Difference between revisions of "Solenoid"
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− | + | Let $ \mathbf n = \langle n _ {i} \rangle _ {i} $ | |
+ | be a sequence of positive integers. From $ \mathbf n $ | ||
+ | one constructs a topological space as follows. | ||
− | + | Let $ T _ {0} $ | |
+ | be a torus in $ \mathbf R ^ {3} $; | ||
+ | inside $ T _ {0} $ | ||
+ | one takes a torus $ T _ {1} $ | ||
+ | wrapped around longitudinally $ n _ {1} $ | ||
+ | times, in a smooth fashion without folding back; inside $ T _ {1} $ | ||
+ | one takes a torus $ T _ {2} $ | ||
+ | wrapped around $ n _ {2} $ | ||
+ | times in the same way. Continuing this procedure indefinitely, one obtains a decreasing sequence of tori. Its intersection is called the $ \mathbf n $- | ||
+ | adic solenoid $ \Sigma _ {\mathbf n } $. | ||
− | + | The basic properties of $ \Sigma _ {\mathbf n } $ | |
+ | are that it is a one-dimensional [[Continuum|continuum]] which, moreover, is indecomposable (cf. [[Indecomposable continuum|Indecomposable continuum]]). | ||
− | + | $ \Sigma _ {\mathbf n } $ | |
+ | is also a [[Topological group|topological group]]; this can be seen if one considers an alternative construction of $ \Sigma _ {\mathbf n } $ | ||
+ | as the inverse limit of the following inverse sequence: | ||
− | Solenoids were first defined by L. Vietoris [[#References|[a2]]] (for the sequence | + | $$ |
+ | {} \dots S _ {3} \rightarrow ^ { {f _ 3} } S _ {2} \mathop \rightarrow \limits ^ { {f _ {2} }} S _ {1} \rightarrow ^ { {f _ 1} } S _ {0} , | ||
+ | $$ | ||
+ | |||
+ | where each $ S _ {i} $ | ||
+ | is the unit circle and $ f _ {i} : S _ {i} \rightarrow S _ {i-} 1 $ | ||
+ | is defined by $ f _ {i} ( z)= z ^ {n _ {i} } $. | ||
+ | There are various other ways in which one can construct the solenoids, see, e.g., [[#References|[a3]]]. | ||
+ | |||
+ | Solenoids were first defined by L. Vietoris [[#References|[a2]]] (for the sequence $ \langle 2, 2 ,\dots \rangle $) | ||
+ | and by D. van Dantzig [[#References|[a1]]] (for all constant sequences). | ||
Solenoids are also important in [[Topological dynamics|topological dynamics]]; on them one can define a [[Flow (continuous-time dynamical system)|flow (continuous-time dynamical system)]] structure [[#References|[a4]]] which has a locally disconnected minimal set of almost-periodic motions. | Solenoids are also important in [[Topological dynamics|topological dynamics]]; on them one can define a [[Flow (continuous-time dynamical system)|flow (continuous-time dynamical system)]] structure [[#References|[a4]]] which has a locally disconnected minimal set of almost-periodic motions. | ||
− | There is a complete classification of the solenoids: first, without loss of generality one may assume that the numbers | + | There is a complete classification of the solenoids: first, without loss of generality one may assume that the numbers $ n _ {i} $ |
+ | are prime. Call two sequences of primes $ \mathbf p $ | ||
+ | and $ \mathbf q $ | ||
+ | equivalent if one can delete from each a finite number of terms such that in the reduced sequences $ \mathbf p ^ \prime $ | ||
+ | and $ \mathbf q ^ \prime $ | ||
+ | every prime is counted the same number of times. One can then show that $ \Sigma _ {\mathbf p } $ | ||
+ | and $ \Sigma _ {\mathbf q } $ | ||
+ | are homeomorphic if and only if $ \mathbf p $ | ||
+ | and $ \mathbf q $ | ||
+ | are equivalent. See [[#References|[a5]]] and [[#References|[a6]]]. | ||
Finally one can characterize the solenoids as those metric continua that are homogeneous and have the property that every proper subcontinuum is an [[Arc (topology)|arc]]. See [[#References|[a7]]]. | Finally one can characterize the solenoids as those metric continua that are homogeneous and have the property that every proper subcontinuum is an [[Arc (topology)|arc]]. See [[#References|[a7]]]. |
Latest revision as of 08:14, 6 June 2020
Let $ \mathbf n = \langle n _ {i} \rangle _ {i} $
be a sequence of positive integers. From $ \mathbf n $
one constructs a topological space as follows.
