Handlebodies, Artin–Tits and HOMFLYPT
Or: All I know about Artin–Tits groups; and a filler for the remaining59minutes Daniel Tubbenhauer
Many open problems,e.g.the
word problem.
Flavor one. Finite
and affine types helps
Flavor two. Con-
figuration spaces helps
Flavor three. Map- ping class groups
helps
Flavor four. Right angled groups
helps
Artin–Tits (braid) groups
Vanilla fla- vor. ?????.
?
My failure. What I would like to understand, but I do not.
Artin–Tits groups come in four main flavors.
Question: Why are these special? What happens in general type?
A different idea for today:
However, this “naive” approach fails for most3-manifolds. Why? Because I do not know what Hecke/Soergel analog
to use for an arbitrary3-manifold.
Today. I explain what we can do.
braids in a3-ball𝒟3
My failure. What I would like to understand, but I do not. Artin–Tits groups come in four main flavors.
Question: Why are these special? What happens in general type?
A different idea for today:
What can Artin–Tits groups tell you about flavor two? However, this “naive” approach fails for most3-manifolds. Why? Because I do not know what Hecke/Soergel analog
to use for an arbitrary3-manifold.
Today. I explain what we can do.
braids in a3-ball𝒟3 𝒷
links in a3-ball𝒟3
Alexander’s theorem
My failure. What I would like to understand, but I do not. Artin–Tits groups come in four main flavors.
Question: Why are these special? What happens in general type?
A different idea for today:
What can Artin–Tits groups tell you about flavor two? However, this “naive” approach fails for most3-manifolds. Why? Because I do not know what Hecke/Soergel analog
to use for an arbitrary3-manifold.
Today. I explain what we can do.
braids in a3-ball𝒟3 𝒷
links in a3-ball𝒟3
Alexander’s theorem
𝒷
𝒸 𝒷
𝒸
=
extra relations for braids
Markov’s theorem
My failure. What I would like to understand, but I do not. Artin–Tits groups come in four main flavors.
Question: Why are these special? What happens in general type?
A different idea for today:
What can Artin–Tits groups tell you about flavor two? However, this “naive” approach fails for most3-manifolds. Why? Because I do not know what Hecke/Soergel analog
to use for an arbitrary3-manifold.
Today. I explain what we can do.
braids in a3-ball𝒟3 𝒷
links in a3-ball𝒟3
Alexander’s theorem
𝒷
𝒸 𝒷
𝒸
=
extra relations for braids
Markov’s theorem
algebraic way to study
links in a3-ball𝒟3
combine
My failure. What I would like to understand, but I do not. Artin–Tits groups come in four main flavors.
Question: Why are these special? What happens in general type?
A different idea for today:
What can Artin–Tits groups tell you about flavor two? However, this “naive” approach fails for most3-manifolds. Why? Because I do not know what Hecke/Soergel analog
to use for an arbitrary3-manifold.
Today. I explain what we can do.
braids in a3-ball𝒟3 𝒷
links in a3-ball𝒟3
Alexander’s theorem
𝒷
𝒸 𝒷
𝒸
=
extra relations for braids
Markov’s theorem
algebraic way to study
links in a3-ball𝒟3
combine
Type A He- cke algebra
My failure. What I would like to understand, but I do not. Artin–Tits groups come in four main flavors.
Question: Why are these special? What happens in general type?
A different idea for today:
What can Artin–Tits groups tell you about flavor two? However, this “naive” approach fails for most3-manifolds. Why? Because I do not know what Hecke/Soergel analog
to use for an arbitrary3-manifold.
Today. I explain what we can do.
braids in a3-ball𝒟3 𝒷
links in a3-ball𝒟3
Alexander’s theorem
𝒷
𝒸 𝒷
𝒸
=
extra relations for braids
Markov’s theorem
algebraic way to study
links in a3-ball𝒟3
combine
Type A He- cke algebra
Braid invariant
Satisfies braid relations
My failure. What I would like to understand, but I do not. Artin–Tits groups come in four main flavors.
Question: Why are these special? What happens in general type?
A different idea for today:
What can Artin–Tits groups tell you about flavor two? However, this “naive” approach fails for most3-manifolds. Why? Because I do not know what Hecke/Soergel analog
to use for an arbitrary3-manifold.
Today. I explain what we can do.
braids in a3-ball𝒟3 𝒷
links in a3-ball𝒟3
Alexander’s theorem
𝒷
𝒸 𝒷
𝒸
=
extra relations for braids
Markov’s theorem
algebraic way to study
links in a3-ball𝒟3
combine
Type A He- cke algebra
Braid invariant
Satisfies braid relations
Markov
Markov
My failure. What I would like to understand, but I do not. Artin–Tits groups come in four main flavors.
Question: Why are these special? What happens in general type?
A different idea for today:
What can Artin–Tits groups tell you about flavor two? However, this “naive” approach fails for most3-manifolds. Why? Because I do not know what Hecke/Soergel analog
to use for an arbitrary3-manifold.
