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Methods A 477, 226 231 (2002) Gostilo, V, Ivanov, V, Kostenko, S, Lisjutin, I, Loupilov, A, Nenonen, S, Sipila, H and Valpas, K, Technological aspects of development of pixel and strip detectors based on CdTe and CdZnTe Nucl Instrum Methods A 460, 27 34 (2001) Gryboo, P and D browski, W, Development of fully intea grated readout system for high count rate position-sensitive measurements of X-rays using silicon strip detectors IEEE Trans Nucl Sci 48, 466 472 (2001) Grybo , P, D browski, W, Hottowy, P, Szczygie , R, s a e Swi tek, K and Wi cek, P, Multichannel mixed-mode IC a for digital readout of silicon strip detectors Microelectron Reliabil 42, 427 436 (2002) He, Z, Review of the Shockley Ramo theorem and its application in semiconductor gamma-ray detectors Nucl Instrum.

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Methods A 463, 250 267 (2001) Hilt, B, Fessler, P and Pr vot, G The quantum X-ray radie ology apparatus Nucl Instrum Methods A 442, 355 359 (2000) Kalemci, E and Matteson, JL, Investigation of charge sharing among electrode strips for a CdZnTe detector Nucl Instrum Methods A 460, 527 537 (2002) Lin, WT, Chang, Y-H, Chen, AE, Hou, SR, Lin, C-H, Kulinich, P, Ryan, J, Steinberg, P, Wadsworth B and Wyslouch, B, Development of a double metal AC-coupled silicon pad detector Nucl Instrum Methods A 389, 415 420 (1997) Lozano, ME, Cabruja, A, Collado, J Santander and Ullan, M, Bump bonding of pixel systems Nucl Instrum Methods A 473, 95 101 (2001) Luke, PN, Amman, M, Lee, JS, Ludewight, BA.

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and Yaver, H, A CdZnTe coplanar-grid detector array for environmental remediation Nucl Instrum Methods A 458, 319 324 (2001) Macri, JR, Dufour, P, Hamel, LA, Julien, M, McConnell, ML, McClish, M, Ryan, JM and Widhom, M, Study of 5 and 10 mm thick CZT strip detectors Presented at the 12th International Workshop on Room-Temperature Semiconductor X- and Gamma-Ray Detectors, San Diego, paper R8 8, (2001)..

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The factor 6 comes from the number of voltages in a coherent group. Coef cient a3 comes from Eq. (4.1). The next term and the factor 2B is from the product of the S0 /2 and S2 (0)/2, the density of the input (Fig. 5.2) and the density at the center to the second-order triangle (Fig. 5.4a). The term R 2 results from the conversion of S0 to a mean-squared voltage (generating R 3 ) and reconversion of the product to a power density (generating 1/R), much as occurred in Eq. (5.12). The factor 3 represents the ratio of average-to-peak value for the triangle in 4 the region B/2 so that multiplication by 3 B amounts to integration over that 4 bandwidth. The factor 3 adds the product of the smaller triangle and rectangle 2 to that of the larger triangle and rectangle. This can be simpli ed to S3 (0) 27 2 = a3 R 2 2 2 = 27 8 S0 2 2 3RpIIP3,IM

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