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[294] P Nordlander, N J Halas, E Prodan, and C Radlo , A Hybridization Model for the Plasmon Response of Complex Nanostructures, Science, Oct 17, 2003 [295] T Prasad, V Colvin, and D Mittleman, Superprism Phenomenon in ThreeDimensional Macroporous Polymer Photonic Crystals, Phys Rev B 67, 165103 (2003); also in Apr 21, 2003, issue of the Virtual Journal of Nanoscale Science and Technology [296] T W Ebbesen, H J Lezec, H F Ghaemi, T Thio, and P AWol , Extraordinary Optical Transmission Through Sub-Wavelength Hole Arrays, Nature 391, 667 (1998) [297] A K Sarychev, V A Podolskiy, A M Dykhe, and V M Shalaev Resonance Transmittance Through Metal Film with Subwavelength Holes, IEEE J Quantum Electron 38, 956 963 (2002) [298] Scientists Announce First 3-D Assembly of Magnetic and Semiconducting Nanoparticles, Press Release, National Science Foundation, Nature, June 26, 2003 [299] D.

1 k k A t = k!

to solve for the cij. This set of equations can be expressed in the form of a matrix equation: HC SCE where H, S, C, and E are matrices of Coulomb integrals, overlap integrals, the cij, and the E , respectively. E.2.2 Hartree Fock (HF) Approach

Screw Tip!

The only two primary aberrations contained in this expression are astigmatism (n 2; l 2) and coma n 3; l 1 , in addition to a tilt of the wavefront about the x axis n 1; l 1 that we may ignore, thus obtaining OPD r; y 2a22 r2 sin 2y sin f 2a31 r3 sin y sin which can also be written as p p f OPD r; y 2a22 r2 cos 2 y sin f 2a31 r3 cos y sin 4 2 2 5:24 f 2 5:23

Davidov, Speci c Topics Related to Nanoscience and Nanotechnology, Racah Institute of Physics, Hebrew University of Jerusalem, Jerusalem, Israel, http://condmatphyshujiacil/davidov/ [300] K Constant, Photonic Band Gap Structures (PBG Structures), Iowa State University (Dept of Material Science and Engineering), Ames Lab (USDOE)/O ce of Basic Energy Sciences [301] Y Fink, The Many Colors of Photonic Bandgap Fibers: Theory, Materials, Processing, Characterization and Applications, Summer 2003 IEEE LEOS Summer Topicals Meeting Series Holey Fibers and Photonic Crystals, Holey Fibers and Photonic Crystals Advance Program, Massachusetts Institute of Technology, Vancouver, Canada, July 14, 2003 [302] M Hatcher, Holey Fiber Delivers Industrial Laser, Opto and Laser Europe Magazine, Dec 2002, p 18 [303] S A Maier, M L Brongersma, P G Kik, S Meltzer, A A G Requicha, and H A Atwater, Plasmonics A Route to Nanoscale Optical Devices, Adv Mater 13(19) (2001) [303a] H.

1. Use ab18-08.dwg if you have it open from the previous exercise. Otherwise, open it from the Results folder of the CD-ROM. 2. Save the drawing as ab18-09.dwg in your AutoCAD Bible folder. 3. Type attdia . If it s currently set to 0, type 1 . 4. Choose Insert Block from the Draw toolbar. Chose ARMCHAIR from the Name drop-down list. Verify that the Specify On-screen option is checked only for Insertion Point, and click OK. 5. Pick a point in front of the desk (turn off OSNAP if necessary) to insert the armchair, and open the Enter Attributes dialog box, as shown in Figure 18-33. The values that were entered when the attributes were defined are displayed, but you can change them.

The post-adaptation nonlinearities are similar in form to those in CIECAM97s, but slightly modi ed to produce a simple power-function response over a larger dynamic range. This facilitates a simple de nition of saturation later in the model. For much of the normal operating range of these functions, the are similar to simple square-root functions. These nonlinearities are given in Equations 16.15 16.17. Ra = Ga = Ba = 400(FL R /100)0.42 + 0.1 27.13 + (FL R /100)0.42 400(FLG /100)0.42 + 0.1 27.13 + (FLG /100)0.42 400(FL B /100)0.42 + 0.1 27.13 + (FL B /100)0.42 (16.15)