Today. I explain what we can do.
braids in a3-ball𝒟3 𝒷
links in a3-ball𝒟3
Alexander’s theorem
𝒷
𝒸 𝒷
𝒸
=
extra relations for braids
Markov’s theorem
algebraic way to study
links in a3-ball𝒟3
combine
Type A He- cke algebra
Braid invariant
Satisfies braid relations
Markov
Markov
Invariant of links in𝒟3
combine
HOMFLYPT polynomial
My failure. What I would like to understand, but I do not. Artin–Tits groups come in four main flavors.
Question: Why are these special? What happens in general type?
A different idea for today:
What can Artin–Tits groups tell you about flavor two? However, this “naive” approach fails for most3-manifolds. Why? Because I do not know what Hecke/Soergel analog
to use for an arbitrary3-manifold.
Today. I explain what we can do.
braids in a3-ball𝒟3 𝒷
links in a3-ball𝒟3
Alexander’s theorem
𝒷
𝒸 𝒷
𝒸
=
extra relations for braids
Markov’s theorem
algebraic way to study
links in a3-ball𝒟3
combine
Type A He- cke algebra
Braid invariant
Satisfies braid relations
Markov
Markov
Invariant of links in𝒟3
combine
Type A He- cke category
HOMFLYPT polynomial
My failure. What I would like to understand, but I do not. Artin–Tits groups come in four main flavors.
Question: Why are these special? What happens in general type?
A different idea for today:
What can Artin–Tits groups tell you about flavor two? However, this “naive” approach fails for most3-manifolds. Why? Because I do not know what Hecke/Soergel analog
to use for an arbitrary3-manifold.
Today. I explain what we can do.
braids in a3-ball𝒟3 𝒷
links in a3-ball𝒟3
Alexander’s theorem
𝒷
𝒸 𝒷
𝒸
=
extra relations for braids
Markov’s theorem
algebraic way to study
links in a3-ball𝒟3
combine
Type A He- cke algebra
Braid invariant
Satisfies braid relations
Markov
Markov
Invariant of links in𝒟3
combine
Type A He- cke category
Braid invariant
Satisfies braid relations
HOMFLYPT polynomial
My failure. What I would like to understand, but I do not. Artin–Tits groups come in four main flavors.
Question: Why are these special? What happens in general type?
A different idea for today:
What can Artin–Tits groups tell you about flavor two? However, this “naive” approach fails for most3-manifolds. Why? Because I do not know what Hecke/Soergel analog
to use for an arbitrary3-manifold.
Today. I explain what we can do.
braids in a3-ball𝒟3 𝒷
links in a3-ball𝒟3
Alexander’s theorem
𝒷
𝒸 𝒷
𝒸
=
extra relations for braids
Markov’s theorem
algebraic way to study
links in a3-ball𝒟3
combine
Type A He- cke algebra
Braid invariant
Satisfies braid relations
Markov
Markov
Invariant of links in𝒟3
combine
Type A He- cke category
Braid invariant
Satisfies braid relations
Markov invariant
Markov 2-trace
HOMFLYPT polynomial
My failure. What I would like to understand, but I do not. Artin–Tits groups come in four main flavors.
Question: Why are these special? What happens in general type?
A different idea for today:
What can Artin–Tits groups tell you about flavor two? However, this “naive” approach fails for most3-manifolds. Why? Because I do not know what Hecke/Soergel analog
to use for an arbitrary3-manifold.
Today. I explain what we can do.
braids in a3-ball𝒟3 𝒷
links in a3-ball𝒟3
Alexander’s theorem
𝒷
𝒸 𝒷
𝒸
=
extra relations for braids
Markov’s theorem
algebraic way to study
links in a3-ball𝒟3
combine
Type A He- cke algebra
Braid invariant
Satisfies braid relations
Markov
Markov
Invariant of links in𝒟3
combine
Type A He- cke category
Braid invariant
Satisfies braid relations
Markov invariant
Markov 2-trace
Invariant of links in𝒟3
combine
HOMFLYPT homology
HOMFLYPT polynomial
My failure. What I would like to understand, but I do not. Artin–Tits groups come in four main flavors.
Question: Why are these special? What happens in general type?
A different idea for today:
What can Artin–Tits groups tell you about flavor two? However, this “naive” approach fails for most3-manifolds. Why? Because I do not know what Hecke/Soergel analog
to use for an arbitrary3-manifold.
Today. I explain what we can do.
braids in a3-mfdℳ3
My failure. What I would like to understand, but I do not. Artin–Tits groups come in four main flavors.
Question: Why are these special? What happens in general type?
A different idea for today:
What can Artin–Tits groups tell you about flavor two? However, this “naive” approach fails for most3-manifolds. Why? Because I do not know what Hecke/Soergel analog
to use for an arbitrary3-manifold.
Today. I explain what we can do.
braids in a3-mfdℳ3 𝒷
links in a3-mfdℳ3
Alexander’s theorem
My failure. What I would like to understand, but I do not. Artin–Tits groups come in four main flavors.
