Van Kampen diagram

In the

The notion of a Van Kampen diagram was introduced by Egbert van Kampen in 1933.^[4] This paper appeared in the same issue of American Journal of Mathematics as another paper of Van Kampen, where he proved what is now known as the Seifert–Van Kampen theorem.^[5] The main result of the paper on Van Kampen diagrams, now known as the van Kampen lemma can be deduced from the Seifert–Van Kampen theorem by applying the latter to the presentation complex of a group.^[6] However, Van Kampen did not notice it at the time and this fact was only made explicit much later (see, e.g.^[7]). Van Kampen diagrams remained an underutilized tool in group theory for about thirty years, until the advent of the small cancellation theory in the 1960s, where Van Kampen diagrams play a central role.^[8] Currently Van Kampen diagrams are a standard tool in geometric group theory. They are used, in particular, for the study of isoperimetric functions in groups, and their various generalizations such as isodiametric functions, filling length functions, and so on.

Formal definition

The definitions and notations below largely follow Lyndon and Schupp.^[9]

Let

${\displaystyle G=\langle A|R\,\rangle }$   (†)

be a

A Van Kampen diagram over the presentation (†) is a planar finite

${\displaystyle {\mathcal {D}}\,}$

${\displaystyle {\mathcal {D}}\subseteq \mathbb {R} ^{2}\,}$

1. The complex ${\displaystyle {\mathcal {D}}\,}$ is connected and
   simply connected
   .
2. Each edge (one-cell) of ${\displaystyle {\mathcal {D}}\,}$ is labelled by an arrow and a letter a∈A.
3. Some vertex (zero-cell) which belongs to the topological boundary of ${\displaystyle {\mathcal {D}}\subseteq \mathbb {R} ^{2}\,}$ is specified as a base-vertex.
4. For each region (two-cell) of ${\displaystyle {\mathcal {D}}}$, for every vertex on the boundary cycle of that region, and for each of the two choices of direction (clockwise or counter-clockwise), the label of the boundary cycle of the region read from that vertex and in that direction is a freely reduced word in F(A) that belongs to R_∗.

Thus the 1-skeleton of ${\displaystyle {\mathcal {D}}\,}$ is a finite connected planar graph Γ embedded in ${\displaystyle \mathbb {R} ^{2}\,}$ and the two-cells of ${\displaystyle {\mathcal {D}}\,}$ are precisely the bounded complementary regions for this graph.

By the choice of R_∗ Condition 4 is equivalent to requiring that for each region of ${\displaystyle {\mathcal {D}}\,}$ there is some boundary vertex of that region and some choice of direction (clockwise or counter-clockwise) such that the boundary label of the region read from that vertex and in that direction is freely reduced and belongs to R.

A Van Kampen diagram ${\displaystyle {\mathcal {D}}\,}$ also has the boundary cycle, denoted ${\displaystyle \partial {\mathcal {D}}\,}$, which is an edge-path in the graph Γ corresponding to going around ${\displaystyle {\mathcal {D}}\,}$ once in the clockwise direction along the boundary of the unbounded complementary region of Γ, starting and ending at the base-vertex of ${\displaystyle {\mathcal {D}}\,}$. The label of that boundary cycle is a word w in the alphabet A ∪ A⁻¹ (which is not necessarily freely reduced) that is called the boundary label of ${\displaystyle {\mathcal {D}}\,}$.

Further terminology

• A Van Kampen diagram ${\displaystyle {\mathcal {D}}\,}$ is called a disk diagram if ${\displaystyle {\mathcal {D}}\,}$ is a topological disk, that is, when every edge of ${\displaystyle {\mathcal {D}}\,}$ is a boundary edge of some region of ${\displaystyle {\mathcal {D}}\,}$ and when ${\displaystyle {\mathcal {D}}\,}$ has no cut-vertices.
• A Van Kampen diagram ${\displaystyle {\mathcal {D}}\,}$ is called non-reduced if there exists a reduction pair in ${\displaystyle {\mathcal {D}}\,}$, that is a pair of distinct regions of ${\displaystyle {\mathcal {D}}\,}$ such that their boundary cycles share a common edge and such that their boundary cycles, read starting from that edge, clockwise for one of the regions and counter-clockwise for the other, are equal as words in A ∪ A⁻¹. If no such pair of region exists, ${\displaystyle {\mathcal {D}}\,}$ is called reduced.
• The number of regions (two-cells) of ${\displaystyle {\mathcal {D}}\,}$ is called the area of ${\displaystyle {\mathcal {D}}\,}$ denoted ${\displaystyle {\rm {Area}}({\mathcal {D}})\,}$.

