Pär Kurlberg
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
Research Subjects
Pär Kurlberg has a total of 65 co-authors. Here are the top co-authors by number of shared publications:
- Igor Wigman
Department of Mathematics, King’s College London, London, UK
8 shared publications - Igor E. Shparlinski
School of Mathematics and Statistics, University of New South Wales, Sydney, Australia
7 shared publications - Thomas J. Tucker
University of Rochester
7 shared publications - Carl Pomerance
Dartmouth College
6 shared publications - Lior Rosenzweig
Afeka Tel Aviv Coll Engn, Unit Math, Mivtza Kadesh 38, Tel Aviv, Israel
6 shared publications - Robert L. Benedetto
Amherst College
6 shared publications
Latest Publications
- Open Access
Superscars in the Šeba billiard
We consider the Laplacian with a delta potential (also known as a "point scatterer", or "Fermi pseudopotential") on an irrational torus, where the square of the side ratio is diophantine. The eigenfunctions fall into two classes -"old" eigenfunctions (75%) of the Laplacian which vanish at the support of the delta potential, and therefore are not affected, and "new" eigenfunctions (25%) which are affected, and as a result feature a logarithmic singularity at the location of the delta potential.Within a full density subsequence of the new eigenfunctions we determine all semiclassical measures in the weak coupling regime and show that they are localized along 4 wave vectors in momentum space -we therefore prove the existence of so-called "superscars" as predicted by Bogomolny and Schmit [6]. This result contrasts the phase space equidistribution which is observed for a full density subset of the new eigenfunctions of a point scatterer on a rational torus [15]. Further, in the strong coupling limit we show that a weaker form of localization holds for an essentially full density subsequence of the new eigenvalues; in particular quantum ergodicity does not hold. We also explain how our results can be modified for rectangles with Dirichlet boundary conditions with a point scatterer in the interior. In this case our results extend previous work of Keating, Marklof and Winn who proved the existence of localized semiclassical measures under a clustering condition on the spectrum of the Laplacian.
Open AccessSuperscars in the Šeba billiard
We consider the Laplacian with a delta potential (also known as a "point scatterer", or "Fermi pseudopotential") on an irrational torus, where the square of the side ratio is diophantine. The eigenfunctions fall into two classes -"old" eigenfunctions (75%) of the Laplacian which vanish at the support of the delta potential, and therefore are not affected, and "new" eigenfunctions (25%) which are affected, and as a result feature a logarithmic singularity at the location of the delta potential.Within a full density subsequence of the new eigenfunctions we determine all semiclassical measures in the weak coupling regime and show that they are localized along 4 wave vectors in momentum space -we therefore prove the existence of so-called "superscars" as predicted by Bogomolny and Schmit [6]. This result contrasts the phase space equidistribution which is observed for a full density subset of the new eigenfunctions of a point scatterer on a rational torus [15]. Further, in the strong coupling limit we show that a weaker form of localization holds for an essentially full density subsequence of the new eigenvalues; in particular quantum ergodicity does not hold. We also explain how our results can be modified for rectangles with Dirichlet boundary conditions with a point scatterer in the interior. In this case our results extend previous work of Keating, Marklof and Winn who proved the existence of localized semiclassical measures under a clustering condition on the spectrum of the Laplacian.
