 1. The argon laser is a commercial 4W tube in a home made cavity. This cavity is made of three Invar rods, decoupled from the tube in order to avoid vibrations. Line selection is made with a prism, and single frequency operation is obtained with a Michel son interferometer. The laser can be frequency locked to a stable Fabry-Perot resonator with a double servo-loop acting on a fast PZT for line narrowing and on a galvo-plate for wide tuna-bility. This results in a linewidth of less than 10 KHz and a continuous tunability of 6 GHz. [Pg.490]

The basic component of most Fourier Transform Infrared spectrometers is the Michel son interferometer. This is not the only interferometer used in FT-IR, but it is employed more often than other designs. A treatment of many other interferometer designs is available. The Michel son interferometer in a Fourier Transform Infrared spectrometer replaces the monochromator in a dispersive instrument, although the functions cannot be correlated. A monochomator divides a continuous bandwidth into its component frequencies, whereas an interferometer produces interference patterns of the bandwidth in a precise and regulated manner. It should be noted that this type of interferometer is not restricted to the infrared region and its use can be extended to the visible and millimeter regions of the electromagnetic spectrum. [Pg.387]

The maximum optical retardation, then, determines the ultimate resolution which is possible with a particular Fourier transform instrument. However, other design features must also be considered when deciding whether that ultimate resolution is in fact achievable. In particular, the size of the aperture through the Michel son interferometer must also be considered. [Pg.427]

Jacquinotl2,13 recognized that the light gathering capability of a Michel son interferometer is greater than that of a dispersive instrument operating that the same resolving power. The improvement offered by the Fourier transform spectrometer can be expressed asl"... [Pg.433]

These experimental modifications represent various applications of the Fourier method and all can be accommodated within the design spirit of Figure 1. Furthermore, the optical features of the Michel son interferometer shown in Figure 1 are only schematic. In the actual design and construction of interferometers which operate in the visible/UV region, several variations from this schematic representation have been implemented. [Pg.440]

Edmonton, Alberta, Canada A modular Michel son interferometer has been constructed at the University of Alberta by Horlick and Yuen.46,47 /vs the French instrument just discussed, this... [Pg.444]

Our recent experiences (14) with a minicomputerized Michel-son interferometer for Fourier transform photoacoustic spectroscopy have suggested a speedier method of aligning a resonance ultrasound cell. Burleigh Instruments, Inc. (P. 0. Box 270,... [Pg.125]

Fig.2.35. Michel son interferometer for measurement of the temporal coherence of radiation from the source S... Fig.2.35. Michel son interferometer for measurement of the temporal coherence of radiation from the source S...
Examples of devices in which only two partial beams interfere, are the Michel son interferometer and the Mach-Zehnder interferometer. Multiple-bem interference is used for instance in the Fabry-Perot interferometer and in multilayer dielectric coatings of highly reflecting mirrors. [Pg.139]

Fig.4,26. (a) Michel son interferometer with optical delay line, allowing a large path difference between the two interfering beams, (b) Michel son interferometer with Littrow prism as preselector... [Pg.144]

Assume that a signal-to-noise ratio of 50 has been achieved in measuring the fringe pattern of a Michel son interferometer with one continuously... [Pg.228]

Often a Michel son interferometer is used for mode selection, coupled by a beam splitter St to the laser resonator (Fig.6.16). The free spectral range of this "Fox-Smith cavity" [6.13], which is AX=c/[2(L2+L )], has... [Pg.287]

As can be seen from Fig. 8a, a mirror displacement of x cm results in an optical path difference of 2x cm for instruments with Michel son interferometers. Instruments with Genzel interferometers, achieve an optical path difference of 4x. Resolution is inversely proportional to optical path differences, so it can be seen that the Genzel interferometer achieves the same resolution for only half the mirror travel of a Michel son interferometer, an important feature when mechanical tolerance is considered. The schematic diagram of the Genzel interferometer is depicted in Fig. 8b. The detector then measures the amount of energy at discrete intervals of mirror travel. [Pg.38]


See other pages where Michel son-interferometer is mentioned: [Pg.399]    [Pg.693]    [Pg.694]    [Pg.363]    [Pg.387]    [Pg.396]    [Pg.396]    [Pg.400]    [Pg.407]    [Pg.423]    [Pg.1769]    [Pg.432]    [Pg.292]    [Pg.123]    [Pg.67]    [Pg.184]    [Pg.289]    [Pg.38]    [Pg.38]    [Pg.39]   
See also in sourсe #XX -- [ Pg.141 , Pg.191 , Pg.289 ]




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