A geometric approach to a result of Benci and Giannoni for Hamiltonian systems with singular potentials.
Zhu Daxin (1991)
Manuscripta mathematica
Similarity:
The search session has expired. Please query the service again.
The search session has expired. Please query the service again.
The search session has expired. Please query the service again.
The search session has expired. Please query the service again.
Zhu Daxin (1991)
Manuscripta mathematica
Similarity:
Patricio L. Felmer (1990)
Manuscripta mathematica
Similarity:
Takashi Ichinose, Tetsuo Tsuchida (1993)
Forum mathematicum
Similarity:
Vieri Benci, Donato Fortunato (1987)
Manuscripta mathematica
Similarity:
Maria Letizia Bertotti (1989)
Manuscripta mathematica
Similarity:
Boris Khesin (1993)
Recherche Coopérative sur Programme n°25
Similarity:
Klaus Thews (1980/81)
Manuscripta mathematica
Similarity:
Antonio Ambrosetti, V. Coti Zelati (1989)
Mathematische Zeitschrift
Similarity:
Fiorella Barone, Renato Grassini (2003)
Banach Center Publications
Similarity:
Dirac's generalized Hamiltonian dynamics is given an accurate geometric formulation as an implicit differential equation and is compared with Tulczyjew's formulation of dynamics. From the comparison it follows that Dirac's equation-unlike Tulczyjew's-fails to give a complete picture of the real laws of classical and relativistic dynamics.
E. Zenhder (1975)
Publications mathématiques et informatique de Rennes
Similarity:
B.A. Kupershmidt, George Wilson (1980/81)
Inventiones mathematicae
Similarity:
Gary Chartrand, S. F. Kapoor (1974)
Colloquium Mathematicae
Similarity:
Jens-P. Bode, Anika Fricke, Arnfried Kemnitz (2015)
Discussiones Mathematicae Graph Theory
Similarity:
In 1980 Bondy [2] proved that a (k+s)-connected graph of order n ≥ 3 is traceable (s = −1) or Hamiltonian (s = 0) or Hamiltonian-connected (s = 1) if the degree sum of every set of k+1 pairwise nonadjacent vertices is at least ((k+1)(n+s−1)+1)/2. It is shown in [1] that one can allow exceptional (k+ 1)-sets violating this condition and still implying the considered Hamiltonian property. In this note we generalize this result for s = −1 and s = 0 and graphs that fulfill a certain connectivity...
Rodman, Leiba (2008)
ELA. The Electronic Journal of Linear Algebra [electronic only]
Similarity:
Henryk Żołądek (2011)
Banach Center Publications
Similarity:
The first and the second Painlevé equations are explicitly Hamiltonian with time dependent Hamilton function. By a natural extension of the phase space one gets corresponding autonomous Hamiltonian systems in ℂ⁴. We prove that the latter systems do not have any additional algebraic first integral. In the proof equations in variations with respect to a parameter are used.
D. Z. Du, D. F. Hsu (1989)
Banach Center Publications
Similarity:
Huang, Xuncheng, Tu, Guizhang (2006)
International Journal of Mathematics and Mathematical Sciences
Similarity: