For a fixed irrational rotation TT of the circle, consider all induced (first-return) maps TAT_A on measurable sets AA of positive measure, topologized through the metric d(A,B)=m(A△B)d(A,B)=m(A\triangle B) on the measure algebra. A question of William Veech, recorded by Petersen (1973) and Conze (1972) and recalled by Knill (2023), asks whether the class of sets AA for which TAT_A has pure point spectrum is dense in this metric. Since the induced maps of an ergodic transformation are generically weakly mixing, this pure point class is meager; the question is whether it is nevertheless dense, as the rationals are in the reals. A positive answer, combined with Simon's Wonderland theorem, would force the generic induced system of a rotation to have purely singular continuous spectrum. The question extends verbatim to any ergodic transformation with pure point spectrum. No resolution of the density question is known in the literature to date.

Background

Let TT be a measure-preserving invertible transformation (automorphism) of a Lebesgue probability space (X,A,m)(X,\mathcal{A},m), that is, a standard non-atomic probability space such as the circle with Lebesgue measure. The map TT is ergodic if every TT-invariant measurable set has measure 00 or 11. The guiding example is the irrational rotation T(x)=x+α mod 1T(x)=x+\alpha \bmod 1 of the circle T\mathbb{T}, which is ergodic exactly when α\alpha is irrational.

For a measurable set AA with m(A)>0m(A)>0, the induced or first-return map TAT_A is the restriction of the dynamics to AA accelerated to successive returns: TA(x)=TrA(x)(x)T_A(x)=T^{r_A(x)}(x), where rA(x)=min⁡{k≥1:Tkx∈A}r_A(x)=\min\{k\ge 1 : T^k x\in A\} is the return-time function. This construction, going back to the 1940s, is the measurable analogue of a Poincaré return map; the original system TT can be rebuilt as a Kakutani skyscraper — a tower whose levels are the successive translates of AA between returns — over TAT_A with roof function rAr_A. Modding out null sets, the family of measurable sets carries the complete separable metric d(A,B)=m(A△B)d(A,B)=m(A\triangle B) (symmetric difference), so questions about the family of induced maps TAT_A become Baire-category questions on this Polish space, the measure algebra.

The spectral side: to any measure-preserving TT one associates the Koopman unitary operator UT:f↦f∘TU_T:f\mapsto f\circ T on L2(X,m)L^2(X,m). The transformation TT has pure point (discrete) spectrum if L2L^2 admits an orthonormal basis of UTU_T-eigenfunctions; by the classical characterization, an ergodic transformation has pure point spectrum exactly when it is measurably isomorphic to an ergodic rotation on a compact abelian group, so for ergodic systems pure point spectrum and being a rotation are synonymous. At the opposite pole, TT is weakly mixing when it has no nonconstant eigenfunctions. Entropy scales under inducing by the standard law h(TA)=h(T)/m(A)h(T_A)=h(T)/m(A), so every induced map of an irrational rotation has zero entropy.

What is known about induced maps of a fixed ergodic TT: weakly mixing induced maps are dense (a classical density result recounted by Knill), and moreover the set {A:TA weakly mixing}\{A : T_A \text{ weakly mixing}\} is residual, that is, comeager — a statement that del Junco and Rudolph attribute to Conze (1972) and that Knill also credits to a 1973 remark of Petersen. Because a weakly mixing map has no nontrivial point spectrum, the class P={A:TA has pure point spectrum}\mathcal{P}=\{A : T_A \text{ has pure point spectrum}\} is meager; it is nonempty, since A=XA=X gives TA=TT_A=T, and inducing a rotation on suitable intervals produces exchanges of two intervals, which are themselves rotations. del Junco and Rudolph (1996) sharpened the residual picture: for TT of zero entropy that is loosely Bernoulli — the zero-entropy analogue of the Bernoulli property, defined by an orbit-name matching condition that irrational rotations satisfy — a residual set of AA yields TAT_A rank-one (generable from a single cutting-and-stacking tower) and rigid (some powers of its Koopman operator converge strongly to the identity); for positive-entropy TT the generic induced map is Bernoulli or K. Hansel (1973) showed a complementary abundance: for any aperiodic TT, any prescribed λ\lambda on the unit circle, and any ε>0\varepsilon>0, there is a set AA with m(A)≥1−εm(A)\ge 1-\varepsilon such that λ\lambda is an eigenvalue of TAT_A — but no way is known to upgrade individual eigenvalues to a complete eigenbasis.

