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Optics, defined

The production of integrated circuits has, in the 40 years since their invention, become the most complex and expensive manufacturing procedure ever it even leaves the production of airliners in the shade. One circuit requires a sequence of several dozen manufacturing steps, with positioning of successive optically defined layers accurate to a fraction of a micrometer, all interconnected electrically, and... [Pg.262]

The actual distributions of microbubble diameters in sea water, measured by Weitendorf in the optically defined control volume, ranged between 20 and 117 pm. Within this diameter range, the usual number of measured microbubbles per cm3 was of the order of 10 to 100, yielding an approximate microbubble concentration of 104-105/liter for these ocean experiments (ref. [Pg.27]

Dhaval A. Doshi, Nicola K. Huesing, Mengcheng Lu, Hongyou Ean, Yunfeng Lu, Kelly Simmons-Potter, B. G. Potter Jr., Alan J. Hurd, C. Jeffrey Blinker, Optically Defined Multifunctional Patterning of Photosensitive Thin-Film Silica Mesophases, Science, 290 (2000), 107-111. [Pg.292]

When micron or sub-micron size electrodes are used, it can sometimes be very difficult to optically define the radius of the electrode. It is thus useful to use available analytical expressions to determine these values (as in equation 6.3.1.1) or to monitor decreases in electrode active area as a result of adsorption processes (4). [Pg.196]

The publications in this field indicate clearly improved performance of the physical side of the analysis, that is, shorter analysis times, better separation efficiencies and a dramatically reduced consumption of reagents. Furthermore, due to the minute volumes for internal connections, new types of combinations can be used, and small samples can be analyzed with success. TTie use of parallel [57, 70, 71] or multi-dimensional arrangements [72] would lead to even larger munbers of analyses per unit time, or to dramatically increased peak capacities (separation of > 1,000 components [73]). The trend to combine biological assays with separation methods, that is, protein protein interactions, enzymes or antibodies with CE [74, 75, 76], could lead to novel concepts for chemical sensing. Optically defined sample plugs allow for precise small volume injections for millisecond separations [55], which can be used for on-line or in-vivo monitoring experiments [77]. Novel approaches to control the flow, e.g., radial control of electroosmosis in capillaries [78] or inductive mechanical micro piunps [79, 80], will allow access to novel cyclic separation techniques. [Pg.23]

VIEEW (Video Image Enhanced Evaluation of Weathering) is a digital macro scale image analysis system allowing objective, visual evaluations for applications such as automotive clearcoat analysis, texture analysis, delamination, chalking, and defect analysis [243]. VIEEW allows visualisation of chromatic and geometric information, optically defines surface defects, eliminates human subjectivity, and supplies reproducible quantitative data. In... [Pg.654]

Doshi D.A., Huesing N.K., Lu M., Fan H., Lu Y., Simmons-Potter K., Potter Jr., B.G., Kurd A.J., Brinker C.J. Optically defined multifunctional patterning of photosensitive thin-film silica mesophases. Science 2000 290 107-111... [Pg.592]

Beam intersection angle of the transmitting optics (defined by the beam separation and the fi ont lens focal length)... [Pg.235]

Umhauer, H., Particle Size Distribution Analysis by Scattered Light Measurements Using an Optically Defined Measuring Volume, J., 4ero5o/5a., 1983, 14, 765-770. [Pg.221]

We need to point out that, if the wavelengths of laser radiation are less than the size of typical structures on the optical element, the Fresnel model gives a satisfactory approximation for the diffraction of the wave on a flat optical element If we have to work with super-high resolution e-beam generators when the size of a typical structure on the element is less than the wavelengths, in principle, we need to use the Maxwell equations. Now, the calculation of direct problems of diffraction, using the Maxwell equations, are used only in cases when the element has special symmetry (for example circular symmetry). As a rule, the purpose of this calculation in this case is to define the boundary of the Fresnel model approximation. In common cases, the calculation of the diffraction using the Maxwell equation is an extremely complicated problem, even if we use a super computer. [Pg.265]

Here E(t) denotes the applied optical field, and-e andm represent, respectively, the electronic charge and mass. The (angular) frequency oIq defines the resonance of the hamionic component of the response, and y represents a phenomenological damping rate for the oscillator. The nonlinear restoring force has been written in a Taylor expansion the temis + ) correspond to tlie corrections to the hamionic... [Pg.1266]

