Symmetry and resonance in Hamiltonian systems (Q2706084)
From MaRDI portal
| This is the item page for this Wikibase entity, intended for internal use and editing purposes. Please use this page instead for the normal view: Symmetry and resonance in Hamiltonian systems |
scientific article
| Language | Label | Description | Also known as |
|---|---|---|---|
| English | Symmetry and resonance in Hamiltonian systems |
scientific article |
Statements
19 March 2001
0 references
discrete symmetry
0 references
Hénon-Heiles family of Hamiltonians
0 references
two-degree-of-freedom Hamiltonian
0 references
homogeneous polynomials
0 references
normal forms
0 references
small parameter
0 references
Hamiltonian flow
0 references
equilibrium
0 references
phase space
0 references
elastic pendulum
0 references
hierarchy of resonances
0 references
2:1 resonance
0 references
4:1 resonance
0 references
asymptotic analysis
0 references
0.9236361
0 references
0.92213714
0 references
Symmetry and resonance in Hamiltonian systems (English)
0 references
The authors consider a two-degree-of-freedom Hamiltonian NEWLINE\[NEWLINEH(p_1,q_1,p_2,q_2)= \textstyle{{1\over 2}} \omega_1(p^2_1+ q^2_1)+ \textstyle{{1\over 2}} \omega_2(p^2_2+ q^2_2)+ H_3+ H_4+\cdots,NEWLINE\]NEWLINE where \(H_k\) \((k\geq 3)\) are homogeneous polynomials of degree \(k\). Using normal forms and introducing in the usual way a small parameter by rescaling the variables, the authors analyze the dynamics of Hamiltonian flow in a neighborhood of equilibrium in the origin of phase space. Due to the presence of a symmetry condition on one of the degrees of freedom, some resonances vanish as lower-order resonances. The authors give a new sharp estimate of the size of resonance domain for higher-order resonances. As an application, the authors discuss one of the classical examples with symmetry -- the elastic pendulum. In this problem, the symmetry assumption produces a new hierarchy of resonances in which, after well-known 2:1 resonance, the 4:1 resonance is the most prominent one. The asymptotic analysis is supplemented by numerical calculations which show excellent agreement.
0 references