Trefoil knot
From Wikipedia, the free encyclopedia
In knot theory, the trefoil knot is the simplest nontrivial knot.
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- It can be obtained by joining the loose ends of an overhand knot.
- It can be described as a (2,3)-torus knot.
- It is the closure of the braid σ13.
- It is the intersection of the unit 3-sphere S3 in C2 with the complex plane curve (a cuspidal cubic) of zeroes of the complex polynomial z2 + w3.
- It is the unique prime knot with three crossings.
- It is chiral, meaning it is not equivalent to its mirror image.
- It is alternating.
- It is not a slice knot, meaning that it does not bound a smooth 2-dimensional disk in the 4-dimensional ball; one way to prove this is to note that its signature is not zero.
- It is a fibered knot, meaning that its complement in S3 is a fiber bundle over the circle S1. In the model of the trefoil as the set of pairs (z,w) of complex numbers such that | z | 2 + | w | 2 = 1 and z2 + w3 = 0, this fiber bundle has the Milnor map φ(z,w) = (z2 + w3) / | z2 + w3 | as its fibration, and a once-punctured torus as its fiber surface.
- Its Alexander polynomial is t2 − t + 1.
- Its Jones polynomial is t + t3 − t4.
- Its knot group is isomorphic to B3, the braid group on 3 strands, which has presentation
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- Rolfsen, Dale (1976). Knots and links. Berkeley: Publish or Perish, Inc. ISBN 0-914098-16-0.
- Eric W. Weisstein, Trefoil Knot at MathWorld.
