 Semiclassical measures on hyperbolic surfaces have full support,
with Long Jin
Using the fractal uncertainty principle proved in a previous paper with Bourgain,
we show that every semiclassical defect measure on a compact hyperbolic surface
has support equal to the entire cosphere bundle.
 Fourier dimension and spectral gaps for hyperbolic surfaces,
with Jean Bourgain, Geometric and Functional Analysis 27(2017), 744–771
For a convex cocompact hyperbolic surface with limit set Λ of dimension δ>0, we show that the Fourier dimension of Λ is at least ε for some ε>0 depending only on δ. The proof uses the discretized sumproduct theorem in R and the nonlinear nature of the transformations in the group Γ; in fact,
our result would be false for linear Cantor sets. Using fractal uncertainty principle,
we deduce an essential spectral gap of size 1/2δ+ε.
 Dolgopyat's method and the fractal uncertainty principle,
with Long Jin
We show that every Ahlfors–David regular subset of R of positive dimension
satisfies the fractal uncertainty principle with exponent strictly larger than the one coming from the volume bound.
The method of proof is inspired by the works of Dolgopyat, Naud, and Stoyanov in the context
of spectral gaps for transfer operators, and can be crudely summarized as follows:
triangle inequality in a Hilbert space is rarely sharp. As an application we obtain
new spectral gaps for convex cocompact hyperbolic surfaces and open quantum baker's maps.
 Spectral gaps without the pressure condition,
with Jean Bourgain
We show that every convex cocompact hyperbolic surface has an essential spectral gap.
The proof uses the approach developed in the paper with Zahl
and the key new component is the fractal uncertainty principle for δregular sets with all δ<1. Previously such gaps were known only under the relaxed pressure
condition δ≤1/2.
 Resonances for open quantum maps and a fractal uncertainty principle,
with Long Jin,
Communications in Mathematical Physics 354(2017), 269–316
We study open quantum baker's maps, which are models in open quantum chaos having Cantor sets as their trapped sets.
Using the fractal uncertainty approach developed in the paper with Zahl
and the arithmetic structure of Cantor sets, we show that all such systems have a spectral gap,
and obtain quantitative bounds on the size of the gap. We also show
an improved Weyl bound similar to the one here.
Both results are supported by numerical evidence.
 Improved fractal Weyl bounds for hyperbolic manifolds,
with an appendix with David Borthwick and Tobias Weich,
to appear in Journal of the European Mathematical Society
We give a Weyl upper bound on the number of scattering resonances on convex cocompact hyperbolic quotients in strips. The exponent in the bound depends on the width of the strip and improves on the standard Weyl upper bound, in particular this exponent is negative until the Patterson–Sullivan gap. The appendix gives numerical evidence for the new Weyl bound.
 Spectral gaps, additive energy, and a fractal uncertainty principle,
with Joshua Zahl,
Geometric and Functional Analysis 26(2016), 1011–1094
We obtain an improved spectral gap for convex cocompact hyperbolic surfaces with the dimension of the limit set close to 1/2.
Compared to previous works on spectral gaps which rely on Dolgopyat's method, we decouple the combinatorial difficulties of
the problem from the analytical ones and obtain an explicit formula for the gap in terms of additive energy of the limit set,
which in turn is estimated using its Ahlfors–David regularity.
 Fractal Weyl laws and wave decay for general trapping,
with Jeffrey Galkowski,
to appear in Nonlinearity
We give an upper bound on the number of resonances in strips for general
manifolds with Euclidean infinite ends, without any assumptions on the trapped set.
Our bound depends on the volume of the set of trajectories which are trapped for
the Ehrenfest time, and gives a polynomial improvement over the standard bound
R^{d1} when the escape rate is positive. We also prove a wave decay result with
high probability for random initial data.
 Lower resolvent bounds and Lyapunov exponents,
with Alden Waters, Applied Mathematics Research Express 2016, 68–97
We obtain a polynomial lower bound on the norm of the scattering resolvent in the lower halfplane under very mild assumptions on trapping, namely existence of a trajectory which is trapped in the past, but not in the future.
The power in the bound, depending on the maximal expansion rate along the trajectory,
gives the smallest number of derivatives lost in an exponential decay of local energy estimate
for the wave equation.
 Resonances and lower resolvent bounds,
with Kiril Datchev and Maciej Zworski,
Journal of Spectral Theory 5(2015), 599–615
We show that in the presence of certain elliptic trapping, onesided bounds on the resolvent with a cutoff supported far away into the infinity are at best exponential. This
is in contrast with the known polynomial twosided bounds.

Resonance projectors and asymptotics
for rnormally hyperbolic trapped sets, Journal of the American Mathematical Society
28(2015), 311–381.
We show existence of a band of resonances with a Weyl law when the trapped
set is rnormally hyperbolic for large r and the normal expansion
rates are halfpinched. This dynamical setting is stable under perturbations and is applied
the next paper
to Kerr–de Sitter black holes. The key tool is a Fourier integral operator microlocally projecting
onto resonant states in the band. This operator lets us microlocally represent resonance expansions as
Taylor expansions; a variety of methods from microlocal analysis, especially positive commutator estimates, finish the proof.
The rnormal hyperbolicity assumption is explicitly needed in the construction of the projector to ensure smoothness
of its symbol.

Fractal Weyl laws for asymptotically hyperbolic manifolds,
with Kiril Datchev,
Geometric and Functional Analysis 23(2013), 1145–1206.
We obtain a fractal upper bound on the number of resonances in disks of fixed size centered at
the unitarity axis for a general class of manifolds, including convex cocompact hyperbolic quotients.
The exponent in the bound is related to the dimension of the trapped set.
We use the techniques of Sjöstrand–Zworski
on resonance counting for hyperbolic trapped sets and of
Vasy
on effective meromorphic continuation of the resolvent for asymptotically hyperbolic
infinite ends.

Symmetry of bound and antibound states in the semiclassical limit
for a general class of potentials, with
Subhroshekhar Ghosh,
Proceedings of the American Mathematical Society 138 (2010), 3203–3210.
It was proved by Bindel and Zworski in this paper
that for scattering on the halfline by a compactly supported
potential with a constant bump at the end of its support,
the purely imaginary poles of the resolvent
become symmetric with respect to the real axis modulo
errors exponentially small in the semiclassical limit.
Our paper is an extension
of this result to a more general class of potentials,
allowing any positive bump, and also provides a different
explanation of why this phenomenon holds.
 Ruelle zeta function at zero for surfaces,
with Maciej Zworski,
Inventiones Mathematicae
Using previous work with Zworski as well
as relatively standard microlocal techniques,
we show that the Ruelle zeta function for
a negatively curved oriented surface vanishes at zero to the order
given by the absolute value of the Euler characteristic.
This result, giving a relation between dynamics
and topology, was previously known only in constant curvature via the Selberg trace formula.
 Pollicott–Ruelle
resonances for open systems,
with Colin Guillarmou,
Annales Henri Poincaré 17(2016), 3089–3146
We define Pollicott–Ruelle resonances for hyperbolic flows on noncompact manifolds (in a setting
closely related to basic sets of Axiom A flows). They arise either as poles of Fourier–Laplace transforms
of correlations or as poles of meromorphic extensions of dynamical zeta functions. Our construction is based
on the microlocal approach of Faure–Sjöstrand
and Dyatlov–Zworski.
 Stochastic stability of Pollicott–Ruelle resonances,
with Maciej Zworski,
Nonlinearity 28(2015), 3511–3534
We show that Pollicott–Ruelle resonances of an Anosov flow are the limits of the L^{2} eigenvalues
of the generator of the flow with an additional damping term. The latter eigenvalues characterize decay of correlations
for a stochastic modification of the flow.
 Power spectrum of the geodesic flow on hyperbolic manifolds,
with Frédéric Faure and Colin Guillarmou,
Analysis & PDE 8(2015), 923–1000.
We describe the Pollicott–Ruelle resonances for compact hyperbolic quotients in all dimensions. In dimensions greater than 2,
this description is much more involved than for surfaces and features in particular the spectrum of the Laplacian on tracefree
divergencefree symmetric tensors of all orders.
 Dynamical zeta functions for Anosov flows via microlocal analysis,
with Maciej Zworski,
Annales de l'ENS 49(2016), 543–577
We prove meromorphic continuation of the Ruelle dynamical zeta function for Anosov flows, recovering
recent results of Giulietti, Liverani, and Pollicott.
We follow the approach of Faure–Sjöstrand; the key new component is the restriction on the wavefront
set of the resolvent, using the methods of Melrose and Vasy, making it possible to take the flat trace.

Sharp polynomial bounds on the number of Pollicott–Ruelle resonances,
with Kiril Datchev
and Maciej Zworski,
Ergodic Theory and Dynamical Systems 34(2014), 1168–1183.
Using the methods of the previous paper,
we obtain sharp upper bounds on the number of Ruelle resonances,
defined using the framework of Faure
and Sjöstrand.
 Spectral gaps for normally hyperbolic trapping,
Annales de l'Institut Fourier 66(2016), 55–82
Motivated by Kerr and Kerr–de Sitter black holes, we show existence of spectral gaps of optimal size for normally hyperbolic
trapped sets with codimension 1 smooth stable/unstable foliations. The short proofs, based on semiclassical defect measures,
simplify and refine some of the earlier results of Wunsch–Zworski,
Nonnenmacher–Zworski (in our special case), and
myself.

