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Resonance. Spectrally sensitive absorption, transmission, and re ection may arise in optical devices and materials as a result of microscopic optical and electronic properties rather than macroscopic optical design. Resonant effects are created by optical cavities and nanostructures or by quantum mechanical materials processes. These effects are used to create spectroscopic lters. Thin- lm lters, organic dyes, metal nanoparticles, and semiconductor quantum dots are the most common such devices in current practice. Spectral analysis may be implemented by using electronic detectors with intrinsic spectral sensitivity, as in the Foveon X3 direct image sensor. Under the rubics photonic crystals, metamaterials, quantum dots, plasmonics, and volume holography, current research focuses on coding the spectral response of materials that are arti cially structured in multiple dimensions. Structured materials for spectroscopy are discussed in Sections 9.6 and 9.8.

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NOTE Where appropriate, try to set neutral end points first by using the eyedroppers in Curves or Levels.

10k 11k 12k 13k 15k 16k 18 k 20k 22k 24k 27k 30 k 33k 36k 39 k 43k 47k 51k 56k 62k 68 k 75k 82k 9 1k

The text also uses speci c shortcuts for choosing commands:

(7.8)

You can move to any record by scrolling through the records and positioning your cursor on the desired record. With a large table, scrolling through all the records might take a while, so you ll want to use other methods to get to speci c records quickly.

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Until 1952, a patentable idea required only novelty and utility. Congress added nonobviousness in that year as a further requirement; 35 U.S.C. 103 provides that

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Assume that the entropy expression is a generalized version of (7.144),

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Problem VI.11 (Property of the DFT) Use expression (27.17) to establish (28.24). Problem V1.12 (Block LMS) Recall from the discussions in Sec. 27.1 that our motivation is to estimate the weight vector g in (27.1) in an efficient manner. The block recursions (28.6)-(28.8) provide one efficient DFT-based solution. Assume B = M , in which case the subband filters { l k , n - l } in Fig. 28.1 have a single coefficient each. Let wn denote the M x 1estimate of the weight vector g at block iteration n. In view of the result of hob. VI.10, the entries of the M x 1 timedomain estimate wn and the entries of the 2M x 1 frequency-domain estimate En can be assumed to be related to each other as follows:

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This drawing of a base assembly for a commercial washing machine has objects that can be linked to the database of parts.

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d kBT-X , : n ( z ) = drj we recover (8.149)-(8.151).

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