143 research outputs found
Nonexistence of an integral of the 6th degree in momenta for the Zipoy-Voorhees metric
We prove nonexistence of a nontrivial integral that is polynomial in momenta
of degree less than 7 for the Zipoy-Voorhees spacetime with the parameter
Comment: 7 pages, no figure
A Poincar\'e section for the general heavy rigid body
A general recipe is developed for the study of rigid body dynamics in terms
of Poincar\'e surfaces of section. A section condition is chosen which captures
every trajectory on a given energy surface. The possible topological types of
the corresponding surfaces of section are determined, and their 1:1 projection
to a conveniently defined torus is proposed for graphical rendering.Comment: 25 pages, 10 figure
Topology of energy surfaces and existence of transversal Poincar\'e sections
Two questions on the topology of compact energy surfaces of natural two
degrees of freedom Hamiltonian systems in a magnetic field are discussed. We
show that the topology of this 3-manifold (if it is not a unit tangent bundle)
is uniquely determined by the Euler characteristic of the accessible region in
configuration space. In this class of 3-manifolds for most cases there does not
exist a transverse and complete Poincar\'e section. We show that there are
topological obstacles for its existence such that only in the cases of
and such a Poincar\'e section can exist.Comment: 10 pages, LaTe
The problem of two fixed centres: bifurcations, actions, monodromy
A comprehensive analysis of the Euler-Jacobi problem of motion in the field of two fixed
attracting centers is given, first classically and then quantum mechanically in semiclassical
approximation. The system was originally studied in the context of celestial mechanics
but, starting with Pauli’s dissertation, became a model for one-electron molecules such as
H+
2 (symmetric case of equal centers) or HHe2+ (asymmetric case of different centers).
The present paper deals with arbitrary relative strength of the two centers and considers
separately the planar and the three-dimensional problems. All versions represent nontrivial
examples of integrable dynamics and are studied here from the unifying point of view
of the energy momentum mapping from phase space to the space of integration constants.
The interesting objects are the critical values of this mapping, i. e., its bifurcation diagram,
and their pre-images which organize the foliation of phase space into Liouville-Arnold
tori. The classical analysis culminates in the explicit derivation of the action variable
representation of iso-energetic surfaces. The attempt to identify a system of global actions,
smoothly dependent on the integration constants wherever these are non-critical, leads to
the detection of monodromy of a special kind which is here described for the first time.
The classical monodromy has its counterpart in the quantum version of the two-center
problem where it prevents the assignments of unique quantum numbers even though the
system is separable
About ergodicity in the family of limacon billiards
By continuation from the hyperbolic limit of the cardioid billiard we show
that there is an abundance of bifurcations in the family of limacon billiards.
The statistics of these bifurcation shows that the size of the stable intervals
decreases with approximately the same rate as their number increases with the
period. In particular, we give numerical evidence that arbitrarily close to the
cardioid there are elliptic islands due to orbits created in saddle node
bifurcations. This shows explicitly that if in this one parameter family of
maps ergodicity occurs for more than one parameter the set of these parameter
values has a complicated structure.Comment: 17 pages, 9 figure
Maslov Indices and Monodromy
We prove that for a Hamiltonian system on a cotangent bundle that is
Liouville-integrable and has monodromy the vector of Maslov indices is an
eigenvector of the monodromy matrix with eigenvalue 1. As a corollary the
resulting restrictions on the monodromy matrix are derived.Comment: 6 page
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