🧮 Brain Teaser

The Torus Knot Group: When Two Loops Cannot Be Separated

Let T=S1×S1T = S^1 \times S^1 be the torus. Consider the two standard loops:

  • aa: the meridian (goes around the "small" circle once)
  • bb: the longitude (goes around the "large" circle once)

We know π1(T)≅Z×Z\pi_1(T) \cong \mathbb{Z} \times \mathbb{Z}, generated by [a][a] and [b][b].

Now consider the loop γ\gamma on the torus that wraps pp times in the aa-direction and qq times in the bb-direction, where gcd⁡(p,q)=1\gcd(p,q) = 1.

Question: Show that γ\gamma is a simple closed curve on TT (it doesn't self-intersect), and that cutting the torus along γ\gamma produces an annulus (a cylinder), not two separate pieces.

As a follow-up: what is the fundamental group of the complement T∖γT \setminus \gamma?

fundamental grouptoruscovering spacesBézoutsimple closed curvecut-and-paste topology

Answer: Torus Knot Curve: Simple Closed Curve and Annular Complement

Key Idea / Intuition

Think of the torus as a square [0,1]2[0,1]^2 with opposite sides identified. The curve γ\gamma becomes a straight line of slope q/pq/p in the square — and because gcd⁡(p,q)=1\gcd(p,q)=1, this line hits exactly the right lattice points to close up into a single embedded loop without self-intersection. When you "cut" the torus along this line, you're unzipping the identification along a diagonal, and what's left is topologically an annulus. The fundamental group of an annulus is Z\mathbb{Z}.


Formal Proof / Solution

Step 1: Visualizing γ\gamma in the Square Model

Represent TT as R2/Z2\mathbb{R}^2 / \mathbb{Z}^2, i.e., the unit square [0,1]2[0,1]^2 with (x,0)∼(x,1)(x,0)\sim(x,1) and (0,y)∼(1,y)(0,y)\sim(1,y).

The curve γ\gamma lifts to the straight line ℓ\ell in R2\mathbb{R}^2 starting at (0,0)(0,0) with direction vector (p,q)(p,q): γ~(t)=(pt, qt),t∈[0,1].\tilde{\gamma}(t) = (pt,\, qt), \quad t \in [0,1].

At t=1t=1 we reach (p,q)(p,q), which maps to (0,0)(0,0) in TT (since both coordinates are integers), so γ\gamma is indeed a closed loop representing [a]p[b]q=p[a]+q[b][a]^p[b]^q = p[a]+q[b] in π1(T)\pi_1(T).

Step 2: γ\gamma Is Simple (No Self-Intersections)

Suppose γ(t1)=γ(t2)\gamma(t_1) = \gamma(t_2) for t1≠t2t_1 \neq t_2 in [0,1)[0,1). Then γ~(t1)≡γ~(t2)(modZ2),\tilde{\gamma}(t_1) \equiv \tilde{\gamma}(t_2) \pmod{\mathbb{Z}^2}, meaning (p(t1−t2), q(t1−t2))∈Z2(p(t_1-t_2),\, q(t_1-t_2)) \in \mathbb{Z}^2.

So p(t1−t2)=mp(t_1-t_2) = m and q(t1−t2)=nq(t_1-t_2) = n for integers m,nm,n. Then: t1−t2=mp=nq  ⟹  mq=np.t_1 - t_2 = \frac{m}{p} = \frac{n}{q} \implies mq = np.

Since gcd⁡(p,q)=1\gcd(p,q)=1, we get p∣mp \mid m and q∣nq \mid n, so t1−t2∈Zt_1 - t_2 \in \mathbb{Z}. But t1,t2∈[0,1)t_1, t_2 \in [0,1) means t1=t2t_1 = t_2. Contradiction. Hence γ\gamma is simple.

Step 3: Cutting Along γ\gamma Gives an Annulus

Since gcd⁡(p,q)=1\gcd(p,q)=1, by Bézout's theorem there exist integers r,sr, s with ps−qr=1ps - qr = 1.

Define a new basis for the lattice Z2\mathbb{Z}^2: u=(p,q),v=(r,s).\mathbf{u} = (p,q), \quad \mathbf{v} = (r,s).

The matrix (prqs)\begin{pmatrix} p & r \\ q & s \end{pmatrix} has determinant ps−qr=1ps - qr = 1, so it's in SL2(Z)\text{SL}_2(\mathbb{Z}): it's a lattice automorphism of R2/Z2\mathbb{R}^2/\mathbb{Z}^2.

In the new coordinates (u,v)(u,v) (where the uu-direction corresponds to γ\gamma), the torus looks like the parallelogram spanned by u\mathbf{u} and v\mathbf{v}, identified on opposite sides. The curve γ\gamma is the segment from (0,0)(0,0) to (1,0)(1,0) in the uu-coordinate.

Cutting along γ\gamma means cutting the square [0,1]2[0,1]^2 (in new coordinates) along the edge v=0v=0 (which, after identification, is exactly γ\gamma). This gives:

  • A square [0,1]2[0,1]^2 where the top and bottom are no longer identified (they were the two sides of γ\gamma), but the left and right are still identified.
  • That's exactly [0,1]×[0,1][0,1] \times [0,1] with (0,v)∼(1,v)(0,v) \sim (1,v), which is a cylinder = annulus.

Step 4: Fundamental Group of T∖γT \setminus \gamma

The complement T∖γT \setminus \gamma is an open annulus (the torus cut open along the simple closed curve γ\gamma). An open annulus deformation retracts onto its core circle S1S^1, so:

π1(T∖γ)≅Z.\boxed{\pi_1(T \setminus \gamma) \cong \mathbb{Z}.}

The generator is any loop that "links" γ\gamma once — in coordinates, it's the loop in the vv-direction (Bézout complement direction).

Why gcd⁡(p,q)=1\gcd(p,q)=1 Is Essential

If gcd⁡(p,q)=d>1\gcd(p,q) = d > 1, then the "line" in the square would close up after time 1/d1/d, tracing the same path dd times — so γ\gamma would self-intersect (or rather, be a dd-fold cover of a simpler curve). The complement would then have a more complicated topology.

Source: Topology (Munkres); Introduction to Topological Manifolds (John M. Lee) — folklore/classical

Type: topologySource: Topology (Munkres); Introduction to Topological Manifolds (John M. Lee) — folklore/classicalEdit on GitHub ↗