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Dekker, New York, 2001; (b) Lund, H, Baizer, M M (Eds) Organic Electrochemistry, 3rd edn, Marcel Dekker, New York, 1991 Mann, C K, Barnes, K K Electrochemical Reactions in Non-aqueous Systems, Marcel Dekker, New York, 1970 Meites, L, Zuman, P (Eds) CRC Handbook Series in Organic Electrochemistry, Vols I VI, CRC Press, Boca Raton, FL, 1977 1983 Bard, A J (Ed) Encyclopedia of Electrochemistry of the Elements, Vols I XIV (Organic Section), Marcel Dekker, New York, 1973 1980 For example, (a) Parker, V D Adv Phys Org Chem 1983, 19, 131; (b) Hammerich, O, Ref 47 a, 2; Hammerich, O, Parker, V D, Ref 47 b, 3; (c) Wayner, D D M, Parker, V D Acc Chem Res 1993, 26, 287; (d) Andrieux, C P, Hapiot, P, Sav ant, J-M Chem Rev 1990, 90, 723; (e) Sav ant, J.

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In 3 we employed the concept of Huygens wavelets to describe the location of a secondary wavefront generated by spherical wavelets and originating from a point source of light in a homogeneous medium In a transparent birefringent material, the ordinary or O ray behaves in the same way, generating a spherical wavefront However, the extraordinary or E waves behave differently As described by Huygens in 1690, the expanding wavefront of the E ray at a time t can be described as the surface of an ellipsoid (Fig 8-8) An ellipsoid is the figure generated by rotating an ellipse about its major or minor axis The ellipsoidal form indicates the presence of different velocities for the E ray along different trajectories in the crystal, where the upper- and lower-limit velocities define the long and short axes of the wavefront ellipsoid.

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M Acc Chem Res 1993, 26, 455; (f) Saveant, J-M Adv Phys Org Chem 1990, 26, 1; (g) Evans, D H Chem Rev 1990, 90, 739 (a) Echegoyen, L, Echegoyen, L E Acc Chem Res 1998, 31, 593; Ref 47 a, 7; (b) Reed, C A, Bolskar, R D Chem Rev 2000, 100, 1075 Latest literature on the electrochemistry of fullerenes and their derivatives For example, Peover, M E, in Electroanalytical Chemistry, Vol 2 (Ed A J Bard), Marcel Dekker, New York, 1967, 1 (a) Dubois, D, Kadish, K M, Flanagan, S, Haufler, R E, Chibante, L P F, Wilson, L J J Am Chem Soc 1991, 91, 4364; (b) Dubois, D, Kadish, K M, Flanagan, S, Wilson, LJ J Am Chem Soc 1991, 91, 7773; (c) Dubois, D, Moninot, G, Kutner, W.

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But this much is clear: Leo Melamed and Jack Sandner knew more about the CME, its successful history, its unique innovations, its operational capability, how it works, what it does, and its future potential than anyone on the planet, and we were better equipped from the point of experience and ability to present the CME s case and respond to questions than anyone on that team Nothing succeeds like success Our stock exploded on the scene, doubling in value during its rst year of trading on the NYSE (now listed exclusively on Nasdaq), then.

The long axis corresponds to the direction along which the wavefront reaches its greatest possible velocity through the crystal, and is termed the fast axis, while the short axis corresponds to the direction giving the smallest velocity, and is called the slow axis The velocities of waves traveling in all other directions have intermediate values Since the velocity of light in a medium is described as v c/n, where c is the speed of light in a vacuum and n is the refractive index, we may infer that n is not constant in a birefringent crystal, but varies, depending on the path taken by a ray through the crystal.

, Thomas Jones, M, Kadish, K M J Phys Chem 1992, 96, 7173; (d) Xie, Q, Perex-Cordero, E, Echegoyen, L J Am Chem Soc 1992, 114, 3798; (e) Ohsawa, Y, Saji, T J Chem Soc Chem Commun 1992, 781; (f) Niyazymbetov, ME, Evans, DH, Lerke, SA, Cahill, PA, Henderson, CC J Phys Chem 1994, 98, 13093; (g) Cliffel, D E, Bard, J A J Phys Chem 1994, 98, 8140..

Several additional points about the propagation of wavefronts in a crystal are worth noting: For uniaxial crystals, the O and E wavefronts coincide at either the slow or the fast axis of the ellipsoid, and the difference in surface wavefronts along the propagation axis is termed the optical path difference or relative retardation If the O and E wavefronts coincide at the major axis of the ellipsoid, ne no in directions other than along the optic axis, and the specimen is said to be positively birefringent (Fig 8-9) This is the case for crystals such as quartz and most ordered biological materials For materials such as calcite, whose O and E wavefronts meet at the minor axis of the ellipsoid, no ne in directions other than along the optic axis Such materials are said to exhibit negative birefringence.

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