Solenoid (mathematics)

This page discusses a class of topological groups. For the wrapped loop of wire, see Solenoid.

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The Smale-Williams solenoid.

In mathematics, a solenoid is a compact connected topological space (i.e. a continuum) that may be obtained as the inverse limit of an inverse system of topological groups and continuous homomorphisms

(S_i, f_i),     f_i: S_i+1 → S_i,     i ≥ 0,

where each S_i is a circle and f_i is the map that uniformly wraps the circle S_i+1 n_i times (n_i ≥ 2) around the circle S_i. This construction can be carried out geometrically in the three-dimensional Euclidean space R³. A solenoid is a one-dimensional homogeneous indecomposable continuum that has the structure of a compact topological group.

In the special case where all n_i have the same value n, so that the inverse system is determined by the multiplication by n self map of the circle, solenoids were first introduced by Vietoris for n = 2 and by van Dantzig for an arbitrary n. Such a solenoid arises as a one-dimensional expanding attractor, or Smale–Williams attractor, and forms an important example in the theory of hyperbolic dynamical systems.

Geometric construction and the Smale–Williams attractor[]

A solid torus wrapped twice around inside another solid torus in R³

The first six steps in the construction of the Smale-Williams attractor.

Each solenoid may be constructed as the intersection of a nested system of embedded solid tori in R³.

Fix a sequence of natural numbers {n_i}, n_i ≥ 2. Let T₀ = S¹ × D be a solid torus. For each i ≥ 0, choose a solid torus T_i+1 that is wrapped longitudinally n_i times inside the solid torus T_i. Then their intersection

${\displaystyle \Lambda =\bigcap _{i\geq 0}T_{i}}$

is homeomorphic to the solenoid constructed as the inverse limit of the system of circles with the maps determined by the sequence {n_i}.

Here is a variant of this construction isolated by Stephen Smale as an example of an expanding attractor in the theory of smooth dynamical systems. Denote the angular coordinate on the circle S¹ by t (it is defined mod 2π) and consider the complex coordinate z on the two-dimensional unit disk D. Let f be the map of the solid torus T = S¹ × D into itself given by the explicit formula

${\displaystyle f(t,z)=\left(2t,{\tfrac {1}{4}}z+{\tfrac {1}{2}}e^{it}\right).}$

This map is a smooth embedding of T into itself that preserves the foliation by meridional disks (the constants 1/2 and 1/4 are somewhat arbitrary, but it is essential that 1/4 < 1/2 and 1/4 + 1/2 < 1). If T is imagined as a rubber tube, the map f stretches it in the longitudinal direction, contracts each meridional disk, and wraps the deformed tube twice inside T with twisting, but without self-intersections. The hyperbolic set Λ of the discrete dynamical system (T, f) is the intersection of the sequence of nested solid tori described above, where T_i is the image of T under the ith iteration of the map f. This set is a one-dimensional (in the sense of topological dimension) attractor, and the dynamics of f on Λ has the following interesting properties:

• meridional disks are the stable manifolds, each of which intersects Λ over a Cantor set
• periodic points of f are dense in Λ
• the map f is topologically transitive on Λ

General theory of solenoids and expanding attractors, not necessarily one-dimensional, was developed by R. F. Williams and involves a projective system of infinitely many copies of a compact branched manifold in place of the circle, together with an expanding self-immersion.

Pathological properties[]

Solenoids are compact metrizable spaces that are connected, but not locally connected or path connected. This is reflected in their pathological behavior with respect to various homology theories, in contrast with the standard properties of homology for simplicial complexes. In Čech homology, one can construct a non-exact long homology sequence using a solenoid. In Steenrod-style homology theories,^[1] the 0th homology group of a solenoid may have a fairly complicated structure, even though a solenoid is a connected space.

See also[]

• Protorus, a class of topological groups that includes the solenoids
• Pontryagin duality
• Inverse limit
• p-adic number
• Profinite integer

References[]

This article includes a list of general references, but it lacks sufficient corresponding inline citations. Please help to improve this article by introducing more precise citations. (January 2012) (Learn how and when to remove this template message)

• D. van Dantzig, Ueber topologisch homogene Kontinua, Fund. Math. 15 (1930), pp. 102–125
• "Solenoid", Encyclopedia of Mathematics, EMS Press, 2001 [1994]
• Clark Robinson, Dynamical systems: Stability, Symbolic Dynamics and Chaos, 2nd edition, CRC Press, 1998 ISBN 978-0-8493-8495-0
• S. Smale, Differentiable dynamical systems, Bull. of the AMS, 73 (1967), 747 – 817.
• L. Vietoris, Über den höheren Zusammenhang kompakter Räume und eine Klasse von zusammenhangstreuen Abbildungen, Math. Ann. 97 (1927), pp. 454–472
• Robert F. Williams, Expanding attractors, Publ. Math. IHES, t. 43 (1974), p. 169–203

Further reading[]

• Semmes, Stephen (12 January 2012), Some remarks about solenoids, arXiv:1201.2647, Bibcode:2012arXiv1201.2647S