2004
DOI: 10.1088/0305-4470/37/24/011
|View full text |Cite
|
Sign up to set email alerts
|

Perturbation theory and control in classical or quantum mechanics by an inversion formula

Abstract: We consider a perturbation of an "integrable" Hamiltonian and give an expression for the canonical or unitary transformation which "simplifies" this perturbed system. The problem is to invert a functional defined on the Lie-algebra of observables. We give a bound for the perturbation in order to solve this inversion. And apply this result to a particular case of the control theory, as a first example, and to the "quantum adiabatic transformation", as another example.

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

0
67
0
10

Year Published

2004
2004
2012
2012

Publication Types

Select...
7

Relationship

0
7

Authors

Journals

citations
Cited by 33 publications
(77 citation statements)
references
References 8 publications
0
67
0
10
Order By: Relevance
“…whose Hamiltonian can be written as H = H 0 + V , where H 0 is integrable and V a perturbation of order ǫ (compared to H 0 ). The results we use here have been proven rigorously [7,8]. In practice, it can be shown that a suitable control term f of order ǫ 2 exists such that H 0 + V + f has an invariant torus at a given frequency ω 0 .…”
Section: Hamiltonian Control Of a Test-particlementioning
confidence: 79%
“…whose Hamiltonian can be written as H = H 0 + V , where H 0 is integrable and V a perturbation of order ǫ (compared to H 0 ). The results we use here have been proven rigorously [7,8]. In practice, it can be shown that a suitable control term f of order ǫ 2 exists such that H 0 + V + f has an invariant torus at a given frequency ω 0 .…”
Section: Hamiltonian Control Of a Test-particlementioning
confidence: 79%
“…[27] for conservative systems that can be described by a near-integrable Hamiltonian of the form H = H 0 + εV , where H 0 is integrable and εV is a small perturbation with ε 1. For ε = 0, the dynamics is integrable, and the phase space presents just invariant tori.…”
Section: Methods Of Controlmentioning
confidence: 99%
“…[27] and presented in Refs. [28][29][30], which consists of the addition of a small perturbation to the Hamiltonian.…”
Section: Introductionmentioning
confidence: 99%
“…The goal of this paper is to present a reliable improvement of beam stability by increasing the DA in a simplified accelerator model, consisting of only one type of element having a sextupole nonlinearity [2,3,4,5]. We work in the framework of the Hamiltonian Control Theory presented in [7,8], where two methods of controlling symplectic maps have been described, namely using Lie transformations and generating functions. In the present paper we use the former method, which allows direct determination of the new controlled map; avoiding the possible problems related to coordinate inversion.…”
Section: Introductionmentioning
confidence: 99%