In general, a Van Kampen diagram has a "cactus-like" structure where one or more disk-components joined by (possibly degenerate) arcs, see the figure below:

Example

The following figure shows an example of a Van Kampen diagram for the free abelian group of rank two

${\displaystyle G=\langle a,b|aba^{-1}b^{-1}\rangle .}$

The boundary label of this diagram is the word

${\displaystyle w=b^{-1}b^{3}a^{-1}b^{-2}ab^{-1}ba^{-1}ab^{-1}ba^{-1}a.}$

The area of this diagram is equal to 8.

Van Kampen lemma

A key basic result in the theory is the so-called Van Kampen lemma^[9] which states the following:

1. Let ${\displaystyle {\mathcal {D}}\,}$ be a Van Kampen diagram over the presentation (†) with boundary label w which is a word (not necessarily freely reduced) in the alphabet A ∪ A⁻¹. Then w=1 in G.
2. Let w be a freely reduced word in the alphabet A ∪ A⁻¹ such that w=1 in G. Then there exists a reduced Van Kampen diagram ${\displaystyle {\mathcal {D}}\,}$ over the presentation (†) whose boundary label is freely reduced and is equal to w.

Sketch of the proof

First observe that for an element w ∈ F(A) we have w = 1 in G if and only if w belongs to the normal closure of R in F(A) that is, if and only if w can be represented as

${\displaystyle w=u_{1}s_{1}u_{1}^{-1}\cdots u_{n}s_{n}u_{n}^{-1}{\text{ in }}F(A),}$   (♠)

where n ≥ 0 and where s_i ∈ R_∗ for i = 1, ..., n.

Part 1 of Van Kampen's lemma is proved by induction on the area of ${\displaystyle {\mathcal {D}}\,}$. The inductive step consists in "peeling" off one of the boundary regions of ${\displaystyle {\mathcal {D}}\,}$ to get a Van Kampen diagram ${\displaystyle {\mathcal {D}}'\,}$ with boundary cycle w and observing that in F(A) we have

${\displaystyle w=usu^{-1}w',\,}$

where s∈R_∗ is the boundary cycle of the region that was removed to get ${\displaystyle {\mathcal {D}}'\,}$ from ${\displaystyle {\mathcal {D}}\,}$.

The proof of part two of Van Kampen's lemma is more involved. First, it is easy to see that if w is freely reduced and w = 1 in G there exists some Van Kampen diagram ${\displaystyle {\mathcal {D}}_{0}\,}$ with boundary label w₀ such that w = w₀ in F(A) (after possibly freely reducing w₀). Namely consider a representation of w of the form (♠) above. Then make ${\displaystyle {\mathcal {D}}_{0}\,}$ to be a wedge of n "lollipops" with "stems" labeled by u_i and with the "candys" (2-cells) labelled by s_i. Then the boundary label of ${\displaystyle {\mathcal {D}}_{0}\,}$ is a word w₀ such that w = w₀ in F(A). However, it is possible that the word w₀ is not freely reduced. One then starts performing "folding" moves to get a sequence of Van Kampen diagrams ${\displaystyle {\mathcal {D}}_{0},{\mathcal {D}}_{1},{\mathcal {D}}_{2},\dots \,}$ by making their boundary labels more and more freely reduced and making sure that at each step the boundary label of each diagram in the sequence is equal to w in F(A). The sequence terminates in a finite number of steps with a Van Kampen diagram ${\displaystyle {\mathcal {D}}_{k}\,}$ whose boundary label is freely reduced and thus equal to w as a word. The diagram ${\displaystyle {\mathcal {D}}_{k}\,}$ may not be reduced. If that happens, we can remove the reduction pairs from this diagram by a simple surgery operation without affecting the boundary label. Eventually this produces a reduced Van Kampen diagram ${\displaystyle {\mathcal {D}}\,}$ whose boundary cycle is freely reduced and equal to w.

Strengthened version of Van Kampen's lemma

Moreover, the above proof shows that the conclusion of Van Kampen's lemma can be strengthened as follows.^[9] Part 1 can be strengthened to say that if ${\displaystyle {\mathcal {D}}\,}$ is a Van Kampen diagram of area n with boundary label w then there exists a representation (♠) for w as a product in F(A) of exactly n conjugates of elements of R_∗. Part 2 can be strengthened to say that if w is freely reduced and admits a representation (♠) as a product in F(A) of n conjugates of elements of R_∗ then there exists a reduced Van Kampen diagram with boundary label w and of area at most n.

