Abstract
As in Chapters 4 and 5, we consider a diffeomorphism on a hyperbolic basic set and a differentiable weight. In this chapter, we study the associated weighted dynamical determinant, giving a lower bound on the disc in which this determinant is analytic and where its zeroes admit a spectral interpretation. We apply the results obtained on the weighted dynamical determinant to study the dynamical zeta function.
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Notes
- 1.
Or an \(C^{r}\) Anosov diffeomorphism on a connected manifold \(M\), not necessarily transitive.
- 2.
This is the same definition as (3.4) in the expanding case, except that \(|\det(\mathrm{Id}-DT^{-m}(x))|\) there is replaced by \(|\det(\mathrm{Id}-DT^{m}(x))|\) here. This is because the transfer operator \(\mathcal{L}_{g}\) is now defined by forward composition with \(T\).
- 3.
By Lemma A.3 and the perturbation results from §5.3 one can construct examples of \(C^{r}\) hyperbolic diffeomorphisms with nontrivial resonances for \(r<\infty\).
- 4.
- 5.
See (6.40) below for a more precise estimate.
- 6.
As usual, if \(\inf|g||_{\Lambda}=0\) we approach \(|g|\) by non-vanishing functions. See Appendix B
- 7.
The decomposition is independent of \(t\) and \(s\).
- 8.
- 9.
- 10.
Or see Footnote 19.
- 11.
- 12.
To write a formal proof involving charts, we may integrate by parts as many times as we like with respect to \(x\) in the relevant kernels, as in the second step of the proof of Lemma 6.9.
- 13.
- 14.
Note that \(\mathrm{tr}\, \,\mathbb{T}_{x}^{m}\ne0\) only if \(x\in V\). If \(T^{m}(x)=x\) this implies \(x\in\Lambda\).
- 15.
For the sake of comparison with [88], note that their transfer operator is defined by composing with \(T^{-1}\) so \(E^{s}\) there replaces \(E^{u}\) here.
- 16.
- 17.
Kitaev worked in the slightly more general setting of Mixed Transfer Operators.
- 18.
In this respect, [68, Remark 2 after Thm 5] should be taken with a grain of salt.
References
Adam, A.: Generic non-trivial resonances for Anosov diffeomorphisms. Nonlinearity 30, 1146–1164 (2017)
Baillif, M.: Kneading operators, sharp determinants, and weighted Lefschetz zeta functions in higher dimensions. Duke Math. J. 124, 145–175 (2004)
Baladi, V.: Periodic orbits and dynamical spectra. Ergodic Theory Dynam. Systems 18, 255–292 (1998)
Baladi, V.: The quest for the ultimate anisotropic Banach space. J. Stat. Phys. Special Volume for D. Ruelle and Ya. Sinai 166, 525–557 (2017)
Baladi, V., Kitaev, A., Ruelle, D., Semmes, S.: Sharp determinants and kneading operators for holomorphic maps. Tr. Mat. Inst. Steklova 216, Din. Sist. i Smezhnye Vopr., 193–235 (1997); translation in Proc. Steklov Inst. Math. 216, 186–228 (1997)
Baladi, V., Ruelle, D., Sharp determinants. Invent. Math. 123, 553–574 (1996)
Baladi, V., Tsujii, M.: Dynamical determinants for hyperbolic diffeomorphisms via dyadic decomposition, unpublished manuscript (2005)
Baladi, V., Tsujii, M.: Dynamical determinants and spectrum for hyperbolic diffeomorphisms. In: Burns, K., Dolgopyat, D., Pesin, Ya. (eds.) Probabilistic and Geometric Structures in Dynamics, pp. 29–68, Contemp. Math., 469, Amer. Math. Soc., Providence, RI (2008)
Bowen, R.: Some systems with unique equilibrium states. Math. Systems Theory 8, 193–202 (1974–1975).
Dang, N.V., Rivière, G.: Spectral analysis of Morse-Smale gradient flows. arXiv:1605.05516
Dang, N.V., Rivière, G.: Pollicott-Ruelle spectrum and Witten Laplacians. arXiv:1709.04265
Dyatlov, S., Zworski, M.: Dynamical zeta functions for Anosov flows via microlocal analysis. Annales ENS 49, 543–577 (2016)
Faure, F., Roy, N.: Ruelle–Pollicott resonances for real analytic hyperbolic maps. Nonlinearity 19, 1233–1252 (2006)
Faure, F., Roy, N., Sjöstrand, J.: Semi-classical approach for Anosov diffeomorphisms and Ruelle resonances. Open Math. J. 1, 35–81 (2008)
Faure, F., Tsujii, M.: Prequantum transfer operator for symplectic Anosov diffeomorphism. Astérisque No. 375. Soc. Math. France, Paris (2015)
Faure, F., Tsujii, M.: Band structure of the Ruelle spectrum of contact Anosov flows. C.R. Acad. Sci. Paris, Ser. I. 351, 385–391 (2013)
Faure, F., Tsujii, M.: The semiclassical zeta function for geodesic flows on negatively curved manifolds. Invent. Math. 208, 851–998 (2017)
Fried, D.: The zeta functions of Ruelle and Selberg I. Ann. Sci. École Norm. Sup. (4) 19, 491–517 (1986)
Fried, D.: Meromorphic zeta functions for analytic flows. Comm. Math. Phys. 174, 161–190 (1995)
Fried, D.: The flat-trace asymptotics of a uniform system of contractions. Ergodic Theory Dynam. Systems 15, 1061–1073 (1995)
Giulietti, P., Liverani, C., Pollicott, M.: Anosov flows and dynamical zeta functions. Annals of Mathematics 178, 687–773 (2013)
Gouëzel, S., Liverani, C.: Banach spaces adapted to Anosov systems. Ergodic Theory Dynam. Systems 26, 189–217 (2006)
Gouëzel, S., Liverani, C.: Compact locally maximal hyperbolic sets for smooth maps: fine statistical properties. J. Differential Geom., 79, 433–477 (2008)
Grothendieck, A.: La théorie de Fredholm. Bull. Soc. Math. France 84, 319–384 (1956)
Hille, E: Analytic function theory. Vol. 1. Introduction to Higher Mathematics, Ginn and Company, Boston (1959)
Katok, A., Hasselblatt, B.: Introduction to the Modern Theory of Dynamical Systems. Cambridge University Press, Cambridge (1995)
Kitaev, A.Yu.: Fredholm determinants for hyperbolic diffeomorphisms of finite smoothness. Nonlinearity 12, 141–179 (1999). Corrigendum: “Fredholm determinants for hyperbolic diffeomorphisms of finite smoothness”. Nonlinearity 12, 1717–1719 (1999)
Liverani, C.: Fredholm determinants, Anosov maps and Ruelle resonances. Discrete Contin. Dyn. Syst. 13, 1203–1215 (2005)
Liverani, C., Tsujii, M.: Zeta functions and dynamical systems. Nonlinearity 19, 2467–2473 (2006)
Mayer, D.: The Ruelle–Araki Transfer Operator in Classical Statistical Mechanics. Lecture Notes in Phys. 123, Springer-Verlag, Berlin-New York (1980)
Naud, F.: Anosov diffeomorphisms with non-trivial Ruelle spectrum. Personal communication (June 2015)
Parry, W., Pollicott, M.: Zeta functions and the periodic orbit structure of hyperbolic dynamics. Astérisque No. 187–188. Soc. Math. France, Paris (1990)
Ruelle, D.: Zeta-functions for expanding maps and Anosov flows. Invent. Math. 34, 231–242 (1976)
Rugh, H.H.: The correlation spectrum for hyperbolic analytic maps. Nonlinearity 5, 1237–1263 (1992)
Rugh, H.H.: Generalized Fredholm determinants and Selberg zeta functions for Axiom A dynamical systems. Ergodic Theory Dynam. Systems 16, 805–819 (1996)
Slipantschuk, J., Bandtlow, O.F., Just, W.: Analytic expanding circle maps with explicit spectra. Nonlinearity 26, 3231–3245 (2013)
Slipantschuk, J., Bandtlow, O.F., Just, W.: Complete spectral data for analytic Anosov maps of the torus. Nonlinearity 30, 2667–2686 (2017)
Tangerman, F.: Meromorphic Continuation of Ruelle Zeta Functions (Heat Operators). Ph.D. thesis, Boston (1986)
Tsujii, M.: Quasi-compactness of transfer operators for contact Anosov flows. Nonlinearity 23, 1495–1545 (2010)
Tsujii, M.: Contact Anosov flows and the Fourier-Bros-Iagolnitzer transform. Ergodic Theory Dynam. Systems 32, 2083–2118 (2012)
Walters, P.: An introduction to ergodic theory. Graduate Texts in Mathematics, 79, Springer-Verlag, New York-Berlin (1982)
Zworski, M.: Mathematical study of scattering resonances. Bull. Math. Sci. 7, 1–85 (2017)
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Baladi, V. (2018). Dynamical determinants for smooth hyperbolic dynamics. In: Dynamical Zeta Functions and Dynamical Determinants for Hyperbolic Maps. Ergebnisse der Mathematik und ihrer Grenzgebiete. 3. Folge / A Series of Modern Surveys in Mathematics, vol 68. Springer, Cham. https://doi.org/10.1007/978-3-319-77661-3_6
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