Titlebook: Stochastic Spectral Theory for Selfadjoint Feller Operators; A Functional Integra Michael Demuth,Jan A. Casteren Book 2000 Birkhäuser Verla

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Michael Demuth,Jan A. van Casterentflow occurs even in the case of a rather large hydromagnetic stability reserve [1–3]. This outflow can be described by the Kruskal—Shafranov criterion, which states that the so-called macroscopical plasma stability is reached when no oscillations occur in the overall characteristics of the discharg

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Michael Demuth,Jan A. van Casterentric interface. Globally, the SPR-based sensing platforms have drawn considerable attention due to their versatility, high sensitivity, and reusable probes. In recent years, 2D nanomaterials (particularly graphene and transition metal dichalcogenides [TMDCs]) have been studied extensively for tuning

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Michael Demuth,Jan A. van Casterenoined. Because these mate­ rials exhibit non-linear and often synergistic properties, they have found increasing application in our technology. Their multifarious uses have, in turn, spurred new research efforts, to find yet different ways of joining two kinds of polymer molecules, with novel physic

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Michael Demuth,Jan A. van Casterend and/or joined. Because these mate­ rials exhibit non-linear and often synergistic properties, they have found increasing application in our technology. Their multifarious uses have, in turn, spurred new research efforts, to find yet different ways of joining two kinds of polymer molecules, with no

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Michael Demuth,Jan A. van Casterend and/or joined. Because these mate­ rials exhibit non-linear and often synergistic properties, they have found increasing application in our technology. Their multifarious uses have, in turn, spurred new research efforts, to find yet different ways of joining two kinds of polymer molecules, with no

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Perturbations of Free Feller Operators,BASSA. An advantage, as described in the previous chapter, is that we are able to consider a large class of generators of Feller semigroups. Among others this class contains all the examples of section C in Chapter 1. The regular and singular perturbations are introduced stochastically via the Feynm

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