2014
DOI: 10.1007/978-3-319-11322-7_4
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Kinetic Models in Natural Sciences

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Cited by 7 publications
(7 citation statements)
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“…Let us recall that A is the realization of A = diag{−c j ∂ x } 1≤j≤m on the domain D(A) = {u ∈ W 1 1 (I); u(0) = Ku(1)}. The following theorem for (7) has been proved in [3] (see also [4]) but the proof for any nonnegative matrix K is practically the same. Here we extend this proof to an arbitrary K. However, for the proof in the general case we need to provide basic steps of the proof for nonnegative matrices.…”
Section: Solvability Of (8)mentioning
confidence: 99%
“…Let us recall that A is the realization of A = diag{−c j ∂ x } 1≤j≤m on the domain D(A) = {u ∈ W 1 1 (I); u(0) = Ku(1)}. The following theorem for (7) has been proved in [3] (see also [4]) but the proof for any nonnegative matrix K is practically the same. Here we extend this proof to an arbitrary K. However, for the proof in the general case we need to provide basic steps of the proof for nonnegative matrices.…”
Section: Solvability Of (8)mentioning
confidence: 99%
“…The generation of these semigroups was obtained in [135]. More information on kinetic models can be found in [136].…”
Section: Birth-and-death Modelsmentioning
confidence: 99%
“…We assume that c1 (x, y; z; γ) = c 1 (x, y; z)e(t (1) z , γ\{x, y}), c2 (x; y; γ) = c 2 (x; y)e(t (2) y , γ\x), with…”
Section: Dynamics Of the Correlation Functionsmentioning
confidence: 99%
“…To the best of our knowledge, the microscopic modeling of this kind of merging is performed here for the first time. All previous theories, see, e.g., [1,2,3,4,10,12,13], deal with the densities of the particles and hence do not take into account the corpuscular structure of the system. However, we do not take into account the particle mass, which is supposed to be done in an extension of the present model.…”
Section: Introductionmentioning
confidence: 99%