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 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
Joint work with Melanie Stein and Peter Wong GAGTA Conference May 28, 2013
We define the Diestel-Leader group Ξπ(π) and generating set ππ(π) so that the resulting Cayley graph is the Diestel-Leader graph πΈππ π :
1 Γ π2 Γ β― Γ ππβ1 Γ ππ
t+π1 t+π2 t+ππβ1 π’β1 Formal Variables: Where the ππ β ππ are chosen so that ππ β ππ β ππ
β.
Generating set ππ π : t+ππ π 1
Β±1
and (t+ππ)(t+ππ)β1 βπ(t+ππ ) 1
Β±1
where b β ππ . This construction of the groups Ξπ(π) is due to Bartholdi, Neuhauser and Woess and requires that if p is any prime divisor of q, then d β€ p+1.
A generic element of Ξπ(π) has the form g= (π’ + ππ)ππ
πβ1 π=1
π 1 where ππ βZ and P is a polynomial in ππ[(t + π1) β1, π’ + π2 β1, β―,(t + ππβ1) β1, π’]. Decomposition Lemma: Let g β Ξπ(π) be as above. Then P can be written uniquely as P=π
1 + π2 + β― + ππβ1 + ππ
ππ is a polynomial in t+ππ with
ππ is a polynomial in π’β1with only terms of non-positive degree.
Rough idea of identification between g and a vertex in πΈππ(π): (π1, π2, β― , ππβ1) and P=π
1 + π2 + β― + ππβ1 + ππ determine the vertex in
πΈππ π corresponding to g.
Elements of Ln are often represented by a finite number of illuminated βbulbsβ along with an integral position of the βlamplighter.β
Configurations of illuminated bulbs Positions of the lamplighter
Commutator subgroup: Configurations of βbulbs,β Vertices have all coordinates at height 0 in all d-1 trees Abelianization: Positions of βlamplighter,β Coordinates represent the heights In the first d-1 trees; height in the last tree is determined.
Upper right entry is l_j-l_i
Upper right entry Is a big mess! Denote it by S-T.
In general, the commutator subgroup of Ξπ π is defined by
View as indexing conjugates of 1 1 1 by products of π’ + ππ 1
ππ
where K is generated by simply polynomial relations between the formal Variables of the form:
From the split short exact sequence we see that if Suppose that Ο corresponds to a permutation in Ξ£πwhich contains the cycle (1 2 3 β― π). Then Ο transforms the relations πΏ1,2, πΏ2,3, β― , πΏπ,1 into a system of equations which has a solution iff k=d-1=q is prime. β then
Defining relations of the kernel
If Ο=Id then this is regular conjugacy.
If Ο=Id then this is regular conjugacy.
2 is SMALL! dβ₯ π ππ π΄π©πΊπ―π πΊ !
The one diagram proofβ¦ When Ο is a permutation matrix it is easy to show that R(Ο )=β and hence that R(Ο)=β. When d=3 and q=2 we can verify this directly for the 4 remaining matrices.