geometric topology
Knot Theory
You should know: fundamental group, manifolds
Overview
Knot theory is the mathematical study of knots — closed curves embedded in three-dimensional space — and their properties up to continuous deformation (ambient isotopy). The central problem is to determine when two knots are equivalent. This is addressed through knot invariants: algebraic or polynomial quantities that do not change under deformation. Knot theory has applications to DNA topology, quantum field theory, and the study of 3-manifolds.
Intuition
A knot is a closed loop in 3-space that may or may not be untangleable into a simple circle (the unknot). Two knots are equivalent if one can be continuously deformed into the other without cutting. To tell knots apart, we compute invariants. The fundamental group of the knot complement is a powerful invariant; polynomial invariants (Alexander, Jones, HOMFLY) give computable algebraic fingerprints. Reidemeister moves provide the combinatorial calculus for knot diagrams.
Formal Definition
A knot is a smooth embedding of S^1 into R^3 (or S^3), considered up to ambient isotopy. A link is a disjoint union of knots.
Notation
| Notation | Meaning |
|---|---|
| A knot (smooth embedding of S^1 in R^3) | |
| Alexander polynomial of knot K | |
| Jones polynomial of knot K | |
| Knot group |
Theorems
Worked Examples
- 1
RI: Add or remove a simple twist (a curl) in a strand. This does not change the topology of the knot.
- 2
RII: Pass two strands over each other, creating or cancelling two crossings of opposite sign.
- 3
RIII: Slide a strand over a crossing. This moves a strand past a crossing without changing connectivity.
✓ Answer
Each Reidemeister move corresponds to a local ambient isotopy of R^3, so it does not change the knot type.
Practice Problems
Show that the trefoil knot is not equivalent to the unknot using the Alexander polynomial.
What is the knot group of the trefoil, and why is it not abelian?
Common Mistakes
Thinking knot equivalence is just homeomorphism of the knot itself
Two knots are equivalent under ambient isotopy: a deformation of the entire surrounding space R^3. The knot itself (as a circle) is always homeomorphic to S^1; the embedding in 3-space is what matters.
Assuming the knot group completely classifies knots
The knot group does not distinguish all knots. For example, a knot and its mirror image have isomorphic groups in some cases. However, the knot group determines the knot for prime knots by Gordon-Luecke.
Quiz
Historical Background
Lord Kelvin's 19th-century vortex atom theory motivated Peter Guthrie Tait to begin systematic tabulation of knots. The mathematical theory developed through the work of Alexander (who introduced the Alexander polynomial in 1928), Conway (skein relations, 1969), and Jones (the Jones polynomial, 1984). The Jones polynomial sparked connections to quantum field theory and led to a revolution in knot invariants.
- 1867
Tait begins tabulating knots inspired by Kelvin's vortex atom theory
Peter Guthrie Tait
- 1928
Alexander introduces the Alexander polynomial, the first polynomial knot invariant
James W. Alexander
- 1969
Conway introduces skein relations for computing knot polynomials
John Conway
- 1984
Jones discovers the Jones polynomial, winning the Fields Medal
Vaughan Jones
- 1988
Witten interprets the Jones polynomial via quantum Chern-Simons theory
Edward Witten
Summary
- A knot is a smooth embedding of S^1 into R^3, studied up to ambient isotopy.
- Reidemeister's theorem reduces knot equivalence to three local moves on diagrams.
- Knot invariants include the knot group, Alexander polynomial, and Jones polynomial.
- The trefoil is the simplest non-trivial knot; the Hopf link is the simplest non-trivial link.
- The Jones polynomial connects knot theory to quantum field theory via Chern-Simons theory.
References
- BookAdams, C. — The Knot Book (2004), American Mathematical Society
- WebsiteWikipedia — Knot theory
- WebsiteMathWorld — Knot Theory
- WebsitenLab — knot theory
Mathematics