The basin equality conjecture for sectional-hyperbolic attracting sets

Let G\EuScriptX1(M)G\in\EuScript{X}^1(M) have a trapping region UU whose attracting set Λ=t>0ϕt(U)\Lambda=\cap_{t>0}\phi_t(U) is sectional-hyperbolic. Define the topological basin of attraction by

U={yM:d(ϕty,Λ)t+0}.{\mathcal U}=\{y\in M:d(\phi_t y,\Lambda)\xrightarrow[t\to+\infty]{}0\}.

Assume that there are finitely many hyperbolic periodic points p1,,plp_1,\dots,p_l of Λ\Lambda and ε0>0\varepsilon_0>0, and let

Wcs={Wxs:xW\EuScriptO(pi)u(ε0); i=1,,l}.{\mathcal W}^{cs}=\{W^s_x:x\in W^u_{\EuScript{O}(p_i)}(\varepsilon_0);\ i=1,\dots,l\}.

Here WxsW^s_x is the stable manifold of xx, and W\EuScriptO(pi)u(ε0)W^u_{\EuScript{O}(p_i)}(\varepsilon_0) is the union of the local unstable manifolds of points on the periodic orbit \EuScriptO(pi)\EuScript{O}(p_i).

Basin equality conjecture. For any sectional-hyperbolic attracting set Λ\Lambda, the topological basin of attraction coincides with the family of stable manifolds through the points of local unstable leaves of finitely many periodic orbits:

U=Wcs.{\mathcal U}={\mathcal W}^{cs}.

The preceding theorem proves that Wcs{\mathcal W}^{cs} is open and dense in U{\mathcal U} and, for C1+C^{1+} vector fields, has full volume and contains the basin of every physical probability measure supported in Λ\Lambda. The conjecture asks whether the remaining points of the topological basin are absent.

Sources & referencesView supporting material

Primary source

Vitor Araujo, “Finitely many physical measures for sectional-hyperbolic attracting sets and statistical stability”, arXiv:1901.10537 (2020).

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