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Titlebook: Classical and Stochastic Laplacian Growth; Björn Gustafsson,Razvan Teodorescu,Alexander Vasil Book 2014 Springer International Publishing

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https://doi.org/10.1007/978-3-319-08287-5Laplacian growth model; balayage; free-boundary problems; inverse-moment problem; random matrices; stocha
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Introduction and Background,e . acts over an area ., then the ratio between the tangential component of . and . gives a shear stress across the liquid. The liquid’s response to this applied shear stress is to flow. In contrast, a solid body undergoes a definite displacement or breaks completely when subject to a shear stress.
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Rational and Other Explicit Strong Solutions,ith the classical ones of Polubarinova-Kochina [438], [439], Galin [199] and Saffman, Taylor [488], [489]. Some properties of polynomial and rational solutions will be discussed, and it will be proved that the property of the conformal map to the fluid domain of being a polynomial or a rational func
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Geometric Properties,pretations are considered. In particular, we ask the following question: which geometrical properties are preserved during the time evolution of the moving boundary? We also discuss the geometry of weak solutions.
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Capacities and Isoperimetric Inequalities,side by the (straight) Mediterranean coast and agreed to pay a fixed sum for as much land as could be enclosed by a bull’s hide. Both statements can be expressed in a more algebraic form which indeed underlines the fact that they are equivalent.
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Laplacian Growth and Random Matrix Theory,lation to the multi-particle wavefunction description of the Quantum Hall Effect, in the single-Landau level approximation. As pointed out in [551], the classical Laplacian growth and its stochastic variant based on the normal random matrix theory (NRMT) can be identified to the dispersionless limit
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