30 resultados para Laplace eigenfunctions

em Bulgarian Digital Mathematics Library at IMI-BAS


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2000 Mathematics Subject Classification: 35J05, 35C15, 44P05

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2010 Mathematics Subject Classification: 35G35, 32A30, 30G35.

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The paper has been presented at the 12th International Conference on Applications of Computer Algebra, Varna, Bulgaria, June, 2006

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2000 Mathematics Subject Classification: 42B20, 42B25, 42B35

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2000 Math. Subject Classification: Primary 42B20, 42B25, 42B35

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Mathematics Subject Classification: 33D15, 44A10, 44A20

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MSC 2010: 44A35, 35L20, 35J05, 35J25

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∗The author was partially supported by Alexander von Humboldt Foundation and the Contract MM-516 with the Bulgarian Ministry of Education, Science and Thechnology.

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Architecture and learning algorithm of self-learning spiking neural network in fuzzy clustering task are outlined. Fuzzy receptive neurons for pulse-position transformation of input data are considered. It is proposed to treat a spiking neural network in terms of classical automatic control theory apparatus based on the Laplace transform. It is shown that synapse functioning can be easily modeled by a second order damped response unit. Spiking neuron soma is presented as a threshold detection unit. Thus, the proposed fuzzy spiking neural network is an analog-digital nonlinear pulse-position dynamic system. It is demonstrated how fuzzy probabilistic and possibilistic clustering approaches can be implemented on the base of the presented spiking neural network.

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Mathematics Subject Classification: 26D10.

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Mathematics Subject Classification: 43A20, 26A33 (main), 44A10, 44A15

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2000 Mathematics Subject Classification: 35A15, 44A15, 26A33

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Mathematics Subject Classification: Primary 35R10, Secondary 44A15

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2000 Mathematics Subject Classification: 33D15, 33D90, 39A13

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This survey is devoted to some fractional extensions of the incomplete lumped formulation, the lumped formulation and the formulation of Lauwerier of the temperature field problem in oil strata. The method of integral transforms is used to solve the corresponding boundary value problems for the fractional heat equation. By using Caputo’s differintegration operator and the Laplace transform, new integral forms of the solutions are obtained. In each of the different cases the integrands are expressed in terms of a convolution of two special functions of Wright’s type.