- Open Access
- 2 July 2025
- Published by Springer Nature in Communications in Mathematical Physics
- Vol. 406 (8) , 1-29
On Quantum Ergodicity for Higher Dimensional Cat Maps
We study eigenfunction localization for higher dimensional cat maps, a popular model of quantum chaos. These maps are given by linear symplectic maps in $$\operatorname {Sp}(2g,{{\mathbb {Z}}})$$ , which we take to be ergodic. Under some natural assumptions, we show that there is a density one sequence of integers N so that as N tends to infinity along this sequence, all eigenfunctions of the quantized map at the inverse Planck constant N are uniformly distributed. For the two-dimensional case ( $$g=1$$ ), this was proved by Kurlberg and Rudnick (Duke Math J 103:47–78, 2000). The higher dimensional case offers several new features and requires a completely different set of tools, including from additive combinatorics, such as a bound of Bourgain (J Am Math Soc 18:477–499, 2005) for Mordell sums, and a study of tensor product structures for the cat map, which has never been exploited in this context.- 2 July 2025
- Published by Springer Nature in Communications in Mathematical Physics
- Vol. 406 (8) , 1-29
Open AccessOn Quantum Ergodicity for Higher Dimensional Cat Maps
We study eigenfunction localization for higher dimensional cat maps, a popular model of quantum chaos. These maps are given by linear symplectic maps in $$\operatorname {Sp}(2g,{{\mathbb {Z}}})$$ , which we take to be ergodic. Under some natural assumptions, we show that there is a density one sequence of integers N so that as N tends to infinity along this sequence, all eigenfunctions of the quantized map at the inverse Planck constant N are uniformly distributed. For the two-dimensional case ( $$g=1$$ ), this was proved by Kurlberg and Rudnick (Duke Math J 103:47–78, 2000). The higher dimensional case offers several new features and requires a completely different set of tools, including from additive combinatorics, such as a bound of Bourgain (J Am Math Soc 18:477–499, 2005) for Mordell sums, and a study of tensor product structures for the cat map, which has never been exploited in this context. - Open Access
- 13 February 2025
- Published by Springer Nature in Inventiones Mathematicae
- Vol. 240 (2) , 537-585
Poisson spacing statistics for lattice points on circles
We show that along a density one subsequence of admissible radii, the nearest neighbor spacing between lattice points on circles is Poissonian.
- 13 February 2025
- Published by Springer Nature in Inventiones Mathematicae
- Vol. 240 (2) , 537-585
Open AccessPoisson spacing statistics for lattice points on circles
We show that along a density one subsequence of admissible radii, the nearest neighbor spacing between lattice points on circles is Poissonian.
- 1 June 2024
- Published by Project MUSE in American Journal of Mathematics
- Vol. 146 (3) , 607-629
Prime and Möbius correlations for very short intervals in $\fq[x]$We investigate function field analogs of the distribution of primes, and prime $k$-tuples, in ``very short intervals'' of the form $I(f):=\{f(x) + a : a \in\fp\}$ for $f(x)\in\fp[x]$ and $p$ prime, as well as cancellation in sums of function field analogs of the M\"{o}bius $\mu$ function and its correlations (similar to sums appearing in Chowla's conjecture). For generic $f$, i.e., for $f$ a Morse polynomial, the error terms are roughly of size $O(\sqrt{p})$ (with typical main terms of order $p$). For non-generic $f$ we prove that independence still holds for ``generic'' set of shifts. We can also exhibit examples for which there is no cancellation at all in M\"{o}bius/Chowla type sums (in fact, it turns out that (square root) cancellation in M\"{o}bius sums is {\em equivalent} to (square root) cancellation in Chowla type sums), as well as intervals where the heuristic ``primes are independent'' fails badly. The results are deduced from a general theorem on correlations of arithmetic class functions; these include characteristic functions on primes, the M\"{o}bius $\mu$ function, and divisor functions (e.g., function field analogs of the Titchmarsh divisor problem can be treated). We also prove analogous, but slightly weaker, results in the more delicate fixed characteristic setting, i.e., for $f(x)\in\fq[x]$ and intervals of the form $f(x)+a$ for $a\in\fq$, where $p$ is fixed and $q=p^{l}$ grows.- 1 June 2024
- Published by Project MUSE in American Journal of Mathematics
- Vol. 146 (3) , 607-629
Prime and Möbius correlations for very short intervals in $\fq[x]$We investigate function field analogs of the distribution of primes, and prime $k$-tuples, in ``very short intervals'' of the form $I(f):=\{f(x) + a : a \in\fp\}$ for $f(x)\in\fp[x]$ and $p$ prime, as well as cancellation in sums of function field analogs of the M\"{o}bius $\mu$ function and its correlations (similar to sums appearing in Chowla's conjecture). For generic $f$, i.e., for $f$ a Morse polynomial, the error terms are roughly of size $O(\sqrt{p})$ (with typical main terms of order $p$). For non-generic $f$ we prove that independence still holds for ``generic'' set of shifts. We can also exhibit examples for which there is no cancellation at all in M\"{o}bius/Chowla type sums (in fact, it turns out that (square root) cancellation in M\"{o}bius sums is {\em equivalent} to (square root) cancellation in Chowla type sums), as well as intervals where the heuristic ``primes are independent'' fails badly. The results are deduced from a general theorem on correlations of arithmetic class functions; these include characteristic functions on primes, the M\"{o}bius $\mu$ function, and divisor functions (e.g., function field analogs of the Titchmarsh divisor problem can be treated). We also prove analogous, but slightly weaker, results in the more delicate fixed characteristic setting, i.e., for $f(x)\in\fq[x]$ and intervals of the form $f(x)+a$ for $a\in\fq$, where $p$ is fixed and $q=p^{l}$ grows.- Open Access
- 4 May 2023
- Published by Cambridge University Press (CUP) in Forum of Mathematics, Sigma
- Vol. 11
Superscars for arithmetic point scatters II
We consider momentum push-forwards of measures arising as quantum limits (semiclassical measures) of eigenfunctions of a point scatterer on the standard flat torus ${\mathbb T}^2 = {\mathbb R}^2/{\mathbb Z}^{2}$ . Given any probability measure arising by placing delta masses, with equal weights, on ${\mathbb Z}^2$ -lattice points on circles and projecting to the unit circle, we show that the mass of certain subsequences of eigenfunctions, in momentum space, completely localizes on that measure and are completely delocalized in position (i.e., concentration on Lagrangian states). We also show that the mass, in momentum, can fully localize on more exotic measures, for example, singular continuous ones with support on Cantor sets. Further, we can give examples of quantum limits that are certain convex combinations of such measures, in particular showing that the set of quantum limits is richer than the ones arising only from weak limits of lattice points on circles. The proofs exploit features of the half-dimensional sieve and behavior of multiplicative functions in short intervals, enabling precise control of the location of perturbed eigenvalues.- 4 May 2023
- Published by Cambridge University Press (CUP) in Forum of Mathematics, Sigma
- Vol. 11
Open AccessSuperscars for arithmetic point scatters II
We consider momentum push-forwards of measures arising as quantum limits (semiclassical measures) of eigenfunctions of a point scatterer on the standard flat torus ${\mathbb T}^2 = {\mathbb R}^2/{\mathbb Z}^{2}$ . Given any probability measure arising by placing delta masses, with equal weights, on ${\mathbb Z}^2$ -lattice points on circles and projecting to the unit circle, we show that the mass of certain subsequences of eigenfunctions, in momentum space, completely localizes on that measure and are completely delocalized in position (i.e., concentration on Lagrangian states). We also show that the mass, in momentum, can fully localize on more exotic measures, for example, singular continuous ones with support on Cantor sets. Further, we can give examples of quantum limits that are certain convex combinations of such measures, in particular showing that the set of quantum limits is richer than the ones arising only from weak limits of lattice points on circles. The proofs exploit features of the half-dimensional sieve and behavior of multiplicative functions in short intervals, enabling precise control of the location of perturbed eigenvalues. - Open Access
- 20 June 2022
- Published by Springer Nature in Annales Henri Poincare
