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Non-Markovian Stochastic Reduced Equations on the Fly

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Book cover Stochastic Parameterizing Manifolds and Non-Markovian Reduced Equations

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Abstract

In this chapter, we consider a new stochastic PM candidate obtained as the pullback limit associated with the two-layer backward-forward system of Chap. 4; and we illustrate that the corresponding reduced system, when applied to the stochastic Burgers-type equation introduced in Chap. 6, provides better performances in modeling the dynamics of the resolved modes when compared with those achieved by the reduced system based on \(\widehat{h}^{(1)}_\lambda \). Methodological aspects are presented in Sects. 7.1 and 7.2, where a numerical procedure is described to determine “on the fly” the reduced random vector field (based on \(\widehat{h}^{(2)}_\lambda \)) along a trajectory \(\xi (t,\omega )\) generated by the latter as the time is advanced. This method is particularly useful when no analytic formulas of \(\widehat{h}^{(2)}_\lambda \) are available. The substitutive cornerstone in this case, is the pullback characterization of \(\widehat{h}^{(2)}_\lambda \) given by (4.45), which allows us to update the reduced vector field once \(\xi (t,\omega )\) is known at a particular time instance \(t\). As illustrated on the stochastic Burgers-type equation, it is shown in Sect. 7.5 that the statistics of the large excursions present in the SPDE dynamics projected onto the resolved modes are reproduced with a very good accuracy from simulations of the reduced dynamics based on \(\widehat{h}^{(2)}_\lambda \).

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Notes

  1. 1.

    This trajectory is determined in practice by the initial datum \(\phi \) used for the reduced system, which itself depends on the initial datum \(u_0\) used for the SPDE simulation; see also Remark 6.3.

  2. 2.

    The latter give indeed access to approximations of \(\widehat{u}^{(2)}_{\mathfrak {s}}[\xi _t](T+t, \theta _{-T}\omega ; 0)\), which in turn is aimed to approximate (when \(T\) is sufficiently large) the parameterizing manifold function \(\widehat{h}^{(2)}_\lambda \) evaluated at \(( \xi (t,\omega ), \theta _t \omega )\).

  3. 3.

    For the sake of the discussion here, we have changed \(T\) in (4.50) by \(\tau \) here.

  4. 4.

    Which falls within the same basin of attraction of a stable stationary solution; see Sect. 6.1.

  5. 5.

    See Fig. 7.2 for \(\lambda =1.7 \lambda _{c}\).

  6. 6.

    See discussion after (7.35).

  7. 7.

    The PDFs as simulated from a two-mode Galerkin reduced systemReduced equations!Galerkin are not shown in Fig. 7.4, since, for instance, the estimated PDF of the second mode SPDE dynamics is overestimated by a factor of three, from such a reduced system.

  8. 8.

    Regime A considered in Chap. 6 and Regime B considered in this chapter.

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Correspondence to Mickaël D. Chekroun .

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Chekroun, M.D., Liu, H., Wang, S. (2015). Non-Markovian Stochastic Reduced Equations on the Fly. In: Stochastic Parameterizing Manifolds and Non-Markovian Reduced Equations. SpringerBriefs in Mathematics. Springer, Cham. https://doi.org/10.1007/978-3-319-12520-6_7

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