Analytic quasiperiodic Schr odinger operators at small coupling - - PowerPoint PPT Presentation

analytic quasiperiodic schr odinger operators at small
SMART_READER_LITE
LIVE PREVIEW

Analytic quasiperiodic Schr odinger operators at small coupling - - PowerPoint PPT Presentation

Analytic quasiperiodic Schr odinger operators at small coupling Milivoje Lukic (Rice University) joint work with Ilia Binder, David Damanik, Michael Goldstein Western States Mathematical Physics Meeting February 12, 2017 Small


slide-1
SLIDE 1

Analytic quasiperiodic Schr¨

  • dinger operators

at small coupling

Milivoje Lukic (Rice University)

joint work with

Ilia Binder, David Damanik, Michael Goldstein Western States Mathematical Physics Meeting February 12, 2017

slide-2
SLIDE 2

Small quasi-periodic operators Isospectral torus KdV equation Comb domains

Setup

Quasi-periodic Schr¨

  • dinger operator HV = − d2

dx2 + V : potential given by

V (x) = U(ωx) with sampling function U : Tν → R and frequency ω ∈ Rν. Analytic sampling function, with small coupling: U(θ) =

  • m∈Zν

c(m)e2πimθ |c(m)| ≤ εe−κ0|m| for some ε > 0, 0 < κ0 ≤ 1. Diophantine frequency ω = (ω1, . . . , ων) ∈ Rν, |mω| ≥ a0|m|−b0, m ∈ Zν \ {0} for some 0 < a0 < 1, ν < b0 < ∞. All our results will hold for ε < ε0(a0, b0, κ0)

slide-3
SLIDE 3

Small quasi-periodic operators Isospectral torus KdV equation Comb domains

Direct spectral theory

Direct spectral properties (Elliason, Damanik–Goldstein): HV has purely a.c. spectrum, Floquet solutions for a.e. E ∈ σ(HV ) Spectrum σ(HV ) = [E, ∞) \

  • m∈Zν\{0}

(E −

m , E + m )

exponential in m decay of gap sizes E +

m − E − m ,

E +

m − E − m ≤ 2εe− κ0

2 |m|

polynomial in m, m′ decay of distances between gaps, dist([E −

m , E + m ], [E − m′, E + m′]) ≥ a|m|−b

if m = m′, |m′| ≥ |m| If E +

m − E − m ≤ ε′e−κ|m| for some κ ≥ 4κ0, then |c(m)| ≤ (2ε′)1/2e− κ

2 |m|

What about inverse spectral theory?

slide-4
SLIDE 4

Small quasi-periodic operators Isospectral torus KdV equation Comb domains

Reflectionless operators

Green’s function is formally given by G(x, y; z) = δx, (HV − z)−1δy V is reflectionless if Re G(0, 0; E + i0) = 0 for Lebesgue-a.e. E ∈ S = σ(HV ) Periodic and “finite-gap” quasiperiodic operators are reflectionless If V is periodic, the set of periodic potentials Q with spectrum σ(HQ) = σ(HV ) is topologically a torus, parametrized by Dirichlet data Kotani: almost periodic operators with pure a.c. spectrum are reflectionless Craig, 1989: definition of Dirichlet data for reflectionless operators and their evolution in x for spectra obeying some conditions Sodin–Yuditskii, 1995: reflectionless operators on homogeneous spectra are almost periodic

slide-5
SLIDE 5

Small quasi-periodic operators Isospectral torus KdV equation Comb domains

Isospectral torus of small quasi-periodic Schr¨

  • dinger operators

V (x) =

  • m∈Zν

c(m)e2πimωx, |c(m)| ≤ εe−κ0|m| Theorem (Damanik–Goldstein–Lukic) Let 0 < ε ≤ ε1(a0, b0, κ0). Assume Q ∈ L∞(R) is reflectionless and σ(HQ) = σ(HV ). Then Q(x) =

  • m∈Zν

d(m)e2πimωx, with |d(m)| ≤ √ 4ε exp

  • − κ0

4 |m|

  • ,

m ∈ Zν. Quasi-periodicity, the frequency ω, analyticity of the sampling function, are all encoded in the spectrum of HV

slide-6
SLIDE 6

Small quasi-periodic operators Isospectral torus KdV equation Comb domains

Proof through periodic approximations

V (x) =

  • m∈Zν

c(m)e2πimωx, |c(m)| ≤ εe−κ0|m| Use periodic approximants ˜ V (x) =

  • m∈Zν

c(m)e2πim ˜

ωx

for ˜ ω ∈ Qν To compare isospectral tori and evolutions of Dirichlet data, we need uniform estimates on distances between gaps and bands (theory of periodic potentials is insufficient: estimates would grow exponentially with period) Consider the quotient group Z(˜ ω) := Zν/{m ∈ Zν : m˜ ω = 0} and adapt the Damanik–Goldstein multiscale analysis to a method on Z(˜ ω) Construct periodic approximations ˜ Q of Q such that σ(H ˜