Question: Why are these special? What happens in general type?
A different idea for today:
What can Artin–Tits groups tell you about flavor two? However, this “naive” approach fails for most3-manifolds. Why? Because I do not know what Hecke/Soergel analog
to use for an arbitrary3-manifold.
Today. I explain what we can do.
braids in a3-mfdℳ3 𝒷
links in a3-mfdℳ3
Alexander’s theorem
𝒷
𝒸 𝒷
𝒸
=
extra relations for braids
Markov’s theorem
My failure. What I would like to understand, but I do not. Artin–Tits groups come in four main flavors.
Question: Why are these special? What happens in general type?
A different idea for today:
What can Artin–Tits groups tell you about flavor two? However, this “naive” approach fails for most3-manifolds. Why? Because I do not know what Hecke/Soergel analog
to use for an arbitrary3-manifold.
Today. I explain what we can do.
braids in a3-mfdℳ3 𝒷
links in a3-mfdℳ3
Alexander’s theorem
𝒷
𝒸 𝒷
𝒸
=
extra relations for braids
Markov’s theorem
algebraic way to study
links in a3-mfdℳ3
combine
My failure. What I would like to understand, but I do not. Artin–Tits groups come in four main flavors.
Question: Why are these special? What happens in general type?
A different idea for today:
What can Artin–Tits groups tell you about flavor two? However, this “naive” approach fails for most3-manifolds. Why? Because I do not know what Hecke/Soergel analog
to use for an arbitrary3-manifold.
Today. I explain what we can do.
braids in a3-mfdℳ3 𝒷
links in a3-mfdℳ3
Alexander’s theorem
𝒷
𝒸 𝒷
𝒸
=
extra relations for braids
Markov’s theorem
algebraic way to study
links in a3-mfdℳ3
combine
Type ? He- cke algebra
My failure. What I would like to understand, but I do not. Artin–Tits groups come in four main flavors.
Question: Why are these special? What happens in general type?
A different idea for today:
What can Artin–Tits groups tell you about flavor two? However, this “naive” approach fails for most3-manifolds. Why? Because I do not know what Hecke/Soergel analog
to use for an arbitrary3-manifold.
Today. I explain what we can do.
braids in a3-mfdℳ3 𝒷
links in a3-mfdℳ3
Alexander’s theorem
𝒷
𝒸 𝒷
𝒸
=
extra relations for braids
Markov’s theorem
algebraic way to study
links in a3-mfdℳ3
combine
Type ? He- cke algebra
Braid invariant
Satisfies braid relations?
My failure. What I would like to understand, but I do not. Artin–Tits groups come in four main flavors.
Question: Why are these special? What happens in general type?
A different idea for today:
What can Artin–Tits groups tell you about flavor two? However, this “naive” approach fails for most3-manifolds. Why? Because I do not know what Hecke/Soergel analog
to use for an arbitrary3-manifold.
Today. I explain what we can do.
braids in a3-mfdℳ3 𝒷
links in a3-mfdℳ3
Alexander’s theorem
𝒷
𝒸 𝒷
𝒸
=
extra relations for braids
Markov’s theorem
algebraic way to study
links in a3-mfdℳ3
combine
Type ? He- cke algebra
Braid invariant
Satisfies braid relations?
Markov
Markov
My failure. What I would like to understand, but I do not. Artin–Tits groups come in four main flavors.
Question: Why are these special? What happens in general type?
A different idea for today:
What can Artin–Tits groups tell you about flavor two? However, this “naive” approach fails for most3-manifolds. Why? Because I do not know what Hecke/Soergel analog
to use for an arbitrary3-manifold.
Today. I explain what we can do.
braids in a3-mfdℳ3 𝒷
links in a3-mfdℳ3
Alexander’s theorem
𝒷
𝒸 𝒷
𝒸
=
extra relations for braids
Markov’s theorem
algebraic way to study
links in a3-mfdℳ3
combine
Type ? He- cke algebra
Braid invariant
Satisfies braid relations?
Markov
Markov
Invariant of links inℳ3
combine
“HOMFLYPT polynomial”
My failure. What I would like to understand, but I do not. Artin–Tits groups come in four main flavors.
Question: Why are these special? What happens in general type?
A different idea for today:
What can Artin–Tits groups tell you about flavor two? However, this “naive” approach fails for most3-manifolds. Why? Because I do not know what Hecke/Soergel analog
to use for an arbitrary3-manifold.
Today. I explain what we can do.
braids in a3-mfdℳ3 𝒷
links in a3-mfdℳ3
Alexander’s theorem
𝒷
𝒸 𝒷
𝒸
=
extra relations for braids
Markov’s theorem
algebraic way to study
links in a3-mfdℳ3
combine
Type ? He- cke algebra
Braid invariant
Satisfies braid relations?
Markov
Markov
Invariant of links inℳ3
combine
Type ? He- cke category
“HOMFLYPT polynomial”
My failure. What I would like to understand, but I do not. Artin–Tits groups come in four main flavors.
