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Representations of one-dimensional Hamiltonians in terms of their invariants

Journal Article · · Journal of Mathematical Physics (New York); (United States)
DOI:https://doi.org/10.1063/1.529794· OSTI ID:5399540
 [1];  [2]; ;  [3]
  1. Los Alamos National Laboratory, Los Alamos, New Mexico 87545 (United States)
  2. CNLS-CAMS, University of the Witwatersrand, Johannesburg, Wits Post Office, 2050 (South Africa)
  3. Physique Mathematique, Modelisation et Simulation, C.N.R.S., 45071 Orleans Cedex 2 (France)
A general formalism for representing the Hamiltonian of a system with one degree of freedom in terms of its invariants is developed. Those Hamiltonians {ital H}({ital q},{ital p},{ital t}) are derived for which any particular function {ital I}({ital q},{ital p},{ital t}) is an invariant. For each of those Hamiltonians, a function canonically conjugate to {ital I}({ital q},{ital p},{ital t}) is derived which is also an invariant of {ital H}({ital q},{ital p},{ital t}). The formalism is also presented for the case in which {ital I}({ital q},{ital p},{ital t}) is expressed as a function of two canonically conjugate functions. The formalism is illustrated by applying it to the case of a particle moving in a time-dependent potential. Some earlier results are recovered and an invariant is found for a new potential. Lines for further study are outlined that may be fruitful for finding more examples of integrable systems.
OSTI ID:
5399540
Journal Information:
Journal of Mathematical Physics (New York); (United States), Journal Name: Journal of Mathematical Physics (New York); (United States) Vol. 33:2; ISSN 0022-2488; ISSN JMAPA
Country of Publication:
United States
Language:
English