Titlebook: Reviews of Physiology, Biochemistry and Pharmacology; Volume: 88 R. H. Adrian,E. Helmreich,A. Weber Book 1981 The Editor(s) (if applicable)

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ich form the central focus of this book — namely . of spatial interaction behavior. To do so, we begin by recalling from the discussion following the Poisson Characterization Theorem in Chapter 1 that each independent interaction process, . = {.:. ∈ .}, is completely characterized by its associated

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Event-related slow (DC) potentials in the human brain,

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Reviews of Physiology, Biochemistry and PharmacologyVolume: 88

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refraction

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K. Michael Spyerterizations of exponential gravity representations in Section 2.4.3 of Chapter 2 are then established in Theorem 4.3. Finally in Section 4.6, the generalizations of gravity models discussed in Sections 2.5.2 and 2.5.3 of Chapter 2 are formally developed within the framework of Chapter 3.

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Manfred Haider,Elisabeth Groll-Knapp,Josef A. Ganglbergerfrequencies for the separation configuration defined by distances, . then each of these expressions is seen to constitute an explicit (finite parameter) model of mean interaction frequencies. More generally, even for spatial interaction processes in which the axioms of frequency independence and/or

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Klaus Starketerizations of exponential gravity representations in Section 2.4.3 of Chapter 2 are then established in Theorem 4.3. Finally in Section 4.6, the generalizations of gravity models discussed in Sections 2.5.2 and 2.5.3 of Chapter 2 are formally developed within the framework of Chapter 3.

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frequencies for the separation configuration defined by distances, . then each of these expressions is seen to constitute an explicit (finite parameter) model of mean interaction frequencies. More generally, even for spatial interaction processes in which the axioms of frequency independence and/or