fully irreducible automorphism

{{Short description|Concept in mathematics}}

In the mathematical subject geometric group theory, a fully irreducible automorphism of the free group Fn is an element of Out(Fn) which has no periodic conjugacy classes of proper free factors in Fn (where n > 1). Fully irreducible automorphisms are also referred to as "irreducible with irreducible powers" or "iwip" automorphisms. The notion of being fully irreducible provides a key Out(Fn) counterpart of the notion of a pseudo-Anosov element of the mapping class group of a finite type surface. Fully irreducibles play an important role in the study of structural properties of individual elements and of subgroups of Out(Fn).

Formal definition

Let \varphi\in \operatorname{Out}(F_n) where n\ge 2. Then \varphi is called fully irreducibleThierry Coulbois and Arnaud Hilion, Botany of irreducible automorphisms of free groups, Pacific Journal of Mathematics 256 (2012), 291–307 if there do not exist an integer p\ne 0 and a proper free factor A of F_n such that \varphi^p([A])=[A], where [A] is the conjugacy class of A in F_n.

Here saying that A is a proper free factor of F_n means that A\ne 1 and there exists a subgroup B\le F_n, B\ne 1 such that F_n=A\ast B.

Also, \Phi\in \operatorname{Aut}(F_n) is called fully irreducible if the outer automorphism class \varphi\in \operatorname{Out}(F_n) of \Phi is fully irreducible.

Two fully irreducibles \varphi,\psi\in \operatorname{Out}(F_n) are called independent if \langle \varphi\rangle \cap \langle \psi \rangle = \{1\}.

=Relationship to irreducible automorphisms=

The notion of being fully irreducible grew out of an older notion of an "irreducible" outer automorphism of F_n originally introduced in. An element \varphi\in \operatorname{Out}(F_n), where n\ge 2, is called irreducible if there does not exist a free product decomposition

:F_n=A_1\ast\dots \ast A_k \ast C

with k\ge 1, and with A_i\ne 1, i=1,\dots k being proper free factors of F_n, such that \varphi permutes the conjugacy classes [A_1], \dots, [A_k] .

Then \varphi\in \operatorname{Out}(F_n) is fully irreducible in the sense of the definition above if and only if for every p\ne 0 \varphi^p is irreducible.

It is known that for any atoroidal \varphi\in \operatorname{Out}(F_n) (that is, without periodic conjugacy classes of nontrivial elements of F_n), being irreducible is equivalent to being fully irreducible.Ilya Kapovich, Algorithmic detectability of iwip automorphisms. Bulletin of the London Mathematical Society 46 (2014), no. 2, 279–290. For non-atoroidal automorphisms, Bestvina and Handel produce an example of an irreducible but not fully irreducible element of \operatorname{Out}(F_n), induced by a suitably chosen pseudo-Anosov homeomorphism of a surface with more than one boundary component.

Properties

  • If \varphi\in \operatorname{Out}(F_n) and p\ne 0 then \varphi is fully irreducible if and only if \varphi^p is fully irreducible.
  • Every fully irreducible \varphi\in \operatorname{Out}(F_n) can be represented by an expanding irreducible train track map.Mladen Bestvina, and Michael Handel, [https://www.jstor.org/pss/2946562 Train tracks and automorphisms of free groups.] Annals of Mathematics (2), vol. 135 (1992), no. 1, pp. 1–51
  • Every fully irreducible \varphi\in \operatorname{Out}(F_n) has exponential growth in F_n given by a stretch factor \lambda=\lambda(\varphi)>1. This stretch factor has the property that for every free basis X of F_n (and, more generally, for every point of the Culler–Vogtmann Outer space X\in cv_n) and for every 1\ne g\in F_n one has:

:: \lim_{k\to\infty}\sqrt[k]{\|\varphi^k(g)\|_X}=\lambda.

Moreover, \lambda=\lambda(\varphi) is equal to the Perron–Frobenius eigenvalue of the transition matrix of any train track representative of \varphi.Oleg Bogopolski. [https://books.google.com/books?id=jEw8MpP6DIgC&dq=Oleg+Bogopolski+Introduction+to+Group+Theory&pg=PT1 Introduction to group theory.] EMS Textbooks in Mathematics. European Mathematical Society, Zürich, 2008. {{ISBN|978-3-03719-041-8}}

  • Unlike for stretch factors of pseudo-Anosov surface homeomorphisms, it can happen that for a fully irreducible \varphi\in \operatorname{Out}(F_n) one has \lambda(\varphi)\ne \lambda(\varphi^{-1})Michael Handel, and Lee Mosher, [https://www.ams.org/journals/tran/2007-359-07/S0002-9947-07-04065-2/S0002-9947-07-04065-2.pdf Parageometric outer automorphisms of free groups.] Transactions of the American Mathematical Society 359 (2007), no. 7, 3153–3183 and this behavior is believed to be generic. However, Handel and MosherMichael Handel, Lee Mosher, [https://www.ams.org/journals/tran/2007-359-07/S0002-9947-07-04066-4/S0002-9947-07-04066-4.pdf The expansion factors of an outer automorphism and its inverse.] Transactions of the American Mathematical Society 359 (2007), no. 7, 3185–3208 proved that for every n\ge 2 there exists a finite constant 0< C_n <\infty such that for every fully irreducible \varphi\in \operatorname{Out}(F_n)

:: \frac{\log\lambda(\varphi) }{\log \lambda(\varphi^{-1})} \le C_n.

