2015
DOI: 10.1007/s10444-015-9425-0
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Geometric integration of non-autonomous linear Hamiltonian problems

Abstract: Symplectic integration of autonomous Hamiltonian systems is a wellknown field of study in geometric numerical integration, but for non-autonomous systems the situation is less clear, since symplectic structure requires an even number of dimensions. We show that one possible extension of symplectic methods in the autonomous setting to the non-autonomous setting is obtained by using canonical transformations. Many existing methods fit into this framework. We also perform experiments which indicate that for expon… Show more

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Cited by 7 publications
(6 citation statements)
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References 28 publications
(54 reference statements)
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“…Ideally, we want to design optimisation methods that preserve these rates, i.e., are "rate-matching", and are also numerically stable. As we will see, such geometric integrators can be constructed by leveraging the shadow Hamiltonian property of symplectic methods on higher-dimensional conservative Hamiltonian systems [9] (see also [98,99]). This holds not only on R 2d but on general settings, namely on arbitrary smooth manifolds [9,10].…”
Section: Rate-matching Integrators For Smooth Optimisationmentioning
confidence: 99%
See 1 more Smart Citation
“…Ideally, we want to design optimisation methods that preserve these rates, i.e., are "rate-matching", and are also numerically stable. As we will see, such geometric integrators can be constructed by leveraging the shadow Hamiltonian property of symplectic methods on higher-dimensional conservative Hamiltonian systems [9] (see also [98,99]). This holds not only on R 2d but on general settings, namely on arbitrary smooth manifolds [9,10].…”
Section: Rate-matching Integrators For Smooth Optimisationmentioning
confidence: 99%
“…The reason for doing this procedure, called symplectification, is purely theoretical: since the theory of symplectic integrators only accounts for conservative systems, we can now extend this theory to dissipative settings by applying a symplectic integrator to (13) and then fixing the relevant coordinates (17) in the resulting method. Geometrically, this corresponds to integrating the time flow exactly [9,98]. In [9] such a procedure was defined under the name of presymplectic integrators, and these connections hold not only for the specific example above but also for general non-conservative Hamiltonian systems.…”
Section: Rate-matching Integrators For Smooth Optimisationmentioning
confidence: 99%
“…From the outset, it might not be so clear which geometric features such a non-autonomous Hamiltonian system has. There seem to be at least two ways to understand this problem [97]. Let us assume that u = (z, p) ∈ T * R M ≡ R M ⊕ R M with 'positions' z and 'momenta' p forming the phase space.…”
Section: Hamiltonian Vector Fieldsmentioning
confidence: 99%
“…Note that these equations are still satisfied along the flow of X H . A presymplectic integrator is, according to Definition 4.1, any symplectic integrator Ψ h for which q 0 , p 0 are integrated exactly (see also [33,34]). Let us denote y ≡ (q µ , p µ ), z ≡ (q i , p i ) and y • ≡ y(s = 0).…”
Section: "Rate-matching" Geometric Integratorsmentioning
confidence: 99%