Question: Why are these special? What happens in general type?
A different idea for today:
What can Artin–Tits groups tell you about flavor two? However, this “naive” approach fails for most3-manifolds. Why? Because I do not know what Hecke/Soergel analog
to use for an arbitrary3-manifold.
Today. I explain what we can do.
braids in a3-mfdℳ3 𝒷
links in a3-mfdℳ3
Alexander’s theorem
𝒷
𝒸 𝒷
𝒸
=
extra relations for braids
Markov’s theorem
algebraic way to study
links in a3-mfdℳ3
combine
Type ? He- cke algebra
Braid invariant
Satisfies braid relations?
Markov
Markov
Invariant of links inℳ3
combine
Type ? He- cke category
Braid invariant
Satisfies braid relations?
“HOMFLYPT polynomial”
My failure. What I would like to understand, but I do not. Artin–Tits groups come in four main flavors.
Question: Why are these special? What happens in general type?
A different idea for today:
What can Artin–Tits groups tell you about flavor two? However, this “naive” approach fails for most3-manifolds. Why? Because I do not know what Hecke/Soergel analog
to use for an arbitrary3-manifold.
Today. I explain what we can do.
braids in a3-mfdℳ3 𝒷
links in a3-mfdℳ3
Alexander’s theorem
𝒷
𝒸 𝒷
𝒸
=
extra relations for braids
Markov’s theorem
algebraic way to study
links in a3-mfdℳ3
combine
Type ? He- cke algebra
Braid invariant
Satisfies braid relations?
Markov
Markov
Invariant of links inℳ3
combine
Type ? He- cke category
Braid invariant
Satisfies braid relations?
Markov invariant
Markov 2-trace?
“HOMFLYPT polynomial”
My failure. What I would like to understand, but I do not. Artin–Tits groups come in four main flavors.
Question: Why are these special? What happens in general type?
A different idea for today:
What can Artin–Tits groups tell you about flavor two? However, this “naive” approach fails for most3-manifolds. Why? Because I do not know what Hecke/Soergel analog
to use for an arbitrary3-manifold.
Today. I explain what we can do.
braids in a3-mfdℳ3 𝒷
links in a3-mfdℳ3
Alexander’s theorem
𝒷
𝒸 𝒷
𝒸
=
extra relations for braids
Markov’s theorem
algebraic way to study
links in a3-mfdℳ3
combine
Type ? He- cke algebra
Braid invariant
Satisfies braid relations?
Markov
Markov
Invariant of links inℳ3
combine
Type ? He- cke category
Braid invariant
Satisfies braid relations?
Markov invariant
Markov 2-trace?
Invariant of links inℳ3
combine
“HOMFLYPT homology”
“HOMFLYPT polynomial”
My failure. What I would like to understand, but I do not. Artin–Tits groups come in four main flavors.
Question: Why are these special? What happens in general type?
A different idea for today:
What can Artin–Tits groups tell you about flavor two? However, this “naive” approach fails for most3-manifolds. Why? Because I do not know what Hecke/Soergel analog
to use for an arbitrary3-manifold.
Today. I explain what we can do.
braids in a3-mfdℳ3 𝒷
links in a3-mfdℳ3
Alexander’s theorem
𝒷
𝒸 𝒷
𝒸
=
extra relations for braids
Markov’s theorem
algebraic way to study
links in a3-mfdℳ3
combine
Type ? He- cke algebra
Braid invariant
Satisfies braid relations?
Markov
Markov
Invariant of links inℳ3
combine
Type ? He- cke category
Braid invariant
Satisfies braid relations?
Markov invariant
Markov 2-trace?
Invariant of links inℳ3
combine
“HOMFLYPT homology”
“HOMFLYPT polynomial”
My failure. What I would like to understand, but I do not. Artin–Tits groups come in four main flavors.
Question: Why are these special? What happens in general type?
A different idea for today:
What can Artin–Tits groups tell you about flavor two?
However, this “naive” approach fails for most3-manifolds.
Why? Because I do not know what Hecke/Soergel analog to use for an arbitrary3-manifold.
Today. I explain what we can do.
braids in a3-mfdℳ3 𝒷
links in a3-mfdℳ3
Alexander’s theorem
𝒷
𝒸 𝒷
𝒸
=
extra relations for braids
Markov’s theorem
algebraic way to study
links in a3-mfdℳ3
combine
Type ? He- cke algebra
Braid invariant
Satisfies braid relations?
Markov
Markov
Invariant of links inℳ3
combine
Type ? He- cke category
Braid invariant
Satisfies braid relations?
Markov invariant
Markov 2-trace?
Invariant of links inℳ3
combine
“HOMFLYPT homology”
“HOMFLYPT polynomial”
My failure. What I would like to understand, but I do not. Artin–Tits groups come in four main flavors.
Question: Why are these special? What happens in general type?
A different idea for today:
What can Artin–Tits groups tell you about flavor two?
