Floquet operators with singular spectrum. II
Annales de l'I.H.P. Physique théorique (1989)
- Volume: 50, Issue: 3, page 325-334
- ISSN: 0246-0211
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topHowland, James S.. "Floquet operators with singular spectrum. II." Annales de l'I.H.P. Physique théorique 50.3 (1989): 325-334. <http://eudml.org/doc/76450>.
@article{Howland1989,
author = {Howland, James S.},
journal = {Annales de l'I.H.P. Physique théorique},
keywords = {spectral properties; Floquet operator; eigenvalues},
language = {eng},
number = {3},
pages = {325-334},
publisher = {Gauthier-Villars},
title = {Floquet operators with singular spectrum. II},
url = {http://eudml.org/doc/76450},
volume = {50},
year = {1989},
}
TY - JOUR
AU - Howland, James S.
TI - Floquet operators with singular spectrum. II
JO - Annales de l'I.H.P. Physique théorique
PY - 1989
PB - Gauthier-Villars
VL - 50
IS - 3
SP - 325
EP - 334
LA - eng
KW - spectral properties; Floquet operator; eigenvalues
UR - http://eudml.org/doc/76450
ER -
References
top- [1] J. Bellissard, Stability and Instability in Quantum Mechanics, in Trends and Developments in the Eighties, ALBEVARIO and BLANCHARD Eds., World Scientific, Singapore, 1985. Zbl0584.35024MR853743
- [2] G. Hagadorn, M. Loss and J. Slawny, Non-stochasticity of time-dependent quadratic Hamiltonians and the spectra of canonical transformations, J. Phys. A, Vol. 19, 1986, pp. 521-531. Zbl0601.70013MR833433
- [3] J.S. Howland, Scattering Theory for Hamiltonians Periodic in Time, Indiana J. Math., Vol. 28, 1979, pp. 471-494. Zbl0444.47010MR529679
- [4] J.S. Howland, Floquet Operators with Singular Spectrum, I. Ann. Inst. H. Poincaré (to appear). Zbl0689.34022
Citations in EuDML Documents
top- G. Nenciu, Floquet operators without absolutely continuous spectrum
- James S. Howland, Floquet operators with singular spectrum. III
- G. Nenciu, Adiabatic theory : stability of systems with increasing gaps
- P. Duclos, P. Šťovíček, M. Vittot, Perturbation of an eigen-value from a dense point spectrum : a general Floquet hamiltonian
- Sandro Graffi, Méthodes KAM pour les opérateurs de Schrödinger non autonomes
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