The question below asks whether the meager class P\mathcal{P} is nonetheless dense. The stakes are set by Simon's Wonderland theorem (1995): in a Polish family of unitary operators in which pure point spectrum is dense and no member has absolutely continuous spectrum, the generic member has purely singular continuous spectrum. Knill observes that a positive answer for a rotation TT would transfer this conclusion to the family of induced Koopman operators, forcing purely singular continuous spectrum for the generic induced system — an expected but unproved behavior.

Problem Statement

Let T(x)=x+α mod 1T(x)=x+\alpha \bmod 1 be an irrational rotation of the circle T\mathbb{T} (so α\alpha is irrational), acting on the Lebesgue probability space (T,A,m)(\mathbb{T},\mathcal{A},m), and for a measurable set AA with m(A)>0m(A)>0 let TAT_A denote the induced (first-return) map on (A,m/m(A))(A,m/m(A)), defined by TA(x)=TrA(x)(x)T_A(x)=T^{r_A(x)}(x) with return time rA(x)=min⁡{k≥1:Tkx∈A}r_A(x)=\min\{k\ge 1 : T^k x\in A\}. Veech's question, as recorded by Petersen (1973, p. 229) and Conze (1972) and recalled by Knill (2023):

Is the class P={A∈A:m(A)>0 and TA has pure point spectrum}\mathcal{P}=\{A\in\mathcal{A} : m(A)>0 \text{ and } T_A \text{ has pure point spectrum}\} dense in the measure algebra (A,d)(\mathcal{A},d) — measurable sets modulo null sets — with d(A,B)=m(A△B)d(A,B)=m(A\triangle B)?

Equivalently: for every measurable set BB (of arbitrary measure, including measure zero) and every ε>0\varepsilon>0, must there exist a measurable set AA with m(A)>0m(A)>0 and m(A△B)<εm(A\triangle B)<\varepsilon such that the Koopman operator of TAT_A (the unitary operator f↦f∘TAf\mapsto f\circ T_A on L2(A,m/m(A))L^2(A,m/m(A))) admits a complete orthonormal basis of eigenfunctions — equivalently, since TAT_A is ergodic whenever TT is, such that TAT_A is measurably isomorphic to an ergodic rotation on a compact abelian group? Knill records the same question for an arbitrary ergodic transformation with pure point spectrum, and notes that a positive answer, combined with Simon's Wonderland theorem, would force the generic induced system TAT_A to have purely singular continuous spectrum. The problem is to prove or refute the density claim for each irrational rotation; as Knill notes, the same question can also be asked in the extended setting of an arbitrary ergodic transformation with pure point spectrum.

References

  1. Oliver Knill, "On the cohomology of measurable sets", arXiv:2307.12476 (2023), DOI: 10.48550/arXiv.2307.12476, https://arxiv.org/abs/2307.12476
  2. Karl Petersen, "Spectra of induced transformations", in Recent Advances in Topological Dynamics (Proc. Conf. Topological Dynamics, Yale Univ. 1972), Lecture Notes in Mathematics 318, pp. 226-230, Springer, 1973, DOI: 10.1007/bfb0061740, https://doi.org/10.1007/bfb0061740
  3. Jean-Pierre Conze, "Équations fonctionnelles et systèmes induits en théorie ergodique", Zeitschrift für Wahrscheinlichkeitstheorie und verwandte Gebiete 23 (1972), 75-82, DOI: 10.1007/BF00536692, https://doi.org/10.1007/BF00536692
  4. G. Hansel, "Automorphismes induits et valeurs propres", Zeitschrift für Wahrscheinlichkeitstheorie und verwandte Gebiete 25 (1973), 155-157, DOI: 10.1007/BF00533101, https://doi.org/10.1007/BF00533101
  5. Andres del Junco and Daniel J. Rudolph, "Residual behavior of induced maps", Israel Journal of Mathematics 93 (1996), 387-398, DOI: 10.1007/BF02761114, https://doi.org/10.1007/BF02761114
  6. Barry Simon, "Operators with singular continuous spectrum: I. General operators", Annals of Mathematics (2) 141, No. 1 (1995), 131-145, DOI: 10.2307/2118629, https://doi.org/10.2307/2118629
  7. Alessandro Carderi, Matthieu Joseph, François Le Maître, and Romain Tessera, "Belinskaya's theorem is optimal", Fundamenta Mathematicae 263, No. 1 (2023), 51-90, DOI: 10.4064/fm266-4-2023, arXiv:2201.06662, https://arxiv.org/abs/2201.06662
  8. Daniel J. Rudolph and Bethany D. Springer, "Nearly Continuous Even Kakutani Equivalence of Strongly Rank One Transformations", arXiv:1211.2297 (2012), https://arxiv.org/abs/1211.2297