Let $ T _ {0} $ be a torus in $ \mathbf R ^ {3} $; inside $ T _ {0} $ one takes a torus $ T _ {1} $ wrapped around longitudinally $ n _ {1} $ times, in a smooth fashion without folding back; inside $ T _ {1} $ one takes a torus $ T _ {2} $ wrapped around $ n _ {2} $ times in the same way. Continuing this procedure indefinitely, one obtains a decreasing sequence of tori. Its intersection is called the $ \mathbf n $- adic solenoid $ \Sigma _ {\mathbf n } $.
The basic properties of $ \Sigma _ {\mathbf n } $ are that it is a one-dimensional continuum which, moreover, is indecomposable (cf. Indecomposable continuum).
$ \Sigma _ {\mathbf n } $ is also a topological group; this can be seen if one considers an alternative construction of $ \Sigma _ {\mathbf n } $ as the inverse limit of the following inverse sequence:
$$ {} \dots S _ {3} \rightarrow ^ { {f _ 3} } S _ {2} \mathop \rightarrow \limits ^ { {f _ {2} }} S _ {1} \rightarrow ^ { {f _ 1} } S _ {0} , $$
where each $ S _ {i} $ is the unit circle and $ f _ {i} : S _ {i} \rightarrow S _ {i-} 1 $ is defined by $ f _ {i} ( z)= z ^ {n _ {i} } $. There are various other ways in which one can construct the solenoids, see, e.g., [a3].
Solenoids were first defined by L. Vietoris [a2] (for the sequence $ \langle 2, 2 ,\dots \rangle $) and by D. van Dantzig [a1] (for all constant sequences).
Solenoids are also important in topological dynamics; on them one can define a flow (continuous-time dynamical system) structure [a4] which has a locally disconnected minimal set of almost-periodic motions.
There is a complete classification of the solenoids: first, without loss of generality one may assume that the numbers $ n _ {i} $ are prime. Call two sequences of primes $ \mathbf p $ and $ \mathbf q $ equivalent if one can delete from each a finite number of terms such that in the reduced sequences $ \mathbf p ^ \prime $ and $ \mathbf q ^ \prime $ every prime is counted the same number of times. One can then show that $ \Sigma _ {\mathbf p } $ and $ \Sigma _ {\mathbf q } $ are homeomorphic if and only if $ \mathbf p $ and $ \mathbf q $ are equivalent. See [a5] and [a6].
Finally one can characterize the solenoids as those metric continua that are homogeneous and have the property that every proper subcontinuum is an arc. See [a7].
References
[a1] | D. van Dantzig, "Ueber topologisch homogene Kontinua" Fund. Math. , 15 (1930) pp. 102–125 |
[a2] | L. Vietoris, "Über den höheren Zusammenhang kompakter Räume und eine Klasse von zusammenhangstreuen Abbildungen" Math. Ann. , 97 (1927) pp. 454–472 |
[a3] | E. Hewitt, K.A. Ross, "Abstract harmonic analysis" , 1 , Springer (1979) |
[a4] | V.V. Nemytskii, V.V. Stepanov, "Qualitative theory of differential equations" , Princeton Univ. Press (1960) (Translated from Russian) |
[a5] | R.H. Bing, "A simple closed curve is the only homogeneous bounded plane continuum that contains an arc" Canad. Math. J. , 12 (1960) pp. 209–230 |
[a6] | M.C. McCord, "Inverse limit sequences with covering maps" Trans. Amer. Math. Soc. , 114 (1965) pp. 197–209 |
[a7] | C.L. Hagopian, "A characterization of solenoids" Pacific J. Math. , 68 (1977) pp. 425–435 |
Solenoid. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Solenoid&oldid=48745