  • A fully irreducible \varphi\in \operatorname{Out}(F_n) is non-atoroidal, that is, has a periodic conjugacy class of a nontrivial element of F_n, if and only if \varphi is induced by a pseudo-Anosov homeomorphism of a compact connected surface with one boundary component and with the fundamental group isomorphic to F_n.
  • A fully irreducible element \varphi\in \operatorname{Out}(F_n) has exactly two fixed points in the Thurston compactification \overline{CV}_n of the projectivized Outer space CV_n, and \varphi\in \operatorname{Out}(F_n) acts on \overline{CV}_n with "North-South" dynamics.{{citation

| last1 = Levitt | first1 = Gilbert

| last2 = Lustig | first2 = Martin

| title = Automorphisms of free groups have asymptotically periodic dynamics

| journal = Journal für die reine und angewandte Mathematik

| pages = 1–36

| volume = 2008

| year = 2008

| issue = 619

| doi=10.1515/CRELLE.2008.038| arxiv = math/0407437

| s2cid = 14724939

}}

  • For a fully irreducible element \varphi\in \operatorname{Out}(F_n), its fixed points in \overline{CV}_n are projectivized \mathbb R-trees [T_+(\varphi)], [T_-(\varphi)], where T_+(\varphi),T_-(\varphi)\in \overline{cv}_n, satisfying the property that T_+(\varphi)\varphi=\lambda(\varphi) T_+(\varphi) and T_-(\varphi)\varphi^{-1}=\lambda(\varphi^{-1}) T_-(\varphi) .
  • A fully irreducible element \varphi\in \operatorname{Out}(F_n) acts on the space of projectivized geodesic currents \mathbb PCurr(F_n) with either "North-South" or "generalized North-South" dynamics, depending on whether \varphi is atoroidal or non-atoroidal.Caglar Uyanik, Dynamics of hyperbolic iwips. Conformal Geometry and Dynamics 18 (2014), 192–216.Caglar Uyanik, Generalized north-south dynamics on the space of geodesic currents. Geometriae Dedicata 177 (2015), 129–148.
  • If \varphi\in \operatorname{Out}(F_n) is fully irreducible, then the commensurator Comm(\langle \varphi\rangle)\le \operatorname{Out}(F_n) is virtually cyclic.Ilya Kapovich, and Martin Lustig, Stabilizers of \mathbb{R}-trees with free isometric actions of FN.

Journal of Group Theory 14 (2011), no. 5, 673–694. In particular, the centralizer and the normalizer of \langle \varphi\rangle in \operatorname{Out}(F_n) are virtually cyclic.

  • If \varphi,\psi\in \operatorname{Out}(F_n) are independent fully irreducibles, then [T_\pm(\varphi)], [T_\pm(\psi)]\in \overline{CV}_n are four distinct points, and there exists M\ge 1 such that for every p,q\ge M the subgroup \langle \varphi^p, \psi^q\rangle \le \operatorname{Out}(F_n) is isomorphic to F_2.
  • If \varphi\in \operatorname{Out}(F_n) is fully irreducible and \varphi\in H\le \operatorname{Out}(F_n), then either H is virtually cyclic or H contains a subgroup isomorphic to F_2.Mladen Bestvina, Mark Feighn and Michael Handel, Laminations, trees, and irreducible automorphisms of free groups. Geometric and Functional Analysis 7 (1997), 215–244. [This statement provides a strong form of the Tits alternative for subgroups of \operatorname{Out}(F_n) containing fully irreducibles.]
  • If H\le \operatorname{Out}(F_n) is an arbitrary subgroup, then either H contains a fully irreducible element, or there exist a finite index subgroup H_0\le H and a proper free factor A of F_n such that H_0[A]=[A].Camille Horbez, A short proof of Handel and Mosher's alternative for subgroups of Out(FN). Groups, Geometry, and Dynamics 10 (2016), no. 2, 709–721.
  • An element \varphi\in \operatorname{Out}(F_n) acts as a loxodromic isometry on the free factor complex \mathcal{FF}_n if and only if \varphi is fully irreducible.Mladen Bestvina, and Mark Feighn, Hyperbolicity of the complex of free factors. Advances in Mathematics 256 (2014), 104–155.
  • It is known that "random" (in the sense of random walks) elements of \operatorname{Out}(F_n) are fully irreducible. More precisely, if \mu is a measure on \operatorname{Out}(F_n) whose support generates a semigroup in \operatorname{Out}(F_n) containing some two independent fully irreducibles. Then for the random walk of length k on \operatorname{Out}(F_n) determined by \mu, the probability that we obtain a fully irreducible element converges to 1 as k\to \infty.Joseph Maher and Giulio Tiozzo, [https://www.degruyter.com/view/j/crll.ahead-of-print/crelle-2015-0076/crelle-2015-0076.xml Random walks on weakly hyperbolic groups], Journal für die reine und angewandte Mathematik, Ahead of print (Jan 2016); cf. Theorem 1.4
  • A fully irreducible element \varphi\in \operatorname{Out}(F_n) admits a (generally non-unique) periodic axis in the volume-one normalized Outer space X_n, which is geodesic with respect to the asymmetric Lipschitz metric on X_n and possesses strong "contraction"-type properties.Yael Algom-Kfir,

Strongly contracting geodesics in outer space.

Geometry & Topology 15 (2011), no. 4, 2181–2233. A related object, defined for an atoroidal fully irreducible \varphi\in \operatorname{Out}(F_n), is the axis bundle A_\varphi\subseteq X_n, which is a certain \varphi-invariant closed subset proper homotopy equivalent to a line.Michael Handel, and Lee Mosher,

Axes in outer space. Memoirs of the American Mathematical Society 213 (2011), no. 1004; {{ISBN|978-0-8218-6927-7}}.

References

{{Reflist}}

Further reading

Category:Geometric group theory

Category:Geometric topology