However, this “naive” approach fails for most3-manifolds.
Why? Because I do not know what Hecke/Soergel analog to use for an arbitrary3-manifold.
Today. I explain what we can do.
1 Links and braids – the classical case Braid diagrams
Links in the 3-ball
2 Links and braids in handlebodies Braid diagrams
Links in handlebodies
3 Some “low-genus-coincidences”
The ball and the torus
The torus and the double torus
4 Arbitrary genus
Braid invariants – some ideas Link invariants – some ideas
LetBr(n)be the group defined as follows.
Generators. Braid generators
𝒷i!
1 1
i+1 i
i i+1
n n ... ... ...
Relations. Reidemeister braid relations,e.g.
= =
𝒷i𝒷−i1= 1 =𝒷−i1𝒷i
& =
𝒷i+1𝒷i𝒷i+1=𝒷i𝒷i+1𝒷i
Example.
“Topology in disguise”.
=
Theorem (Gauß≤1830 ? , Artin ∼1925.)
Letℬr(n)be the group of braids in a disk𝒟2×[0,1]. The map
7→
𝒟2×[0,1]
is an isomorphism of groupsBr(n)→ℬr(n).
LetBr(n)be the group defined as follows.
Generators. Braid generators
𝒷i!
1 1
i+1 i
i i+1
n n ... ... ...
Relations. Reidemeister braid relations,e.g.
= =
𝒷i𝒷−i1= 1 =𝒷−i1𝒷i
& =
𝒷i+1𝒷i𝒷i+1=𝒷i𝒷i+1𝒷i
Example.
“Topology in disguise”.
=
Theorem (Gauß≤1830 ? , Artin ∼1925.)
Letℬr(n)be the group of braids in a disk𝒟2×[0,1]. The map
7→
𝒟2×[0,1]
is an isomorphism of groupsBr(n)→ℬr(n).
LetBr(n)be the group defined as follows.
Generators. Braid generators
𝒷i!
1 1
i+1 i
i i+1
n n ... ... ...
Relations. Reidemeister braid relations,e.g.
= =
𝒷i𝒷−i1= 1 =𝒷−i1𝒷i
& =
𝒷i+1𝒷i𝒷i+1=𝒷i𝒷i+1𝒷i
Example.
“Topology in disguise”.
=
Theorem (Gauß≤1830 ? , Artin ∼1925.)
Letℬr(n)be the group of braids in a disk𝒟2×[0,1]. The map
7→
𝒟2×[0,1]
is an isomorphism of groupsBr(n)→ℬr(n).
LetBr(n)be the group defined as follows.
Generators. Braid generators
𝒷i!
1 1
i+1 i
i i+1
n n ... ... ...
Relations. Reidemeister braid relations,e.g.
= =
𝒷i𝒷−i1= 1 =𝒷−i1𝒷i
& =
𝒷i+1𝒷i𝒷i+1=𝒷i𝒷i+1𝒷i
Example.
“Topology in disguise”.
=
Theorem (Gauß≤1830 ? , Artin∼1925.)
Letℬr(n)be the group of braids in a disk𝒟2×[0,1].
The map
7→
𝒟2×[0,1]
is an isomorphism of groupsBr(n)→ℬr(n).
The Alexander closure onℬr(∞)is given by:
This is the classical Alexander closure.
Theorem (Brunn∼1897, Alexander∼1923). For any link𝓁in the3-ball𝒟3 there is a braid inℬr(∞)
whose closure is isotopic to𝓁.
Proof?
The Alexander closure onℬr(∞)is given by:
This is the classical Alexander closure.
Theorem (Brunn∼1897, Alexander∼1923).
For any link𝓁in the3-ball𝒟3 there is a braid inℬr(∞) whose closure is isotopic to𝓁.
Proof?
The Markov moves onℬr(∞)are conjugation and stabilization.
Conjugation.
... ...
... ...
𝒷 ∼
... ...
... ...
𝒷 𝒸
𝒸-1
⇔
... ...
... ...
𝒸
𝒷
∼
... ...
... ...
𝒷
𝒸
Stabilization.
n n
𝒷 𝒸
∼
n n
𝒷 𝒸
∼
n n
𝒷 𝒸
These are the classical Markov moves.
Theorem (Markov∼1936). Two links in𝒟3 are equivalent if and only if they are equal inℬr(∞)up to conjugation and stabilization.
Proof?
The upshot.
Together with Alexander’s theorem, this gives a way to algebraically study
links in𝒟3.
The Markov moves onℬr(∞)are conjugation and stabilization.
Conjugation.
... ...
... ...
𝒷 ∼
... ...
... ...
𝒷 𝒸
𝒸-1
⇔
... ...
... ...
𝒸
𝒷
∼
... ...
... ...
𝒷
𝒸
Stabilization.
n n
𝒷 𝒸
∼
n n
𝒷 𝒸
∼
n n
𝒷 𝒸
These are the classical Markov moves.
Theorem (Markov∼1936).