- Vol. 23 (12) , 4449-4462
Level Repulsion for Arithmetic Toral Point Scatterers in Dimension 3
We show that arithmetic toral point scatterers in dimension three (“Šeba billiards on $${\mathbb R}^3/{\mathbb Z}^3$$ ”) exhibit strong level repulsion between the set of “new” eigenvalues. More precisely, let $$\Lambda := \{ \lambda _{1}< \lambda _{2} < \ldots \}$$ denote the unfolded set of new eigenvalues. Then, given any $$\gamma >0$$ , $$\begin{aligned} \frac{|\{ i \le N : \lambda _{i+1}-\lambda _{i} \le \epsilon \}|}{N} = O_{\gamma }(\epsilon ^{4-\gamma }) \end{aligned}$$ as $$N \rightarrow \infty $$ (and $$\epsilon >0$$ small.) To the best of our knowledge, this is the first mathematically rigorous demonstration of a level repulsion phenomena for the quantization of a deterministic system.- 20 June 2022
- Published by Springer Nature in Annales Henri Poincare
- Vol. 23 (12) , 4449-4462
Open AccessLevel Repulsion for Arithmetic Toral Point Scatterers in Dimension 3
We show that arithmetic toral point scatterers in dimension three (“Šeba billiards on $${\mathbb R}^3/{\mathbb Z}^3$$ ”) exhibit strong level repulsion between the set of “new” eigenvalues. More precisely, let $$\Lambda := \{ \lambda _{1}< \lambda _{2} < \ldots \}$$ denote the unfolded set of new eigenvalues. Then, given any $$\gamma >0$$ , $$\begin{aligned} \frac{|\{ i \le N : \lambda _{i+1}-\lambda _{i} \le \epsilon \}|}{N} = O_{\gamma }(\epsilon ^{4-\gamma }) \end{aligned}$$ as $$N \rightarrow \infty $$ (and $$\epsilon >0$$ small.) To the best of our knowledge, this is the first mathematically rigorous demonstration of a level repulsion phenomena for the quantization of a deterministic system. - Open Access
- 10 August 2021
- Published by IOP Publishing in Nonlinearity
- Vol. 34 (9) , 6651-6684
The defect of toral Laplace eigenfunctions and arithmetic random waves
We study the defect (or ‘signed area’) distribution of standard toral Laplace eigenfunctions restricted to shrinking balls of radius above the Planck scale, either for deterministic eigenfunctions averaged w.r.t. the spatial variable, or in a random Gaussian scenario (‘arithmetic random waves’). In either case we exploit the associated symmetry of the eigenfunctions to show that the expectation (spatial or Gaussian) vanishes. In the deterministic setting, we prove that the variance of the defect of flat eigenfunctions, restricted to balls shrinking above the Planck scale, vanishes for ‘most’ energies. Hence the defect of eigenfunctions restricted to most of the said balls is small. We also construct ‘esoteric’ eigenfunctions with large defect variance, by choosing our eigenfunctions so that to mimic the situation on the hexagonal torus, thus breaking the symmetries associated to the standard torus. In the random Gaussian setting, we establish various upper and lower bounds for the defect variance w.r.t. the Gaussian probability measure. A crucial ingredient in the proof of the lower bound is the use of Schmidt’s subspace theorem.
- 10 August 2021
- Published by IOP Publishing in Nonlinearity
- Vol. 34 (9) , 6651-6684
Open AccessThe defect of toral Laplace eigenfunctions and arithmetic random waves
We study the defect (or ‘signed area’) distribution of standard toral Laplace eigenfunctions restricted to shrinking balls of radius above the Planck scale, either for deterministic eigenfunctions averaged w.r.t. the spatial variable, or in a random Gaussian scenario (‘arithmetic random waves’). In either case we exploit the associated symmetry of the eigenfunctions to show that the expectation (spatial or Gaussian) vanishes. In the deterministic setting, we prove that the variance of the defect of flat eigenfunctions, restricted to balls shrinking above the Planck scale, vanishes for ‘most’ energies. Hence the defect of eigenfunctions restricted to most of the said balls is small. We also construct ‘esoteric’ eigenfunctions with large defect variance, by choosing our eigenfunctions so that to mimic the situation on the hexagonal torus, thus breaking the symmetries associated to the standard torus. In the random Gaussian setting, we establish various upper and lower bounds for the defect variance w.r.t. the Gaussian probability measure. A crucial ingredient in the proof of the lower bound is the use of Schmidt’s subspace theorem.
