并排上下
发表于 2025-3-28 18:37:00
Natalie J. Garton,Michael R. Barerover time of a shallow water wave. This equation has its roots in Scott Russel’s horseback journey along the Edinburgh to Glasgow canal; he followed a wave created by the prow of a boat, which . refused to change its shape over miles. This revival in the 60’s was driven by a discovery of Kruskal and
制定法律
发表于 2025-3-28 22:08:26
Otto Geigerone, {.., ..} = {.., ..} = 0 and {.., ..} = .., where 1 ≤ . ≤ .. For a mechanical interpretation, consider . unit mass particles on a circle that are connected by exponential springs. In , Bogoyavlensky proposed a Lie algebraic generalization, where the original Toda lattice corresponds to the r
四目在模仿
发表于 2025-3-28 23:49:39
Claire Rossi,Hélène Cazzola,Nicola J. Holden,Yannick Rosseznctions on .. and (.., ..., .., .. ..., ..) are linear coordinates on ... He observed that if . and . are two first integrals of a mechanical system (defined on ..) then their . {.} is also a first integral. Notice that the Poisson bracket also allows one to describe the equations of motion in their
出没
发表于 2025-3-29 03:49:22
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花费
发表于 2025-3-29 08:43:24
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fidelity
发表于 2025-3-29 15:02:01
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最有利
发表于 2025-3-29 19:11:59
Howard Goldfine by the method of Example 2.1.8(i) as the Euler characteristic of suitable 2-extensions, called the . lying in.for r ≥ 1, where . is a Galois extension with group .(.). Actually, when . is a .-adic local field K. (.) is not a finitely generated .[.(.)]-module and so one applies the construction of E
Exclaim
发表于 2025-3-29 21:24:47
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强化
发表于 2025-3-30 01:07:04
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Monotonous
发表于 2025-3-30 05:46:36
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