Two links in𝒟3 are equivalent if and only if they are equal inℬr(∞)up to conjugation and stabilization.
Proof?
The upshot.
Together with Alexander’s theorem, this gives a way to algebraically study
links in𝒟3.
The Markov moves onℬr(∞)are conjugation and stabilization.
Conjugation.
... ...
... ...
𝒷 ∼
... ...
... ...
𝒷 𝒸
𝒸-1
⇔
... ...
... ...
𝒸
𝒷
∼
... ...
... ...
𝒷
𝒸
Stabilization.
n n
𝒷 𝒸
∼
n n
𝒷 𝒸
∼
n n
𝒷 𝒸
These are the classical Markov moves.
Theorem (Markov∼1936).
Two links in𝒟3 are equivalent if and only if they are equal inℬr(∞)up to conjugation and stabilization.
Proof?
The upshot.
Together with Alexander’s theorem, this gives a way to algebraically study
links in𝒟3.
LetBr(g, n)be the group defined as follows.
Generators. Braid and twist generators
𝒷i!
1 1
g g
1 1
i+1 i
i i+1
n n
... ... ... & 𝓉i!
1 1
g g
i 1
i 1
2 2
n n ...
...
...
...
...
Relations. Reidemeister braid relations , type C relations and special relations,e.g.
=
𝒷1𝓉2𝒷1𝓉2=𝓉2𝒷1𝓉2𝒷1
& =
(𝒷1𝓉2𝒷−11 )𝓉3=𝓉3(𝒷1𝓉2𝒷−11 ) Involves three players and inverses!
Example.
The “full wrap”.
=
Fact (typeA embedding).
Br(g, n)is a subgroup of the usual braid groupℬr(g+n).
= 7→ =
A visualization exercise.
LetBr(g, n)be the group defined as follows.
Generators. Braid and twist generators
𝒷i!
1 1
g g
1 1
i+1 i
i i+1
n n
... ... ... & 𝓉i!
1 1
g g
i 1
i 1
2 2
n n ...
...
...
...
...
Relations. Reidemeister braid relations , type C relations and special relations,e.g.
=
𝒷1𝓉2𝒷1𝓉2=𝓉2𝒷1𝓉2𝒷1
& =
(𝒷1𝓉2𝒷−11 )𝓉3=𝓉3(𝒷1𝓉2𝒷−11 ) Involves three players and inverses!
Example.
The “full wrap”.
=
Fact (typeA embedding).
Br(g, n)is a subgroup of the usual braid groupℬr(g+n).
= 7→ =
A visualization exercise.
LetBr(g, n)be the group defined as follows.
Generators. Braid and twist generators
𝒷i!
1 1
g g
1 1
i+1 i
i i+1
n n
... ... ... & 𝓉i!
1 1
g g
i 1
i 1
2 2
n n ...
...
...
...
...
Relations. Reidemeister braid relations , type C relations and special relations,e.g.
=
𝒷1𝓉2𝒷1𝓉2=𝓉2𝒷1𝓉2𝒷1
& =
(𝒷1𝓉2𝒷−11 )𝓉3=𝓉3(𝒷1𝓉2𝒷−11 ) Involves three players and inverses!
Example.
The “full wrap”.
=
Fact (typeA embedding).
Br(g, n)is a subgroup of the usual braid groupℬr(g+n).
= 7→ =
A visualization exercise.
LetBr(g, n)be the group defined as follows.
Generators. Braid and twist generators
𝒷i!
1 1
g g
1 1
i+1 i
i i+1
n n
... ... ... & 𝓉i!
1 1
g g
i 1
i 1
2 2
n n ...
...
...
...
...
Relations. Reidemeister braid relations , type C relations and special relations,e.g.
=
𝒷1𝓉2𝒷1𝓉2=𝓉2𝒷1𝓉2𝒷1
& =
(𝒷1𝓉2𝒷−11 )𝓉3=𝓉3(𝒷1𝓉2𝒷−11 ) Involves three players and inverses!
Example.
The “full wrap”.
=
Fact (typeA embedding).
Br(g, n)is a subgroup of the usual braid groupℬr(g+n).
= 7→ =
A visualization exercise.
The groupℬr(g, n)of braid in ag-times punctures disk𝒟g2×[0,1]:
Two types of braidings, the usual ones and “winding around cores”,e.g.
𝒟32×[0,1]
&
𝒟32×[0,1]
Theorem (H¨aring-Oldenburg–Lambropoulou∼2002, Vershinin∼1998). The map
7→
7→
is an isomorphism of groupsBr(g, n)→ℬr(g, n). From this perspective the type A embedding
is just shrinking holes to points!
shrink
Note.
For the proof it is crucial that𝒟g2 and the boundary points of the braids• are only defined up to isotopy,e.g.
•
• 𝒟32
∼= • •
𝒟32
⇒one can always “conjugate cores to the left”. This is useful to defineℬr(g,∞).
The groupℬr(g, n)of braid in ag-times punctures disk𝒟g2×[0,1]:
Two types of braidings, the usual ones and “winding around cores”,e.g.