- 1 August 2021
- Published by Elsevier in Finite Fields and Their Applications
- Vol. 73
The Chebotarev density theorem for function fields — Incomplete intervals
- 1 August 2021
- Published by Elsevier in Finite Fields and Their Applications
- Vol. 73
The Chebotarev density theorem for function fields — Incomplete intervals
- Open Access
Superscars for Arithmetic Point Scatterers II
We consider momentum push-forwards of measures arising as quantum limits (semi-classical measures) of eigenfunctions of a point scatterer on the standard flat torus $\mathbb T^2 = \mathbb R^2/\mathbb Z^{2}$. Given any probability measure arising by placing delta masses, with equal weights, on $\mathbb Z^2$-lattice points on circles and projecting to the unit circle, we show that the mass of certain subsequences of eigenfunctions, in momentum space, completely localizes on that measure and is completely delocalized in position (i.e., concentration on Lagrangian states.) We also show that the mass, in momentum, can fully localize on more exotic measures, e.g. singular continous ones with support on Cantor sets. Further, we can give examples of quantum limits that are certain convex combinations of such measures, in particular showing that the set of quantum limits is richer than the ones arising only from weak limits of lattice points on circles. The proofs exploit features of the half-dimensional sieve and behavior of multiplicative functions in short intervals.Open AccessSuperscars for Arithmetic Point Scatterers II
We consider momentum push-forwards of measures arising as quantum limits (semi-classical measures) of eigenfunctions of a point scatterer on the standard flat torus $\mathbb T^2 = \mathbb R^2/\mathbb Z^{2}$. Given any probability measure arising by placing delta masses, with equal weights, on $\mathbb Z^2$-lattice points on circles and projecting to the unit circle, we show that the mass of certain subsequences of eigenfunctions, in momentum space, completely localizes on that measure and is completely delocalized in position (i.e., concentration on Lagrangian states.) We also show that the mass, in momentum, can fully localize on more exotic measures, e.g. singular continous ones with support on Cantor sets. Further, we can give examples of quantum limits that are certain convex combinations of such measures, in particular showing that the set of quantum limits is richer than the ones arising only from weak limits of lattice points on circles. The proofs exploit features of the half-dimensional sieve and behavior of multiplicative functions in short intervals. - Open Access
The Chebotarev density theorem for function fields -- incomplete intervals
We prove a Polya-Vinogradov type variation of the the Chebotarev density theorem for function fields over finite fields valid for "incomplete intervals" $I \subset \mathbb{F}_p$, provided $(p^{1/2}\log p)/|I| = o(1)$. Applications include density results for irreducible trinomials in $\mathbb{F}_p[x]$, i.e. the number of irreducible polynomials in the set $\{ f(x) = x^{d} + a_{1} x + a_{0} \in \mathbb{F}_p[x] \}_{a_{0} \in I_{0}, a_{1}\in I_{1}}$ is $\sim |I_{0}|\cdot |I_{1}|/d$ provided $|I_{0}| > p^{1/2+\epsilon}$, $|I_{1}| > p^{\epsilon}$, or $|I_{1}| > p^{1/2+\epsilon}$, $|I_{0}| > p^{\epsilon}$, and similarly when $x^{d}$ is replaced by any monic degree $d$ polynomial in $\mathbb{F}_p[x]$. Under the above assumptions we can also determine the distribution of factorization types, and find it to be consistent with the distribution of cycle types of permutations in the symmetric group $S_{d}$.Open AccessThe Chebotarev density theorem for function fields -- incomplete intervals
We prove a Polya-Vinogradov type variation of the the Chebotarev density theorem for function fields over finite fields valid for "incomplete intervals" $I \subset \mathbb{F}_p$, provided $(p^{1/2}\log p)/|I| = o(1)$. Applications include density results for irreducible trinomials in $\mathbb{F}_p[x]$, i.e. the number of irreducible polynomials in the set $\{ f(x) = x^{d} + a_{1} x + a_{0} \in \mathbb{F}_p[x] \}_{a_{0} \in I_{0}, a_{1}\in I_{1}}$ is $\sim |I_{0}|\cdot |I_{1}|/d$ provided $|I_{0}| > p^{1/2+\epsilon}$, $|I_{1}| > p^{\epsilon}$, or $|I_{1}| > p^{1/2+\epsilon}$, $|I_{0}| > p^{\epsilon}$, and similarly when $x^{d}$ is replaced by any monic degree $d$ polynomial in $\mathbb{F}_p[x]$. Under the above assumptions we can also determine the distribution of factorization types, and find it to be consistent with the distribution of cycle types of permutations in the symmetric group $S_{d}$.