By I Prigogine

Advances in Chemical Physics, quantity 127 covers fresh advances on the leading edge of analysis relative to chemical physics. The sequence, Advances in Chemical Physics, offers a discussion board for serious, authoritative reviews of advances in each zone of the self-discipline.

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5 - Geometry of the surface plasmon. In order to have a guided mode, fields should decay exponentially into the metal and insulator regions. e. Hz = 0. 10) x>0. 11) =0. 11) results in K2mi = k2 - co2(ie0emii. 5) one can get the expression for the transverse magnetic field CHAPTER 2 . BACKGROUND INFORMATION VJ component as fcm7C*i 2 2 k - oo \ie0em Hy = ja>e0EMe>at-> —CiKi 2 k - oo2ue0ei e KmX x <0 x>0. From the definition of Km>, factors in the definition of Hy can be further simplified to get — eKmX wt H y = jwe 0 £ M eJ -J**.

2 Some Definitions Throughout the chapter, we will be using nomenclature from operator theory. 3 The reader well versed in operator theory can directly skip to the next section. A linear vector space is a space which is closed under the operations of addition and of multiplication by a scalar. We will call the elements of the space vectors. Spaces need not be finite dimensional—infinite dimensional vector spaces are also possible. For instance, the collection of all square integrable functions f(x) defined on an interval a < x **
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**X=0 We see that U = e_1Le which makes L by definition pseudo-Hermitian [50, 51]. It has 4 Examples on how to calculate operator adjoints can be found in [45, pp. 150-154]. CHAPTER 3. METAL-INSULATOR-METAL MODES 33 been proved that a pseudo-Hermitian operator does not have a real spectrum if &2 is indefinite [50, Th. 3]. 5) as k2 L Hy = Hy. 1) it can be shown that L' is self-adjoint in L2 so that (Hy2\\-'Hyl) = (\JHy2\Hy\) which leads to the generalized eigenvalue problem for the self-adjoint operators L' and e~l as L'Hy = k2ze-lHy where k\ is the eigenvalue. **