- a fixed point,
- a periodic orbit, or
- a connected set composed of a finite number of fixed points together with homoclinic and heteroclinic orbits connecting these.
Moreover, there is at most one orbit connecting different fixed points in the same direction. However, there could be countably many homoclinic orbits connecting one fixed point.
The condition that the dynamical system be on the plane is necessary to the theorem. On a torus, for example, it is possible to have a recurrent non-periodic orbit. In particular, chaotic behaviour can only arise in continuous dynamical systems whose phase space has three or more dimensions. However the theorem does not apply to discrete dynamical systems, where chaotic behaviour can arise in two- or even one-dimensional systems.
One important implication is that a two-dimensional continuous dynamical system cannot give rise to a strange attractor. If a strange attractor C did exist in such a system, then it could be enclosed in a closed and bounded subset of the phase space. By making this subset small enough, any nearby stationary points could be excluded. But then the Poincaré–Bendixson theorem says that C is not a strange attractor at all—it is either a limit cycle or it converges to a limit cycle.
- Coddington, Earl A.; Levinson, Norman (1955). "The Poincaré–Bendixson Theory of Two-Dimensional Autonomous Systems". Theory of Ordinary Differential Equations. New York: McGraw-Hill. pp. 389–403. ISBN 0-89874-755-4.
- Teschl, Gerald (2012). Ordinary Differential Equations and Dynamical Systems. Providence: American Mathematical Society. ISBN 978-0-8218-8328-0.
- D'Heedene, R.N. (1961). "A third order autonomous differential equation with almost periodic solutions". Journal of Mathematical Analysis and Applications. Elsevier. 3 (2): 344–350. doi:10.1016/0022-247X(61)90059-2. Retrieved 8 July 2016.