𝒟32×[0,1]
&
𝒟32×[0,1]
Theorem (H¨aring-Oldenburg–Lambropoulou∼2002, Vershinin∼1998).
The map
7→
7→
From this perspective the type A embedding is just shrinking holes to points!
shrink
Note.
For the proof it is crucial that𝒟g2 and the boundary points of the braids• are only defined up to isotopy,e.g.
•
• 𝒟32
∼= • •
𝒟32
⇒one can always “conjugate cores to the left”. This is useful to defineℬr(g,∞).
The groupℬr(g, n)of braid in ag-times punctures disk𝒟g2×[0,1]:
Two types of braidings, the usual ones and “winding around cores”,e.g.
𝒟32×[0,1]
&
𝒟32×[0,1]
Theorem (H¨aring-Oldenburg–Lambropoulou∼2002, Vershinin∼1998). The map
7→
7→
is an isomorphism of groupsBr(g, n)→ℬr(g, n).
From this perspective the type A embedding is just shrinking holes to points!
shrink
Note.
For the proof it is crucial that𝒟g2 and the boundary points of the braids• are only defined up to isotopy,e.g.
•
• 𝒟32
∼= • •
𝒟32
⇒one can always “conjugate cores to the left”. This is useful to defineℬr(g,∞).
The groupℬr(g, n)of braid in ag-times punctures disk𝒟g2×[0,1]:
Two types of braidings, the usual ones and “winding around cores”,e.g.
𝒟32×[0,1]
&
𝒟32×[0,1]
Theorem (H¨aring-Oldenburg–Lambropoulou∼2002, Vershinin∼1998). The map
7→
7→
is an isomorphism of groupsBr(g, n)→ℬr(g, n). From this perspective the type A embedding
is just shrinking holes to points!
shrink
Note.
For the proof it is crucial that𝒟g2 and the boundary points of the braids• are only defined up to isotopy,e.g.
•
• 𝒟32
∼= • •
𝒟32
⇒one can always “conjugate cores to the left”.
This is useful to defineℬr(g,∞).
The Alexander closure onℬr(g,∞)is given by merging core strands at infinity.
wrong closure correct closure
This is different from the classical Alexander closure.
Theorem (Lambropoulou∼1993).
For any link𝓁in the genusghandlebodyℋg there is a braid inℬr(g,∞)whose (correct!) closure is isotopic to𝓁.
Proof? L-move. Fact.
ℋg is given by a complement in the3-sphere𝒮3 by an open tubular neighborhood of the embedded graph obtained
by gluingg+ 1unknotted “core” edges to two vertices.
𝒮3
the3-ballℋ0=𝒟3
𝒮3
a torusℋ1
𝒮3
ℋ2
The Alexander closure onℬr(g,∞)is given by merging core strands at infinity.
wrong closure correct closure
This is different from the classical Alexander closure.
Theorem (Lambropoulou∼1993).
For any link𝓁in the genusghandlebodyℋg there is a braid inℬr(g,∞)whose (correct!) closure is isotopic to𝓁.
Proof? L-move.
Fact.
ℋg is given by a complement in the3-sphere𝒮3 by an open tubular neighborhood of the embedded graph obtained
by gluingg+ 1unknotted “core” edges to two vertices.
𝒮3
the3-ballℋ0=𝒟3
𝒮3
a torusℋ1
𝒮3
ℋ2
The Alexander closure onℬr(g,∞)is given by merging core strands at infinity.
wrong closure correct closure
This is different from the classical Alexander closure.
Theorem (Lambropoulou∼1993).
For any link𝓁in the genusghandlebodyℋg there is a braid inℬr(g,∞)whose (correct!) closure is isotopic to𝓁.
Proof? L-move.
Fact.
ℋg is given by a complement in the3-sphere𝒮3 by an open tubular neighborhood of the embedded graph obtained
by gluingg+ 1unknotted “core” edges to two vertices.
𝒮3 𝒮3 𝒮3
The Markov moves onℬr(g,∞)are conjugation and stabilization.
Conjugation.
𝒷∼𝓈𝒷𝓈−1
for𝒷∈ℬr(g, n),𝓈∈ h𝒷1, . . . ,𝒷n−1i ⇐⇒
... ...
n
... ...
n
𝒷 ∼
...
...
n ...
...
n
𝒷 𝓈
𝓈-1
Stabilization.
(𝒸↑)𝒷n(𝒷↑)
∼𝒸𝒷∼(𝒸↑)𝒷−n1(𝒷↑) for𝒷,𝒸∈ℬr(g, n),
⇐⇒
n n
𝒷 𝒸
∼
n n
𝒷 𝒸
∼
n n
𝒷 𝒸
They are weaker than the classical Markov moves.
Theorem (H¨aring-Oldenburg–Lambropoulou∼2002). Two links inℋg are equivalent if and only if
they are equal inℬr(g,∞)up to conjugation and stabilization. Proof? L-move.
