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Unmarked spectral rigidity of expanding circle maps

Kostiantyn Drach, Vadim Kaloshin

TL;DR

The paper investigates whether the unmarked length spectrum of a smooth expanding circle map determines its smooth conjugacy class. It proves a local rigidity result: if a map $g$ is close to the linear model $L_d$ and its length spectrum is sufficiently sparse in a quantified $(\beta,\gamma)$-sense, then any nearby map $f$ with the same unmarked spectrum is $C^r$-conjugate to $g$, with the conjugacy gaining $C^r$ regularity. The approach combines a sharp Whitney extension scheme, a quantitative Livšic-type theorem, and an iterative distortion-control framework, carefully preserving a Lebesgue measure normalization along the way. The paper also demonstrates that general unmarked rigidity fails by constructing near-linear counterexamples with identical spectra but non-smooth markings. Together, these results illuminate how spectral data robustly determines smooth structure in one dimension under sparsity, while also highlighting the limits of unmarked spectral rigidity.

Abstract

For a smooth expanding map $f$ of the circle, its (unmarked) length spectrum is defined as the set of logarithms of multipliers of periodic orbits of $f$. This spectrum is analogous to the set of lengths of all closed geodesics on negatively curved surfaces -- the classical length spectrum. In the paper, we prove a length spectral rigidity result for expanding circle maps. Namely, we show that a smooth expanding circle map $f$ of degree $d \ge 2$, under certain assumptions on the sparsity of its length spectrum, cannot be perturbed with an arbitrarily small perturbation (depending on $f$) so that its length spectrum stays the same. The proof uses the Whitney extension theorem, a quantitative Livsic-type theorem, and a novel iterative scheme.

Unmarked spectral rigidity of expanding circle maps

TL;DR

The paper investigates whether the unmarked length spectrum of a smooth expanding circle map determines its smooth conjugacy class. It proves a local rigidity result: if a map is close to the linear model and its length spectrum is sufficiently sparse in a quantified -sense, then any nearby map with the same unmarked spectrum is -conjugate to , with the conjugacy gaining regularity. The approach combines a sharp Whitney extension scheme, a quantitative Livšic-type theorem, and an iterative distortion-control framework, carefully preserving a Lebesgue measure normalization along the way. The paper also demonstrates that general unmarked rigidity fails by constructing near-linear counterexamples with identical spectra but non-smooth markings. Together, these results illuminate how spectral data robustly determines smooth structure in one dimension under sparsity, while also highlighting the limits of unmarked spectral rigidity.

Abstract

For a smooth expanding map of the circle, its (unmarked) length spectrum is defined as the set of logarithms of multipliers of periodic orbits of . This spectrum is analogous to the set of lengths of all closed geodesics on negatively curved surfaces -- the classical length spectrum. In the paper, we prove a length spectral rigidity result for expanding circle maps. Namely, we show that a smooth expanding circle map of degree , under certain assumptions on the sparsity of its length spectrum, cannot be perturbed with an arbitrarily small perturbation (depending on ) so that its length spectrum stays the same. The proof uses the Whitney extension theorem, a quantitative Livsic-type theorem, and a novel iterative scheme.

Paper Structure

This paper contains 24 sections, 25 theorems, 199 equations, 4 figures.

Key Result

Lemma 2.1

Let $f, g \colon \mathbb S^1 \to \mathbb S^1$ be, respectively, a $C^{s,1}$-smooth and $C^{s+1,1}$-smooth maps of the circle (not necessarily bijective), $s \geqslant 1$, and let $h \colon \mathbb S^1 \to \mathbb S^1$ be a $C^{s,1}$-smooth diffeomorphism. Assume that for some $M > 0$. Then $h \circ f \circ h^{-1}$ is $C^{s,1}$-smooth, and there is a constant $T = T(s, M)$ such that

Figures (4)

  • Figure 1: The structure of a $(\beta,\gamma)$-sparse length spectrum at the given level $n$. The subset of $\mathop{\mathrm{\mathscr{L}}}\nolimits_n(f)$ is shown in green. A similar structure holds for $\mathop{\mathrm{\mathscr{L}}}\nolimits(f)$ with overlap.
  • Figure 2: A $(p,p)$-messenger connecting $0$ to $x_i \in \mathbb P^g_n$ is shown in blue, while a $(p,p)$-messenger connecting $0$ to $x_j = g^t(x_i)$ is shown in green. A hybrid messenger (in red) connects $0$, $x_i$ and $x_j = g^t(x_i)$ by shadowing halves of the orbits of blue and green messengers and the orbit $x_i, g(x_i), \ldots, g^t(x_i) = x_j$ (in black).
  • Figure 3: Local inductive adjustments. Note that all for all $k \geqslant \kappa_0$, we have $\widetilde{f}_{k-1} = \widetilde{f}_k$ by the uniqueness of a Lebesgue measure preserving map in the smooth conjugacy class of $f$.
  • Figure 4: The example of two length iso-spectral expanding circle maps that are not smoothly conjugate via an orientation preserving diffeomorphism. The graph of $f(x) = 2x+0.1 \cdot \sin^2(\pi x) \colon [0,1] \to [0,1]$ is shown in orange, and the graph of $g(x) = - f(-x) = 2x-0.1 \cdot \sin^2(\pi x)$ is shown in green. The maps $f$ and $g$ are not smoothly conjugate: the multiplier at the points corresponding to the symbolic sequence $\overline{001}$ of period $3$ for $f$ is $\approx 2.31$ (the orange points), while for $g$ it is $\approx 1.9$ (the green points).

Theorems & Definitions (54)

  • Remark 1.1: On the choice of the sparsity parameters $\beta$ and $\gamma$
  • Remark 1.2: On the final smoothness of $\varphi$
  • Remark 1.3: Beyond expanding circle maps
  • Lemma 2.1
  • proof
  • Lemma 2.2
  • Lemma 2.3: Improvement by density
  • proof
  • Lemma 2.4: À la Rolle
  • proof
  • ...and 44 more