In mathematics, two functions are said to be topologically conjugate to one another if there exists a homeomorphism that will conjugate the one into the other. Topological conjugacy is important in the study of iterated functions and more generally dynamical systems, since, if the dynamics of one iterated function can be solved, then those for any topologically conjugate function follow trivially.
To illustrate this directly: suppose that and are iterated functions, and there exists an such that
so that f and g are topologically conjugate. Then of course one must have
being topologically semiconjugate to means, by definition, that is a surjection such that .
and being topologically conjugate means, by definition, that they are topologically semiconjugate and is a homeomorphism; further, is termed a topological conjugation between and .
Similarly, on , and on are flows, with , and as above.
being topologically semiconjugate to means, by definition, that is a surjection such that , for each , .
and being topologically conjugate means, by definition, that they are topologically semiconjugate and h is a homeomorphism.
- The logistic map and the tent map are topologically conjugate.
- The logistic map of unit height and the Bernoulli map are topologically conjugate.
Topological conjugation – unlike semiconjugation – defines an equivalence relation in the space of all continuous surjections of a topological space to itself, by declaring and to be related if they are topologically conjugate. This equivalence relation is very useful in the theory of dynamical systems, since each class contains all functions which share the same dynamics from the topological viewpoint. For example, orbits of are mapped to homeomorphic orbits of through the conjugation. Writing makes this fact evident: . Speaking informally, topological conjugation is a "change of coordinates" in the topological sense.
However, the analogous definition for flows is somewhat restrictive. In fact, we are requiring the maps and to be topologically conjugate for each , which is requiring more than simply that orbits of be mapped to orbits of homeomorphically. This motivates the definition of topological equivalence, which also partitions the set of all flows in into classes of flows sharing the same dynamics, again from the topological viewpoint.
We say that two flows and are topologically equivalent, if there is a homeomorphism , mapping orbits of to orbits of homeomorphically, and preserving orientation of the orbits. In other words, letting denote an orbit, one has
for each . In addition, one must line up the flow of time: for each , there exists a such that, if , and if s is such that , then .
Overall, topological equivalence is a weaker equivalence criterion than topological conjugacy, as it does not require that the time term is mapped along with the orbits and their orientation. An example of a topologically equivalent but not topologically conjugate system would be the non-hyperbolic class of two dimensional systems of differential equations that have closed orbits. While the orbits can be transformed to each other to overlap in the spatial sense, the periods of such systems cannot be analogously matched, thus failing to satisfy the topological conjugacy criterion while satisfying the topological equivalence criterion.
Smooth and orbital equivalence
More equivalence criteria can be studied if the flows, and , arise from differential equations.
Two dynamical systems defined by the differential equations, and , are said to be smoothly equivalent if there is a diffeomorphism, , such that
In that case, the dynamical systems can be transformed into each other by the coordinate transformation, .
Two dynamical systems on the same state space, defined by and , are said to be orbitally equivalent if there is a positive function, , such that . Orbitally equivalent system differ only in the time parametrization.
Systems that are smoothly equivalent or orbitally equivalent are also topologically equivalent. However, the reverse is not true. For example, consider linear systems in two dimensions of the form . If the matrix, , has two positive real eigenvalues, the system has an unstable node; if the matrix has two complex eigenvalues with positive real part, the system has an unstable focus (or spiral). Nodes and foci are topologically equivalent but not orbitally equivalent or smoothly equivalent, because their eigenvalues are different (notice that the Jacobians of two locally smoothly equivalent systems must be similar, so their eigenvalues, as well as algebraic and geometric multiplicities, must be equal).
Generalizations of dynamic topological conjugacy
There are two reported extensions of the concept of dynamic topological conjugacy:
- Analogous systems defined as isomorphic dynamical systems
- Adjoint dynamical systems defined via adjoint functors and natural equivalences in categorical dynamics.
- Alligood, K. T., Sauer, T., and Yorke, J.A. (1997). Chaos: An Introduction to Dynamical Systems. Springer. pp. 114–124. ISBN 0-387-94677-2.
- Kuznetsov, Yuri A. (1998). Elements of Bifurcation Theory (Second ed.). Springer. ISBN 0-387-98382-1.
- http://planetphysics.org/encyclopedia/Complexity.html Complexity and Categorical Dynamics
- http://planetphysics.org/encyclopedia/AnalogousSystems3.html Analogous systems, Topological Conjugacy and Adjoint Systems