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1: 29.19 Physical Applications
§29.19(i) Lamé Functions
Brack et al. (2001) shows that Lamé functions occur at bifurcations in chaotic Hamiltonian systems. …
2: 32.6 Hamiltonian Structure
§32.6 Hamiltonian Structure
The Hamiltonian for P I  is … The Hamiltonian for P II  is … The Hamiltonian for P III  (§32.2(iii)) is …
3: Bibliography Y
  • H. A. Yamani and W. P. Reinhardt (1975) L -squared discretizations of the continuum: Radial kinetic energy and the Coulomb Hamiltonian. Phys. Rev. A 11 (4), pp. 1144–1156.
  • 4: 36.13 Kelvin’s Ship-Wave Pattern
    The wake is a caustic of the “rays” defined by the dispersion relation (“Hamiltonian”) giving the frequency ω as a function of wavevector 𝐤 : …
    5: Bibliography B
  • T. Bountis, H. Segur, and F. Vivaldi (1982) Integrable Hamiltonian systems and the Painlevé property. Phys. Rev. A (3) 25 (3), pp. 1257–1264.
  • M. Brack, M. Mehta, and K. Tanaka (2001) Occurrence of periodic Lamé functions at bifurcations in chaotic Hamiltonian systems. J. Phys. A 34 (40), pp. 8199–8220.
  • 6: Bibliography
  • J. V. Armitage (1989) The Riemann Hypothesis and the Hamiltonian of a Quantum Mechanical System. In Number Theory and Dynamical Systems (York, 1987), M. M. Dodson and J. A. G. Vickers (Eds.), London Math. Soc. Lecture Note Ser., Vol. 134, pp. 153–172.
  • 7: 18.39 Applications in the Physical Sciences
    The fundamental quantum Schrödinger operator, also called the Hamiltonian, , is a second order differential operator of the form …
    8: 1.18 Linear Second Order Differential Operators and Eigenfunction Expansions
    The sum of the kinetic and potential energies give the quantum Hamiltonian, or energy operator; often also referred to as a Schrödinger operator. …