Global Aspects of Classical Integrable Systems
By R. Cushman, L. Bates. 2004
514 citations recorded by the source corpus.
Subfields: Geometry and Topology, Statistical and Nonlinear Physics
View Paper: https://www.semanticscholar.org/paper/2a633f3334ecc5de0673f3a2099374ac24fc9032
How researchers see this paper
The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.
In Geometry and Topology
- 'Alvaro Pelayo
- San Vũ Ngọc
- Tudor S. Ratiu
- Nguyen Tien Zung
- Mikhail Lemeshko
- J. Hoo
- Emilio Freire
- Francesco Fassò
In Statistical and Nonlinear Physics
- 'Alvaro Pelayo
- San Vũ Ngọc
- Tudor S. Ratiu
- Nguyen Tien Zung
- Guido Blankenstein
- Mikhail Lemeshko
- J. Hoo
- Francesco Fassò
Citations in the corpus
- Symplectic theory of completely integrable Hamiltonian systems (2011, background): “ out by many authors, including Marsden, Ratiu and their collaborators. The semiclassical aspects of integrable systems have been recently studied in the book [110] and the article [109]. In the book [26] singular Lagrangian fibrations are treated from the point of view of classical mechanics. Finall”
- Quantum control of molecular rotation (2018, methodology): “The two systems are known as the Euler top and the Lagrange top in mathematics and have been studied for many centuries (Cushman and Bates, 1997).”
- Normal linear stability of quasi-periodic tori (2007, methodology): “The Hamiltonian 1 : −1 resonance is of interest, since it is observed in many mechanical systems including the Lagrange top [34,35], the double spherical pendulum [63], the restricted three body problem [64] and the 3D Hénon–Heiles family as this models the movement of galaxies [38,46,47].”
- Continuation of periodic orbits in conservative and Hamiltonian systems (2003, methodology): “Following Cushman and Bates [5] we define a mapping w : C2 → R3 by w1 = w1(z) := i(ab̄ − āb), w2 = w2(z) := ab̄ + āb, w3 = w3(z) := aā − bb̄, ∀z = (a, b) ∈ C2; (8.11) together with F (z) the scalar functions w1(z), w2(z) and w3(z) form a basis for the quadratic invariants under the S1-action on C”
- Singular reduction of implicit Hamiltonian systems (2003, methodology): “Define the set of smooth functions on M0 as follows (see [9], or for the original source see [25]).”
- Superintegrable Hamiltonian Systems: Geometry and Perturbations (2005, background): “Monodromy has been identified in several Liouville integrable systems, see, e.g., [ 14 ], and plays an important role in their quantization, see, e.g., [46, 15] and references therein.”
- Symplectic Topology of Integrable Hamiltonian Systems, II: Topological Classification (2000, methodology): “us interesting examples. 2. Regular Lagrangian torus foliations This Section is based on the works of Duistermaat [15] and Dazord and Delzant [11] (see also Boucetta and Molino [7], Cushman and Bates [9], and Marle [23]). 2.1. Action-angle coordinates. Let π : (M2n,ω,L) → On be a regular Lagrangian ”