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An aberration of a lens that causes the focal plane to be curved instead of flat 52 Cyanine dyes Fluorescent dyes produced by Amersham, Inc, that are known for their photostability, solubility, and relatively high quantum efficiency 185 Dark count and dark noise In electronic cameras, the photon-independent signal in an image The major constituents of the dark count are the bias signal, thermal noise, and camera read noises from the detector and processing circuits The dark count must be subtracted from a raw image in order to obtain a corrected image based solely on photon-dependent counts The dark noise is defined as the square root of the dark count and remains a part of the corrected image The dark count is determined by acquiring an image (a dark frame) without opening the camera shutter 273 Dark-field microscopy.

The potential windows applicable in the bulk of solutions may be somewhat narrower However, the above tendency must also be true in solutions Thus, in solvents with wide potential windows on the two sides, many redox reactions,.

A mode of light microscopy in which 0th order undeviated light is excluded from the objective, and image formation is based solely on the interference of waves of diffracted light Typically, dark-field optics are obtained by illuminating the object with a steeply pitched cone of light produced with a transparent annulus in an otherwise opaque mask at the condenser front aperture A relatively.

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An image feature is a function that maps an image into a number or a vector (array) Viola and Jones [27] used only features that map images into numbers Moreover, they used some speci c types of features, obtained by selecting several rectangles within the training set, nding the sum of pixel intensities in each rectangle, assigning a positive or negative sign and/or weight to each sum, and then summing them The pixel measurements used by Viola and Jones were the actual grayscale intensities of pixels If the areas of the dark (positive sign) and light (negative sign) regions are not equal, the weight of the lesser region is raised For example, feature 21 in Figure 112 has a twice greater light area than a dark one The area of the dark rectangle in this case would be multiplied by 2 to normalize the feature.

TABLE 3.2 Class Window glass Non-window glass Case Selection Result Samples Correctly Classi ed 158 43 Cases Selected 112 29

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The main problem is to nd which of these features, among the thousands available, would best distinguish positive and negative examples, and how to combine them into a learning machine Figure 112 shows the set of basic shapes used by Viola and Jones [27] Adding features to the feature set can increase the accuracy of the AdaBoost machine at the cost of additional training time Each of the shapes seen in Figure 112 is scaled and translated anywhere in the test images, consequently forming features Therefore, each feature includes a basic shape (as seen in Fig 112), its translated position in the image, and its scaling factors (height and width scaling) These features de ne the separating ability between positive and negative sets This phenomenon is illustrated in Figure 113 Both of the features seen in Figure 11.

For the system of four interconnection lines, an even- and odd-mode excitation can be used to calculate the even- and odd-mode capacitances of each line separately. For the even-mode excitation, each line is assumed to be 1 V potential with respect to the conducting ground plane. For the odd-mode excitation, one line is kept at 1 V while the other three lines are kept at 1 V potential. This means that when nding the odd-mode charge on the rst line, the potential on the rst line is kept at 1 V while the potentials on each of the second, third, and fourth lines are kept at 1 V, and so on. First, the four lines are divided into N1 , N2 , N3 , and N4 number of subsections. Thus, the total number of subsections becomes N N1 N2 N3 N4 Then, the voltage excitation for the even mode of each interconnection line is an N-row unit column matrix, that is, 2 3 1 6.7 . 6.7 6 7 617 6 7 617 6.7 6.7 6.7 617 6 7 617 6 7 6.7 4.5 . 1

As just described, incident rays of linearly polarized light are split by the condenser DIC prism into O- and E-ray pairs, traverse the specimen, and are recombined by the objective DIC prism, generating linearly and elliptically polarized waves that are differentially transmitted by the analyzer according to the azimuths of their vibrational planes. Since transmitted rays are linearly polarized and are plane parallel, they interfere in the image plane and generate an amplitude image of the object. Another useful way of viewing the

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