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Chem. Phys. 104, 1427–1440. 1, C. T. ), CRC Press, Boca Raton, FL (1974). CRC Handbook of Chemistry and Physics (1995) 75th Edition. CRC Press, Boca Raton, FL. de Boer, J. H. (1953) The Dynamical Character of Adsorption. Clarendon Press, Oxford. , Li, X. Y. and MacNee, W. (1998) Ultrafine (nanometre) particle mediated lung injury. J. Aerosol Sci. 29, 553–560. Feynman, R. , Leighton, R. B. and Sands, M. (1965) The Feynman Lectures of Physics, Vol. III. Quantum Mechanics. Addison-Wesley, Reading, MA.

The requirement of materials characterized by the smallest ratio third-order dispersion (and in general higher order dispersion) to GDD, D3/D, greatly stimulated research in material science. Fused silica was found to be the best candidate to be employed in prism-controlled KLM Ti:Sa lasers. For Ti:Sa laser oscillator a pulse duration of 10 fs was reached ([56, 57] among the others). The limitation due to higher order dispersion terms (see Eq. (2-6)), which prevented from obtaining even shorter pulse durations approaching the gain-bandwidth limit of Ti:Sa, was finally overcome with the invention and realization of chirped multilayer dielectric mirrors [58, 59].

They must therefore be regarded as a state of matter which is distinct in its own right. In this state of matter, in particular, we cannot—unlike for much larger entities—approach particles by thinking of them simply in terms of a solid, well-defined surface. There is no such continuum-based description. Rather, the particle must now be regarded as a complex structure 12 FUNDAMENTALS whose properties, and resultant behavior, will depend on the relative positions of the individual molecules in the particle and finally on the structure of the combined electronic charge distribution (probability density).

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Applied Differential Equations by F. E. Relton

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