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Titlebook: Algebraic Integrability, Painlevé Geometry and Lie Algebras; Mark Adler,Pierre Moerbeke,Pol Vanhaecke Book 2004 Springer-Verlag Berlin Hei

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樓主: cerebellum
11#
發(fā)表于 2025-3-23 10:31:11 | 只看該作者
12#
發(fā)表于 2025-3-23 16:29:36 | 只看該作者
13#
發(fā)表于 2025-3-23 20:24:41 | 只看該作者
14#
發(fā)表于 2025-3-24 00:41:02 | 只看該作者
15#
發(fā)表于 2025-3-24 06:13:11 | 只看該作者
Deep Belief Nets in C++ and CUDA C: Volume 2omials in involution, the Poisson structure, the commuting vector fields) becomes homogeneous upon assigning weights to each of these coordinates. For these systems we will provide methods by means of which one can reveal the whole geometry of the system and prove (or disprove) algebraic complete integrability.
16#
發(fā)表于 2025-3-24 10:31:44 | 只看該作者
Weight Homogeneous A.c.i. Systemsomials in involution, the Poisson structure, the commuting vector fields) becomes homogeneous upon assigning weights to each of these coordinates. For these systems we will provide methods by means of which one can reveal the whole geometry of the system and prove (or disprove) algebraic complete integrability.
17#
發(fā)表于 2025-3-24 11:11:58 | 只看該作者
Massachusetts: Going to the Court House,r?dinger operator; it ties in with later developments around coadjoint orbits in the algebra of pseudo-differential operators. Very soon it was realized that this isolated example of a “soliton equation” had many striking properties, leading to an explosion of ideas, following each other at a rapid pace.
18#
發(fā)表于 2025-3-24 16:12:46 | 只看該作者
An Invitation to Deep Active Learning.. The above identity is now known as the .. To see how Poisson’s Theorem follows from the Jacobi identity it suffices to remark that . is a constant of the motion (3.2), precisely if . Poisson-commutes with ., i.e., {.} = 0, since
19#
發(fā)表于 2025-3-24 22:46:53 | 只看該作者
20#
發(fā)表于 2025-3-25 02:34:03 | 只看該作者
Poisson Manifolds.. The above identity is now known as the .. To see how Poisson’s Theorem follows from the Jacobi identity it suffices to remark that . is a constant of the motion (3.2), precisely if . Poisson-commutes with ., i.e., {.} = 0, since
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