proceedings of the
american mathematical society
Volume 113, Number 3, November 1991
ENTROPY AND COMPLETELY INTEGRABLE
HAMILTONIAN SYSTEMS
GABRIEL PATERNAIN
(Communicated by Kenneth R. Meyer)
Abstract. Let H be a Hamiltonian on a four-dimensional symplectic man-
ifold. Suppose the system is completely integrable and on some nonsingular
compact level surface Q the integral is such that the connected components of
the set of critical points form submanifolds. Then we prove that the topologi-
cal entropy of the system restricted to Q is zero. As a corollary we deduce the
nonexistence of completely integrable geodesic flows by means of integrals as
described above for compact surfaces with negative Euler characteristic.
1. Introduction
Let M be a four-dimensional symplectic manifold and H a Hamiltonian on
M. Denote by sgrad H the symplectic gradient of H. Let Q be a nonsingular
compact level surface of H. Suppose the system is completely integrable; that
is, suppose there exists an additional function on M which is independent of
H (almost everywhere) and is in involution with H (such a function is called
an integral). Restricting this integral to Q gives a smooth function /. Denote
by htop the topological entropy of the Hamiltonian flow restricted to Q. In
this article we want to prove the following:
Theorem 1. Let M be a smooth symplectic manifold and let sgrad// be a
Hamiltonian field on M4 . Suppose that the system is completely integrable and
that on some nonsingular compact level surface Q the integral f verifies either
of the following conditions:
(a) / is real analytic.
(b) The connected components of the set of critical points of f form sub-
manifolds.
Then hlo=0.
top
Received by the editors March 9, 1990.
1980 Mathematics Subject Classification (1985 Revision). Primary 58F07, 58F11; Secondary
58F17.
Key words and phrases. Completely integrable Hamiltonians, topological entropy, geodesic flow,
homoclinic orbits, integral.
© 1991 American Mathematical Society
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