Q) = σ(H ˜ V )

slide-7
SLIDE 7

Small quasi-periodic operators Isospectral torus KdV equation Comb domains

KdV equation with almost periodic initial data

Consider the initial value problem for the KdV equation: ∂tu − 6u∂xu + ∂3

xu = 0

u(x, 0) = V (x) By Lax pair representation, solutions give isospectral families Hu(·,t) McKean–Trubowitz, 1976: If V ∈ Hn(T), then there is a global solution u(x, t) on T × R and this solution is Hn(T)-almost periodic in t (i.e., u(·, t) = F(ζt) for some continuous F : T∞ → Hn(T) and ζ ∈ R∞) Conjecture (Deift): If V : R → R is almost periodic, then there is a global solution u(x, t) that is almost periodic in t.

slide-8
SLIDE 8

Small quasi-periodic operators Isospectral torus KdV equation Comb domains

Global existence, uniqueness, and almost periodicity

V (x) =

  • m∈Zν

c(m)e2πimωx, |c(m)| ≤ εe−κ0|m| Theorem (Binder–Damanik–Goldstein–Lukic) If ε < ε0(a0, b0, κ0), then

1

(existence) there exists a global solution u(x, t);

2

(uniqueness) if ˜ u is another solution on R × [−T, T], and ˜ u, ∂3

x ˜

u ∈ L∞(R × [−T, T]), then ˜ u = u;

3

(x-dependence) for each t, u(·, t) is quasi-periodic in x, u(x, t) =

  • m∈Zν

c(m, t)e2πimωx |c(m, t)| ≤ √ 4ε e− κ0

4 |m| 4

(t-dependence) t → u(·, t) is W k,∞(R)-almost periodic in t, for any integer k ≥ 0.

slide-9
SLIDE 9

Small quasi-periodic operators Isospectral torus KdV equation Comb domains

Global existence, uniqueness, and almost periodicity

The previous result is a corollary of a more general conditional statement: Theorem (Binder–Damanik–Goldstein–Lukic) If V : R → R is almost periodic, σac(HV ) = σ(HV ) = S, and S obeys some Craig-type and homogeneity conditions, then

1

(existence) there exists a global solution u(x, t);

2

(uniqueness) if ˜ u is another solution on R × [−T, T], and ˜ u, ∂3

x ˜

u ∈ L∞(R × [−T, T]), then ˜ u = u;

3

(x-dependence) for each t, x → u(x, t) is almost periodic in x;

4

(t-dependence) t → u(·, t) is W 4,∞(R)-almost periodic in t.

slide-10
SLIDE 10

Small quasi-periodic operators Isospectral torus KdV equation Comb domains

Trajectory on isospectral torus

Rybkin, 2008: Assume that V is reflectionless and σac(HV ) = σ(HV ) = S. Assume that u(x, t) is a solution such that u, ∂3

xu ∈ L∞(R × [−T, T])

for some T > 0. Then, u(·, t) is reflectionless for all t Prove that the t-evolution of Dirichlet data is given by a Lipshitz vector field, conclude uniqueness Use finite-gap approximants to prove existence Use the Sodin–Yuditskii map to prove almost periodicity in t

slide-11
SLIDE 11

Small quasi-periodic operators Isospectral torus KdV equation Comb domains

Comb domains

V (x) =

  • m∈Zν

c(m)e2πimωx, |c(m)| ≤ εe−κ0|m| Almost-periodicity of V implies almost-periodicity of m-functions, so following Johnson–Moser, consider w(z) = lim

L→∞

1 L L m+(x; z)dx Theorem (Binder–Damanik–Goldstein–Lukic) If ε < ε0(a0, b0, κ0), then w(z) is a conformal map from C \ [E, ∞) to a comb domain of the form C+ \

  • m∈Zν

{mω + iy | 0 < y < hm} where hm < ε1/2e− κ0

5 |m|

slide-12
SLIDE 12

Small quasi-periodic operators Isospectral torus KdV equation Comb domains

Prescribing the heights hm

Theorem (Binder–Damanik–Goldstein–Lukic) If hm < ε′e−κ|m| with ε′ < ε0(a0, b0, κ0) and κ ≥ 5κ0, then there exists V (x) =

  • m∈Zν

c(m)e2πimωx, |c(m)| ≤ (ε′)1/4e− κ

3 |m|

which corresponds to the comb domain C+ \

  • m∈Zν

{mω + iy | 0 < y < hm} Corollary Within the class of analytic quasi-periodic Schr¨

  • dinger operators at small

coupling, we can prescribe an arbitrary set M ⊂ Zν and there exists V such that E +

m − E − m > 0 ⇐

⇒ m ∈ M In particular, we have, within this class, approximation by finite gap potentials just like in the periodic case.

slide-13
SLIDE 13

Thank you!