... we use the lattice equations 3 11 d 2 ui (n, t ) = ALjkl R D-,- uk (m, t )+ M i L dt ... j j =1 +A L 1 j =1 L 1 3 R D -,- L 11 u j (m, t ) + A ji L 2 L 2 j =1 R -,+,- L 3 R ...
... Phys. 45 333952 [11] Zaslavsky G M 1994 Fractional kinetic equation for hamiltonian ... Simul. 11 at press [26] Korabel N, Zaslavsky G M and Tarasov V E 2006 Coupled ...
... m( + ) (13) 344 V. E. Tarasov The omega function for system (11) is defined by n = k=1 f gk + qk p k k , (14) and describes the ... 9. G. M. Zaslavsky and M. Edelman, Chaos 11, 295 (2001). 10. R. Nigmatullin, Phys. Stat. Solidi B 133, 425 (1986). ...
... Russian version of the program is here . Организаторы: ЛИТ ОИЯИ, ВМК и НИИЯФ МГУ . 24-25 мая 2007 г. 1. 11:00-11:20 . ... Abramov С.А. (Dorodnicyn Computing Centre of RAS), Barkatou M. A. (Universite de Limoges, XLIM, France) D'Alembertian Series ...
... 11:?00-11:?20|Abramov С.А. (Dorodnicyn Computing Centre of RAS), Barkatou M. A. (Universite de Limoges, XLIM, France) D'?Alembertian Series Solutions of LODE with Polynomial Coefficients|љ ...
... 11:?00-11:?20|Abramov С.А. (Dorodnicyn Computing Centre of RAS), Barkatou M. A. (Universite de Limoges, XLIM, France) D'?Alembertian Series Solutions of LODE with Polynomial Coefficients|љ ...
... 11:?00-11:?20|Abramov С.А. (Dorodnicyn Computing Centre of RAS), Barkatou M. A. (Universite de Limoges, XLIM, France) D'?Alembertian Series Solutions of LODE with Polynomial Coefficients|љ ...