In order to describe the second-order nonlinear response from the interface of two centrosynnnetric media, the material system may be divided into tlnee regions the interface and the two bulk media. The interface is defined to be the transitional zone where the material properties—such as the electronic structure or molecular orientation of adsorbates—or the electromagnetic fields differ appreciably from the two bulk media. For most systems, this region occurs over a length scale of only a few Angstroms. With respect to the optical radiation, we can thus treat the nonlinearity of the interface as localized to a sheet of polarization. Fonnally, we can describe this sheet by a nonlinear dipole moment per unit area, -P ", which is related to a second-order bulk polarization by hy P - lx, y,r) = y. Flere z is the surface nonnal direction, and the... [Pg.1275]

Figure Bl.5.5 Schematic representation of the phenomenological model for second-order nonlinear optical effects at the interface between two centrosynnnetric media. Input waves at frequencies or and m2, witii corresponding wavevectors /Cj(co and k (o 2), are approaching the interface from medium 1. Nonlinear radiation at frequency co is emitted in directions described by the wavevectors /c Cco ) (reflected in medium 1) and /c2(k>3) (transmitted in medium 2). The linear dielectric constants of media 1, 2 and the interface are denoted by E2, and s, respectively. The figure shows the vz-plane (the plane of incidence) withz increasing from top to bottom and z = 0 defining the interface. Figure Bl.5.5 Schematic representation of the phenomenological model for second-order nonlinear optical effects at the interface between two centrosynnnetric media. Input waves at frequencies or and m2, witii corresponding wavevectors /Cj(co and k (o 2), are approaching the interface from medium 1. Nonlinear radiation at frequency co is emitted in directions described by the wavevectors /c Cco ) (reflected in medium 1) and /c2(k>3) (transmitted in medium 2). The linear dielectric constants of media 1, 2 and the interface are denoted by E2, and s, respectively. The figure shows the vz-plane (the plane of incidence) withz increasing from top to bottom and z = 0 defining the interface.
The linear and nonlinear optical responses for this problem are defined by e, 2, e and respectively, as indicated in figure Bl.5.5. In order to detemiine the nonlinear radiation, we need to introduce appropriate pump radiation fields E(m ) and (co2)- If these pump beams are well-collimated, they will give rise to well-collimated radiation emitted tlirough the surface nonlmear response. Because the nonlinear response is present only in a thin layer, phase matching [37] considerations are unimportant and nonlinear emission will be present in both transmitted and reflected directions. [Pg.1277]

The velocity distribution/(v) depends on the conditions of the experiment. In cell and trap experiments it is usually a Maxwell-Boltzmann distribution at some well defined temperature, but /(v) in atomic beam experiments, arising from optical excitation velocity selection, deviates radically from the nonnal thennal distribution [471. The actual signal count rate, relates to the rate coefficient through... [Pg.2476]

Sharpness. This describes the steepness of the electro-optical switching as a function of voltage. This is defined in tenns of the ratio of voltages required to achieve 90% compared to 10% transmission of light. This ratio should be as close to unity as possible. [Pg.2563]

This wave equation is tire basis of all wave optics and defines tire fimdamental stmcture of electromagnetic tlieory witli tire scalar function U representing any of tire components of tire vector functions E and H. (Note tliat equation (C2.15.5) can be easily derived by taking tire curl of equation (C2.15.1) and equation (C2.15.2) and substituting relations (C2.15.3) and (C2.15.4) into tire results.)... [Pg.2854]


See other pages where Optics, defined is mentioned: [Pg.27]    [Pg.10]    [Pg.484]    [Pg.141]    [Pg.65]    [Pg.65]    [Pg.173]    [Pg.562]    [Pg.170]    [Pg.184]    [Pg.302]    [Pg.188]    [Pg.311]    [Pg.194]    [Pg.171]    [Pg.27]    [Pg.10]    [Pg.484]    [Pg.141]    [Pg.65]    [Pg.65]    [Pg.173]    [Pg.562]    [Pg.170]    [Pg.184]    [Pg.302]    [Pg.188]    [Pg.311]    [Pg.194]    [Pg.171]    [Pg.670]    [Pg.887]    [Pg.1211]    [Pg.1269]    [Pg.1276]    [Pg.1297]    [Pg.1541]    [Pg.1657]    [Pg.1659]    [Pg.2024]    [Pg.2073]    [Pg.2208]    [Pg.2417]    [Pg.2456]    [Pg.2463]    [Pg.2501]    [Pg.2685]    [Pg.2853]   
See also in sourсe #XX -- [ Pg.109 ]




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