Diestel-Leader Groups Jennifer Taback Bowdoin College Joint work - - PowerPoint PPT Presentation

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Diestel-Leader Groups Jennifer Taback Bowdoin College Joint work - - PowerPoint PPT Presentation

Automorphisms of Diestel-Leader Groups Jennifer Taback Bowdoin College Joint work with Melanie Stein and Peter Wong GAGTA Conference May 28, 2013 Diestel-Leader Groups We define the Diestel-Leader group () and generating set


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Automorphisms of Diestel-Leader Groups

Jennifer Taback Bowdoin College

Joint work with Melanie Stein and Peter Wong GAGTA Conference May 28, 2013

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Diestel-Leader Groups

We define the Diestel-Leader group Γ𝑒(π‘Ÿ) and generating set 𝑇𝑒(π‘Ÿ) so that the resulting Cayley graph is the Diestel-Leader graph 𝐸𝑀𝑒 π‘Ÿ :

𝐸𝑀𝑒 π‘Ÿ βŠ† π‘ˆ

1 Γ— π‘ˆ2 Γ— β‹― Γ— π‘ˆπ‘’βˆ’1 Γ— π‘ˆπ‘’

t+π‘š1 t+π‘š2 t+π‘šπ‘’βˆ’1 π‘’βˆ’1 Formal Variables: Where the π‘šπ‘— ∈ π‘Žπ‘Ÿ are chosen so that π‘šπ‘— βˆ’ π‘šπ‘˜ ∈ π‘Žπ‘Ÿ

βˆ—.

Generating set 𝑇𝑒 π‘Ÿ : t+π‘šπ‘— 𝑐 1

Β±1

and (t+π‘šπ‘—)(t+π‘šπ‘˜)βˆ’1 βˆ’π‘(t+π‘šπ‘˜ ) 1

Β±1

where b ∈ π‘Žπ‘Ÿ . This construction of the groups Γ𝑒(π‘Ÿ) is due to Bartholdi, Neuhauser and Woess and requires that if p is any prime divisor of q, then d ≀ p+1.

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Diestel-Leader Groups

A generic element of Γ𝑒(π‘Ÿ) has the form g= (𝑒 + π‘šπ‘—)𝑓𝑗

π‘’βˆ’1 𝑗=1

𝑄 1 where 𝑓𝑗 ∈Z and P is a polynomial in π‘Žπ‘Ÿ[(t + π‘š1) βˆ’1, 𝑒 + π‘š2 βˆ’1, β‹―,(t + π‘šπ‘’βˆ’1) βˆ’1, 𝑒]. Decomposition Lemma: Let g ∈ Γ𝑒(π‘Ÿ) be as above. Then P can be written uniquely as P=𝑄

1 + 𝑄2 + β‹― + π‘„π‘’βˆ’1 + 𝑄𝑒

𝑄𝑗 is a polynomial in t+π‘šπ‘— with

  • nly negative degree terms.

𝑄𝑒 is a polynomial in π‘’βˆ’1with only terms of non-positive degree.

Rough idea of identification between g and a vertex in 𝐸𝑀𝑒(π‘Ÿ): (𝑓1, 𝑓2, β‹― , π‘“π‘’βˆ’1) and P=𝑄

1 + 𝑄2 + β‹― + π‘„π‘’βˆ’1 + 𝑄𝑒 determine the vertex in

𝐸𝑀𝑒 π‘Ÿ corresponding to g.

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Algebraic comparison to Lamplighter groups

Lamplighter group:

π‘€π‘œ = π‘Žπ‘œβˆ« Z = < a,t |π‘π‘œ=1, [𝑏𝑒𝑗, π‘π‘’π‘˜]=1,i,j∈ π‘Ž>

Elements of Ln are often represented by a finite number of illuminated β€œbulbs” along with an integral position of the β€œlamplighter.”

Configurations of illuminated bulbs Positions of the lamplighter

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Algebraic comparison to Lamplighter groups

Diestel-Leader groups

Here L is the analog of the infinite string of β€œlamps” and is the union of d-1 rays in π‘Žπ‘’βˆ’1.

Commutator subgroup: Configurations of β€œbulbs,” Vertices have all coordinates at height 0 in all d-1 trees Abelianization: Positions of β€œlamplighter,” Coordinates represent the heights In the first d-1 trees; height in the last tree is determined.

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Automorphisms of Diestel-Leader groups

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Induced automorphisms on the quotient

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Proof that induced automorphisms of the quotient are permutation matrices

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Proof that induced automorphisms of the quotient are permutation matrices

Upper right entry is l_j-l_i

Question: What is 𝑄𝑒?

Upper right entry Is a big mess! Denote it by S-T.

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Proof that induced automorphisms of the quotient are permutation matrices

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Understanding the commutator subgroup Γ𝑒(π‘Ÿ)β€²

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The commutator subgroup of Γ𝑒(π‘Ÿ)

In general, the commutator subgroup of Γ𝑒 π‘Ÿ is defined by

View as indexing conjugates of 1 1 1 by products of 𝑒 + π‘šπ‘— 1

𝑓𝑗

where K is generated by simply polynomial relations between the formal Variables of the form:

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Further restriction of induced automorphisms

  • f π‘Žπ‘’βˆ’1

From the split short exact sequence we see that if Suppose that Ο† corresponds to a permutation in Σ𝑒which contains the cycle (1 2 3 β‹― 𝑙). Then Ο† transforms the relations 𝐿1,2, 𝐿2,3, β‹― , 𝐿𝑙,1 into a system of equations which has a solution iff k=d-1=q is prime. ∎ then

Defining relations of the kernel

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Counting twisted conjugacy classes in Γ𝑒(q)

If Ο•=Id then this is regular conjugacy.

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Counting twisted conjugacy classes in Γ𝑒(q)

If Ο•=Id then this is regular conjugacy.

2 is SMALL! dβ‰₯ πŸ’ 𝒋𝒕 𝑴𝑩𝑺𝑯𝑭 𝑺 !

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Counting twisted conjugacy classes in Γ𝑒(q)

The one diagram proof… When Ο† is a permutation matrix it is easy to show that R(Ο† )=∞ and hence that R(Ο•)=∞. When d=3 and q=2 we can verify this directly for the 4 remaining matrices.