Dehn functions and isoperimetric functions

Area of a word representing the identity

Let w ∈ F(A) be such that w = 1 in G. Then the area of w, denoted Area(w), is defined as the minimum of the areas of all Van Kampen diagrams with boundary labels w (Van Kampen's lemma says that at least one such diagram exists).

One can show that the area of w can be equivalently defined as the smallest n≥0 such that there exists a representation (♠) expressing w as a product in F(A) of n conjugates of the defining relators.

Isoperimetric functions and Dehn functions

A nonnegative

${\displaystyle {\rm {Area}}(w)\leq f(|w|),}$

where |w| is the length of the word w.

Suppose now that the alphabet A in (†) is finite. Then the Dehn function of (†) is defined as

${\displaystyle {\rm {Dehn}}(n)=\max\{{\rm {Area}}(w):w=1{\text{ in }}G,|w|\leq n,w{\text{ freely reduced}}.\}}$

It is easy to see that Dehn(n) is an isoperimetric function for (†) and, moreover, if f(n) is any other isoperimetric function for (†) then Dehn(n) ≤ f(n) for every n ≥ 0.

Let w ∈ F(A) be a freely reduced word such that w = 1 in G. A Van Kampen diagram ${\displaystyle {\mathcal {D}}\,}$ with boundary label w is called minimal if ${\displaystyle {\rm {Area}}({\mathcal {D}})={\rm {Area}}(w).}$ Minimal Van Kampen diagrams are discrete analogues of minimal surfaces in Riemannian geometry.

Generalizations and other applications

• There are several generalizations of van-Kampen diagrams where instead of being planar, connected and simply connected (which means being
  Klein's bottle
  are related to elements that are conjugated to their own inverse.
• Van Kampen diagrams are central objects in the
  group presentations where the defining relations have "small overlaps" with each other. This condition is reflected in the geometry of reduced Van Kampen diagrams over small cancellation presentations, forcing certain kinds of non-positively curved or negatively cn curved behavior. This behavior yields useful information about algebraic and algorithmic properties of small cancellation groups, in particular regarding the word and the conjugacy problems. Small cancellation theory was one of the key precursors of geometric group theory, that emerged as a distinct mathematical area in the late 1980s and it remains an important part of geometric group theory
  .
• Van Kampen diagrams play a key role in the theory of
  finitely presented group either it is hyperbolic and satisfies a linear isoperimetric inequality or else the Dehn function is at least quadratic.^[13][14]
• The study of isoperimetric functions for finitely presented groups has become an important general theme in geometric group theory where substantial progress has occurred. Much work has gone into constructing groups with "fractional" Dehn functions (that is, with Dehn functions being polynomials of non-integer degree).^[15] The work of Rips, Ol'shanskii, Birget and Sapir^[16][17] explored the connections between Dehn functions and time complexity functions of Turing machines and showed that an arbitrary "reasonable" time function can be realized (up to appropriate equivalence) as the Dehn function of some finitely presented group.
• Various stratified and relativized versions of Van Kampen diagrams have been explored in the subject as well. In particular, a stratified version of small cancellation theory, developed by Ol'shanskii, resulted in constructions of various group-theoretic "monsters", such as the
  Tarski Monster,^[18] and in geometric solutions of the Burnside problem for periodic groups of large exponent.^[19][20] Relative versions of Van Kampen diagrams (with respect to a collection of subgroups) were used by Osin to develop an isoperimetric function approach to the theory of relatively hyperbolic groups.^[21]

• Geometric group theory
• Presentation of a group
• Seifert–Van Kampen theorem

Basic references

• Alexander Yu. Ol'shanskii. Geometry of defining relations in groups. Translated from the 1989 Russian original by Yu. A. Bakhturin. Mathematics and its Applications (Soviet Series), 70. Kluwer Academic Publishers Group, Dordrecht, 1991.
  ISBN 0-7923-1394-1
• Roger C. Lyndon and Paul E. Schupp. Combinatorial Group Theory. Springer-Verlag, New York, 2001. "Classics in Mathematics" series, reprint of the 1977 edition.
  ISBN 978-3-540-41158-1
  ; Ch. V. Small Cancellation Theory. pp. 235–294.