<p>Given two Hölder potentials <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\( \phi _+ \)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>ϕ</mi> <mo>+</mo> </msub> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\( \psi _- \)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>ψ</mi> <mo>-</mo> </msub> </math></EquationSource> </InlineEquation> for the unilateral shift, we define anisotropic Banach spaces of distributions on the bilateral shift space with a finite alphabet. On these spaces, the transfer operator for the bilateral shift is quasicompact with a spectral gap, and the unique Gibbs state associated with <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\( \phi _+ \)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>ϕ</mi> <mo>+</mo> </msub> </math></EquationSource> </InlineEquation> spans its <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\( 1 \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>-eigenspace. This result allows us to establish exponential decay of correlations for Hölder observables and a wide range of measures on the bilateral shift space.</p>

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Anisotropic spaces for the bilateral shift

  • Mateus Marra,
  • Daniel Smania

摘要

Given two Hölder potentials \( \phi _+ \) ϕ + and \( \psi _- \) ψ - for the unilateral shift, we define anisotropic Banach spaces of distributions on the bilateral shift space with a finite alphabet. On these spaces, the transfer operator for the bilateral shift is quasicompact with a spectral gap, and the unique Gibbs state associated with \( \phi _+ \) ϕ + spans its \( 1 \) 1 -eigenspace. This result allows us to establish exponential decay of correlations for Hölder observables and a wide range of measures on the bilateral shift space.