Trapping of waves and null geodesics for rotating black holes,
with Maciej Zworski,
Physical Review D
88(2013), 084037.
A note outlining some of the recent work on resonances for rotating black holes.

Asymptotics of linear waves and resonances
with applications to black holes, Communications in Mathematical Physics 335(2015), 1445–1485.
We apply the methods and results of a previous paper
to the setting of Kerr–de Sitter black holes, proving a Weyl law for resonances and an asymptotic
decomposition of linear waves for high frequencies. The latter fact, related to resonance expansion,
is also proved for Kerr black holes using the work of Vasy–Zworski.

Asymptotic distribution of quasinormal modes for
Kerr–de Sitter black holes,
Annales Henri Poincaré 13(2012), 1101–1166.
We establish a Bohr–Sommerfeld type quantization condition for quasinormal
modes of a slowly rotating Kerr–de Sitter black hole, observing in particular
a Zeemanlike splitting once spherical symmetry is broken. We compute the resulting
pseudopoles numerically [click here for MATLAB codes and data]
and compare them to those
numerically studied by physicists.
Finally, we prove a resonance decomposition of linear waves.

Exponential energy decay for Kerr–de Sitter
black holes beyond event horizons,
Mathematical Research Letters
18 (2011), 1023–1035.
The redshift effect and a parametrix near the event horizons are used
to extend the exponential decay proved in the previous paper
to the whole space.

Quasinormal modes and exponential energy decay for the
Kerr–de Sitter black hole,
Communications in Mathematical Physics
306 (2011), 119–163.
This paper constructs an analogue of the scattering resolvent in the case of
a slowly rotating Kerr–de Sitter black hole. The poles are proven to form
a discrete set; they are the
quasinormal modes
of black holes that have been
numerically studied by physicists.
Using the recent result by Wunsch and Zworski,
we prove existence of a resonance free strip and exponential energy decay for the wave
equation on a fixed compact set.

Scattering phase asymptotics with fractal remainders,
with Colin Guillarmou,
Communications in Mathematical Physics
324(2013), 425–444.
Using our previous work, we derive scattering
phase asymptotics for manifolds with asymptotically Euclidean ends with remainders that
are fractal for hyperbolic flows. We next derive asymptotics with a similar remainder
for hyperbolic quotients, and nonsharp lower bounds on the remainder in some cases.
Finally, we investigate the relation of scattering phase asymptotics with counting resonances
near the unitarity axis, in particular with the fractal Weyl law.

Microlocal limits of plane waves and Eisenstein functions,
with Colin Guillarmou,
Annales de l'ENS 47(2014), 371–448.
For Riemannian manifolds that are either Euclidean or hyperbolic near infinity, and
with trapped set of Liouville measure zero, we
show that plane waves, also known as Eisenstein functions, converge to some semiclassical
measure, if one averages in frequency in an hsized window and in
the direction of the wave. The speed of convergence is estimated in terms
of the classical escape rate and the Ehrenfest time; in many cases,
this is a power of h (in contrast with quantum ergodicity on compact manifolds,
where the best known result is 1/log h). As an application,
we derive a local Weyl law for spectral projectors with a fractal remainder.

Quantum ergodicity for restrictions to hypersurfaces,
with Maciej Zworski,
Nonlinearity 26(2013), 35–52.
We show that on a compact Riemannian manifold with ergodic geodesic flow,
restrictions of the eigenfunctions of the Laplacian to any hypersurface
satisfying a simple geometric condition are equidistributed in phase space.
This work generalizes a paper of
John Toth
and Steve Zelditch using
the methods of semiclassical analysis, and provides a shorter proof.

Microlocal limits of Eisenstein functions
away from the unitarity axis, Journal of Spectral Theory
2 (2012), 181–202.
We consider a Riemannian surface with cusp ends and show that the Eisenstein functions
in the upper halfplane, away from the real line, converge to a certain canonical
measure. This statement is similar to quantum unique ergodicity(QUE); however,
being away from the real line considerably simplifies the problem. In particular,
no global dynamical properties of the flow are used. As an application,
we prove that the scattering matrix converges to zero in any strip away from the real line.
[ First version, using a more direct analysis
in the cusp ]