<p>It is known that if <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(f: \mathbb {S}^{1} \rightarrow \mathbb {S}^{1}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>f</mi> <mo>:</mo> <msup> <mrow> <mi mathvariant="double-struck">S</mi> </mrow> <mn>1</mn> </msup> <mo stretchy="false">→</mo> <msup> <mrow> <mi mathvariant="double-struck">S</mi> </mrow> <mn>1</mn> </msup> </mrow> </math></EquationSource> </InlineEquation> is a transitive <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(C^{1+\alpha }\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>C</mi> <mrow> <mn>1</mn> <mo>+</mo> <mi>α</mi> </mrow> </msup> </math></EquationSource> </InlineEquation>-local diffeomorphism non-invertible and non-uniformly expanding, then there is a unique parameter <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(t_{0} \in (0, 1]\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>t</mi> <mn>0</mn> </msub> <mo>∈</mo> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo stretchy="false">]</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> such that the topological pressure function <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\mathbb {R} \ni t \mapsto P_{top}(f, -t\log |Df|)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="double-struck">R</mi> <mo>∋</mo> <mi>t</mi> <mo>↦</mo> <msub> <mi>P</mi> <mrow> <mi mathvariant="italic">top</mi> </mrow> </msub> <mrow> <mo stretchy="false">(</mo> <mi>f</mi> <mo>,</mo> <mo>-</mo> <mi>t</mi> <mo>log</mo> <mo stretchy="false">|</mo> <mi>D</mi> <mi>f</mi> <mo stretchy="false">|</mo> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> is not analytic, in particular <i>f</i> has a phase transition with respect to potential <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\phi := -\log |Df|\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ϕ</mi> <mo>:</mo> <mo>=</mo> <mo>-</mo> <mo>log</mo> <mo stretchy="false">|</mo> <mi>D</mi> <mi>f</mi> <mo stretchy="false">|</mo> </mrow> </math></EquationSource> </InlineEquation>. On the other hand, it is known that for continuous potentials, the topological pressure function can exhibit an infinite number of phase transitions. In this paper, we study the possibilities of the behaviour of the topological pressure function and transfer operator for transitive local diffeomorphism with break points on the circle and Hölder continuous potentials. In particular, we showed that: (1) there is an open and dense subset of continuous potentials such that if a Hölder continuous potential belongs to this subset, then it has no phase transition and the transfer operator has the spectral gap property; (2) if a Hölder continuous potential has a phase transition, then the topological pressure function and the associated transfer operator are described. Consequently, every Hölder continuous potential has at most two phase transitions and the set of smooth potentials such that <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\mathcal {L}_{f,\phi }\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="script">L</mi> <mrow> <mi>f</mi> <mo>,</mo> <mi>ϕ</mi> </mrow> </msub> </math></EquationSource> </InlineEquation> has the spectral gap property, acting on the Hölder continuous space, is dense in the uniform topology. Furthermore, we obtain applications for multifractal analysis of the Birkhoff average.</p>

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Phase transitions for transitive local diffeomorphism with break points on the circle and Hölder continuous potentials

  • Thiago Bomfim,
  • Afonso Fernandes

摘要

It is known that if \(f: \mathbb {S}^{1} \rightarrow \mathbb {S}^{1}\) f : S 1 S 1 is a transitive \(C^{1+\alpha }\) C 1 + α -local diffeomorphism non-invertible and non-uniformly expanding, then there is a unique parameter \(t_{0} \in (0, 1]\) t 0 ( 0 , 1 ] such that the topological pressure function \(\mathbb {R} \ni t \mapsto P_{top}(f, -t\log |Df|)\) R t P top ( f , - t log | D f | ) is not analytic, in particular f has a phase transition with respect to potential \(\phi := -\log |Df|\) ϕ : = - log | D f | . On the other hand, it is known that for continuous potentials, the topological pressure function can exhibit an infinite number of phase transitions. In this paper, we study the possibilities of the behaviour of the topological pressure function and transfer operator for transitive local diffeomorphism with break points on the circle and Hölder continuous potentials. In particular, we showed that: (1) there is an open and dense subset of continuous potentials such that if a Hölder continuous potential belongs to this subset, then it has no phase transition and the transfer operator has the spectral gap property; (2) if a Hölder continuous potential has a phase transition, then the topological pressure function and the associated transfer operator are described. Consequently, every Hölder continuous potential has at most two phase transitions and the set of smooth potentials such that \(\mathcal {L}_{f,\phi }\) L f , ϕ has the spectral gap property, acting on the Hölder continuous space, is dense in the uniform topology. Furthermore, we obtain applications for multifractal analysis of the Birkhoff average.