Abstract:We prove the existence of infinitely many time-periodic solutions of nonlinear Schrödinger equations using pseudo-holomorphic curve methods from Hamiltonian Floer theory. For the generalization of the Gromov–Floer compactness theorem to infinite dimensions, we show how to solve the arising small divisor problem by combining elliptic methods with results from the theory of diophantine approximations.
“…Note that this is an infinite-dimensional analogue of the perturbed Cauchy-Riemann equation used to define Floer homology for general symplectomorphisms in [6]. The following main theorem of this paper is an analogue of [8,Theorem 10.4], see also [7,Theorem 3.4].…”
Section: Floer Curves In Infinite Dimensionsmentioning
confidence: 97%
“…In analogy with our work in [7] and [8], it is the goal of this paper to prove the existence of T -periodic solutions of…”
Section: The Symplectic Hilbert Spacementioning
confidence: 98%
“…In order to prove Theorem 2.1, we essentially combine our work in [7] and [8] on pseudoholomorphic curves for infinite-dimensional Hamiltonian systems with the celebrated paper [5] on pseudoholomorphic curves in cotangent bundles in order to prove an existence result for Floer curves in T * Q × H.…”
Section: Properties Of the Particle-field Hamiltonianmentioning
confidence: 99%
“…Apart from the fact that the underlying phase space M = T * Q × H is infinitedimensional, as in [7], [8] we first need to deal with the fact that the field Hamiltonian…”
Section: Properties Of the Particle-field Hamiltonianmentioning
confidence: 99%
“…As in [2], [5], [14] and [7], [8] we follow the idea of A. Floer in [9] to study flow lines of the gradient ∇ A Ḡ φ of the action functional with respect to the L 2 -metric on H 1 φ (R, T * Q × H) given by the canonical Riemannian metric •, • on M = T * Q × H. The reason why Floer preferred to choose the L 2 -gradient over the more natural H 1 -gradient follows from the observation that the gradient flow equation…”
Section: Floer Curves In Infinite Dimensionsmentioning
We consider a natural class of time-periodic infinite-dimensional nonlinear Hamiltonian systems modelling the interaction of a classical mechanical system of particles with a scalar wave field. When the field is defined on a space torus T d = R d /(2π Z) d and the coordinates of the particles are constrained to a submanifold Q ⊂ T d , we prove that the number of T -periodic solutions of the coupled Hamiltonian particle-field system is bounded from below by the Z 2 -cuplength of the space Λ contr Q of contractible loops in Q, provided that the square of the ratio T /2π of time period T and space period X = 2π is a Diophantine irrational number. The latter condition is necessary since for the infinite-dimensional version of Gromov-Floer compactness as well as for the C 0 -bounds we need to deal with small divisors.
“…Note that this is an infinite-dimensional analogue of the perturbed Cauchy-Riemann equation used to define Floer homology for general symplectomorphisms in [6]. The following main theorem of this paper is an analogue of [8,Theorem 10.4], see also [7,Theorem 3.4].…”
Section: Floer Curves In Infinite Dimensionsmentioning
confidence: 97%
“…In analogy with our work in [7] and [8], it is the goal of this paper to prove the existence of T -periodic solutions of…”
Section: The Symplectic Hilbert Spacementioning
confidence: 98%
“…In order to prove Theorem 2.1, we essentially combine our work in [7] and [8] on pseudoholomorphic curves for infinite-dimensional Hamiltonian systems with the celebrated paper [5] on pseudoholomorphic curves in cotangent bundles in order to prove an existence result for Floer curves in T * Q × H.…”
Section: Properties Of the Particle-field Hamiltonianmentioning
confidence: 99%
“…Apart from the fact that the underlying phase space M = T * Q × H is infinitedimensional, as in [7], [8] we first need to deal with the fact that the field Hamiltonian…”
Section: Properties Of the Particle-field Hamiltonianmentioning
confidence: 99%
“…As in [2], [5], [14] and [7], [8] we follow the idea of A. Floer in [9] to study flow lines of the gradient ∇ A Ḡ φ of the action functional with respect to the L 2 -metric on H 1 φ (R, T * Q × H) given by the canonical Riemannian metric •, • on M = T * Q × H. The reason why Floer preferred to choose the L 2 -gradient over the more natural H 1 -gradient follows from the observation that the gradient flow equation…”
Section: Floer Curves In Infinite Dimensionsmentioning
We consider a natural class of time-periodic infinite-dimensional nonlinear Hamiltonian systems modelling the interaction of a classical mechanical system of particles with a scalar wave field. When the field is defined on a space torus T d = R d /(2π Z) d and the coordinates of the particles are constrained to a submanifold Q ⊂ T d , we prove that the number of T -periodic solutions of the coupled Hamiltonian particle-field system is bounded from below by the Z 2 -cuplength of the space Λ contr Q of contractible loops in Q, provided that the square of the ratio T /2π of time period T and space period X = 2π is a Diophantine irrational number. The latter condition is necessary since for the infinite-dimensional version of Gromov-Floer compactness as well as for the C 0 -bounds we need to deal with small divisors.
We consider a natural class of time-periodic infinite-dimensional nonlinear Hamiltonian systems modelling the interaction of a classical mechanical system of particles with a scalar wave field. When the field is defined on a space torus $${\mathbb {T}}^d={\mathbb {R}}^d/(2\pi {\mathbb {Z}})^d$$
T
d
=
R
d
/
(
2
π
Z
)
d
and the coordinates of the particles are constrained to a submanifold $$Q\subset {\mathbb {T}}^d$$
Q
⊂
T
d
, we prove that the number of contractible T-periodic solutions of the coupled Hamiltonian particle-field system is bounded from below by the $${\mathbb {Z}}_2$$
Z
2
-cuplength of the space $$\Lambda ^{{\text {contr}}} Q$$
Λ
contr
Q
of contractible loops in Q, provided that the square of the ratio $$T/2\pi $$
T
/
2
π
of time period T and space period $$X=2\pi $$
X
=
2
π
is a Diophantine irrational number. The latter condition is necessary since for the infinite-dimensional version of Gromov–Floer compactness as well as for the $$C^0$$
C
0
-bounds we need to deal with small divisors.
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