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Theory of Interferometry

Closure phase Sum of the measured coherence phase around a triad of array elements invariant to all effects that factorize per element, e.g., extra path lengths introduced into the signal path by the atmosphere. [Pg.271]

Coherence Time-averaged product of the electric field at two different points in space. For a distant incoherent source the measured coherence is a Fourier transform of the source brightness distribution. [Pg.271]

Correlator Computer for calculating the coherence between two antennas, usually realized with digital logic. [Pg.271]

Deconvolution Correction for the effects of limited sampling of the coherence function. Accomplished by utilizing knowledge of the coherence sampling function and a priori information about the source brightness distribution, such as positivity and confinement. [Pg.271]

Heterodyne Shift in the frequency of a spectrum accomplished by adding a carrier wave at an offset frequency, and then passing the signal into a nonlinear device. [Pg.271]


Optical Interferometry. 2d ed. San Diego Academic Press, 2003. Overview of the basic theory of interferometry methods, including sections on laser interferometry. [Pg.1116]

Fig. 8. (ii) Geometry and interferometry in the SFA. The distance between the surfaces is determined from the wavelengths of FECO. (a) The PECO fringes when the surfaces are in contact. The separation profile, D versus r, can be measured from the fringe profile, and compared to that predicted by the JKR theory of contact mechanics, (b) The FECO when the surfaces are separated. By measuring the wavelengths of the fringes when the surfaces are in contact and when they are separated, we can determine the distance between the two surfaces. [Pg.97]

Theory of HHG in Mixed Gases and Heterodyne Interferometry for Detection of Ultrafast Molecular Dynamics... [Pg.67]

Whittaker s early work [27,28] is the precursor [4] to twistor theory and is well developed. Whittaker showed that a scalar potential satisfying the Laplace and d Alembert equations is structured in the vacuum, and can be expanded in terms of plane waves. This means that in the vacuum, there are both propagating and standing waves, and electromagnetic waves are not necessarily transverse. In this section, a straightforward application of Whittaker s work is reviewed, leading to the feasibility of interferometry between scalar potentials in the vacuum, and to a trouble-free method of canonical quantization. [Pg.172]

Very much more is known about the theory of concentration gradients at electrodes than has been mentioned in this brief account. Experimental methods for observing them have also been devised, based on the dependence of refractive index on concentration (the Schlieren method) by means of interferometry (O Brien, 1986). Nevertheless, the basic concept of an effective diffusion-layer thickness, treated here as varying in thickness with fi until the onset of natural convection and as constant with time after convection sets in (though decreasing in value with the degree of disturbance, Table 7.10), is a useful aid to the simple and approximate analysis of many transport-controlled electrodic situations. A few of the uses of the concept of 8 will now be outlined. [Pg.518]

Nafie LA, Diem M (1979) Theory of high-frequency differential interferometry - application to the measurement of infrared circular and linear dichroism via Fourier-transform spectroscopy. Appl Spectrosc 33 130-135... [Pg.229]

Optical interferometry has an interest in its own right in the determination of the refractive indices of gases. For example, precise laser refractometry of pure helium gas can lead to a better determination of the Boltzmann constant [80] when combined with the latest ab initio theory of atomic polarisability [81]. [Pg.460]

In this chapter the two Spectro-Spatial Interferometry Testbeds in which I have been involved during my programme have been presented the FIRI laboratory testbed and WIIT, the Wide-field Imaging Interferometry Testbed. Both testbeds demonstrate the theory of Double Fourier Spatio-Spectral Interferometry or the application of a Fourier-transform spectrometer (FTS) to aperture synthesis interferometry presented in the previous chapter, at far infrared wavelengths and optical wavelengths, respectively. [Pg.70]

When a GI medium is applied to coherent optics such as in interferometry and holography, however, it is important that a two-dimensional system theory based on wave optics be introduced into the treatment of transforms by an optical system with a GI medium. In this article we introduce such a theory, which applies an integral transform associated with a GI medium into the system theory of optics. This will enable us to learn not only about the imaging condition but also about some types of transform representations. [Pg.123]

As described in the article on the theory of surface plasmon resonance, surface plasmons create a surface-bound evanescent electromagnetic wave which propagates along the surface of an active medium (usually a thin metallic film), with the electric field intensity maximized at this surface and diminishing exponentially on both sides of the interface. As a consequence of this property, the phenomenon has been utilized extensively in studies of surfaces and of thin dielectric films deposited on the active medium. Although numerous other optical techniques have also been applied to such systems (e.g. ellipsometry, interferometry, spectrophotometry, and microscopy the surface plasmon resonance (SPR) method has some important advantages over all other optical techniques, as follows. The method utilizes a relatively simple optical system, it has a superior sensitivity, and the complete system of measurement is located on the side of the apparatus that is remote from the sample, and thus there is no optical interference from the bulk medium. Furthermore, the surfaces of the sample need no extra treatment to increase... [Pg.1128]

Snieder R (2006) The theory of coda wave interferometry. Pure Appl Geophys 163 455 73. doi 10.1007/ S00024-005-0026-6... [Pg.3786]

The P on the left-hand side of Eq. (162) denotes path ordering and the P denotes area ordering [4]. Equation (162) is the result of a round trip or closed loop in Minkowski spacetime with 0(3) covariant derivatives. Equation (161) is a direct result of our basic assumption that the configuration of the vacuum can be described by gauge theory with an internal 0(3) symmetry (Section I). Henceforth, we shall omit the P and P from the left- and right-hand sides, respectively, and give a few illustrative examples of the use of Eq. (162) in interferometry and physical optics. [Pg.116]

Rhee H, Ha JH, Jeon SJ et al (2008) Femtosecond spectral interferometry of optical activity theory. J Chem Phys 129 094507... [Pg.236]

Earlier investigations on N20 have been summarized by Herzfeld and Litovitz [8] and by Calvert [252]. Simpson, Bridgman, and Chandler [253] have more recently examined vibrational relaxation in pure N20 over the range 320-820°K using shock-tube interferometry. As in the case of C02, single relaxation is observed. Experimental relaxation times are depicted in Figure 3.31, and are compared with SSH theory. [Pg.252]

The technique used to measure the surface tension of foils in this work couples two well Imown technologies the zero creep technique for foils, and the technique of laser interferometry. The theory behind each of these techniques will be discussed briefly in order to develop the expressions necessary to generate the desired surface tension data which will be used to calculate the surface free energy. [Pg.304]


See other pages where Theory of Interferometry is mentioned: [Pg.114]    [Pg.40]    [Pg.19]    [Pg.271]    [Pg.271]    [Pg.114]    [Pg.40]    [Pg.19]    [Pg.271]    [Pg.271]    [Pg.173]    [Pg.260]    [Pg.5]    [Pg.41]    [Pg.1115]    [Pg.41]    [Pg.237]    [Pg.3784]    [Pg.322]    [Pg.334]    [Pg.96]    [Pg.17]    [Pg.92]    [Pg.83]    [Pg.87]    [Pg.95]    [Pg.115]    [Pg.49]    [Pg.146]    [Pg.149]    [Pg.19]   


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