Example.
𝒷
wrong closure
𝒷
correct closure
not stuck stuck
The upshot.
Together with Alexander’s theorem, this gives a way to algebraically study
links inℋg.
Let me explain what we can do.
The Markov moves onℬr(g,∞)are conjugation and stabilization.
Conjugation.
𝒷∼𝓈𝒷𝓈−1
for𝒷∈ℬr(g, n),𝓈∈ h𝒷1, . . . ,𝒷n−1i ⇐⇒
... ...
n
... ...
n
𝒷 ∼
...
...
n ...
...
n
𝒷 𝓈
𝓈-1
Stabilization.
(𝒸↑)𝒷n(𝒷↑)
∼𝒸𝒷∼(𝒸↑)𝒷−n1(𝒷↑) for𝒷,𝒸∈ℬr(g, n),
⇐⇒
n n
𝒷 𝒸
∼
n n
𝒷 𝒸
∼
n n
𝒷 𝒸
They are weaker than the classical Markov moves.
Theorem (H¨aring-Oldenburg–Lambropoulou∼2002).
Two links inℋg are equivalent if and only if
they are equal inℬr(g,∞)up to conjugation and stabilization.
Proof? L-move.
Example.
𝒷
wrong closure
𝒷
correct closure
not stuck stuck
The upshot.
Together with Alexander’s theorem, this gives a way to algebraically study
links inℋg.
Let me explain what we can do.
The Markov moves onℬr(g,∞)are conjugation and stabilization.
Conjugation.
𝒷∼𝓈𝒷𝓈−1
for𝒷∈ℬr(g, n),𝓈∈ h𝒷1, . . . ,𝒷n−1i ⇐⇒
... ...
n
... ...
n
𝒷 ∼
...
...
n ...
...
n
𝒷 𝓈
𝓈-1
Stabilization.
(𝒸↑)𝒷n(𝒷↑)
∼𝒸𝒷∼(𝒸↑)𝒷−n1(𝒷↑) for𝒷,𝒸∈ℬr(g, n),
⇐⇒
n n
𝒷 𝒸
∼
n n
𝒷 𝒸
∼
n n
𝒷 𝒸
They are weaker than the classical Markov moves.
Theorem (H¨aring-Oldenburg–Lambropoulou∼2002).
Two links inℋg are equivalent if and only if
they are equal inℬr(g,∞)up to conjugation and stabilization.
Proof? L-move.
Example.
𝒷
wrong closure
𝒷
correct closure
The upshot.
Together with Alexander’s theorem, this gives a way to algebraically study
links inℋg.
Let me explain what we can do.
The Markov moves onℬr(g,∞)are conjugation and stabilization.
Conjugation.
𝒷∼𝓈𝒷𝓈−1
for𝒷∈ℬr(g, n),𝓈∈ h𝒷1, . . . ,𝒷n−1i ⇐⇒
... ...
n
... ...
n
𝒷 ∼
...
...
n ...
...
n
𝒷 𝓈
𝓈-1
Stabilization.
(𝒸↑)𝒷n(𝒷↑)
∼𝒸𝒷∼(𝒸↑)𝒷−n1(𝒷↑) for𝒷,𝒸∈ℬr(g, n),
⇐⇒
n n
𝒷 𝒸
∼
n n
𝒷 𝒸
∼
n n
𝒷 𝒸
They are weaker than the classical Markov moves.
Theorem (H¨aring-Oldenburg–Lambropoulou∼2002). Two links inℋg are equivalent if and only if
they are equal inℬr(g,∞)up to conjugation and stabilization. Proof? L-move.
Example.
𝒷
wrong closure
𝒷
correct closure
not stuck stuck
The upshot.
Together with Alexander’s theorem, this gives a way to algebraically study
links inℋg.
Let me explain what we can do.
The Markov moves onℬr(g,∞)are conjugation and stabilization.
Conjugation.
𝒷∼𝓈𝒷𝓈−1
for𝒷∈ℬr(g, n),𝓈∈ h𝒷1, . . . ,𝒷n−1i ⇐⇒
... ...
n
... ...
n
𝒷 ∼
...
...
n ...
...
n
𝒷 𝓈
𝓈-1
Stabilization.
(𝒸↑)𝒷n(𝒷↑)
∼𝒸𝒷∼(𝒸↑)𝒷−n1(𝒷↑) for𝒷,𝒸∈ℬr(g, n),
⇐⇒
n n
𝒷 𝒸
∼
n n
𝒷 𝒸
∼
n n
𝒷 𝒸
They are weaker than the classical Markov moves.
Theorem (H¨aring-Oldenburg–Lambropoulou∼2002). Two links inℋg are equivalent if and only if
they are equal inℬr(g,∞)up to conjugation and stabilization. Proof? L-move.
Example.
𝒷
wrong closure
𝒷
correct closure
not stuck stuck
The upshot.
Together with Alexander’s theorem, this gives a way to algebraically study
links inℋg.
Let me explain what we can do.