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Trefoil knot

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Trefoil
Common nameOverhand knot
Arf invariant1
Braid length3
Braid no.2
Bridge no.2
Crosscap no.1
Crossing no.3
Genus1
Hyperbolic volume0
Stick no.6
Tunnel no.1
Unknotting no.1
Conway notation[3]
A–B notation31
Dowker notation4, 6, 2
Last / Next0141
Other
alternating, torus, fibered, pretzel, prime, knot slice, reversible, tricolorable, twist

In knot theory, a branch of mathematics, the trefoil knot is the simplest example of a nontrivial knot. The trefoil can be obtained by joining the two loose ends of a common overhand knot, resulting in a knotted loop. As the simplest knot, the trefoil is fundamental to the study of mathematical knot theory.

The trefoil knot is named after the three-leaf clover (or trefoil) plant.

Descriptions

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The trefoil knot can be defined as the curve obtained from the following parametric equations:

The (2,3)-torus knot is also a trefoil knot. The following parametric equations give a (2,3)-torus knot lying on torus :

Video on making a trefoil knot
Overhand knot becomes a trefoil knot by joining the ends.
A realization of the trefoil knot figure

Any continuous deformation of the curve above is also considered a trefoil knot. Specifically, any curve isotopic to a trefoil knot is also considered to be a trefoil. In addition, the mirror image of a trefoil knot is also considered to be a trefoil. In topology and knot theory, the trefoil is usually defined using a knot diagram instead of an explicit parametric equation.

In algebraic geometry, the trefoil can also be obtained as the intersection in C2 of the unit 3-sphere S3 with the complex plane curve of zeroes of the complex polynomial z2 + w3 (a cuspidal cubic).

Left-handed trefoil
Right-handed trefoil
A left-handed trefoil and a right-handed trefoil

If one end of a tape or belt is turned over three times and then pasted to the other, the edge forms a trefoil knot.[1]

Symmetry

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The trefoil knot is chiral, in the sense that a trefoil knot can be distinguished from its own mirror image. The two resulting variants are known as the left-handed trefoil and the right-handed trefoil. It is not possible to deform a left-handed trefoil continuously into a right-handed trefoil, or vice versa. (That is, the two trefoils are not ambient isotopic.)

Though chiral, the trefoil knot is also invertible, meaning that there is no distinction between a counterclockwise-oriented and a clockwise-oriented trefoil. That is, the chirality of a trefoil depends only on the over and under crossings, not the orientation of the curve.

But the knot has rotational symmetry. The axis is about a line perpendicular to the page for the 3-coloured image.

The trefoil knot is tricolorable.
Form of trefoil knot without visual three-fold symmetry

Nontriviality

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The trefoil knot is nontrivial, meaning that it is not possible to "untie" a trefoil knot in three dimensions without cutting it. Mathematically, this means that a trefoil knot is not isotopic to the unknot. In particular, there is no sequence of Reidemeister moves that will untie a trefoil.

Proving this requires the construction of a knot invariant that distinguishes the trefoil from the unknot. The simplest such invariant is tricolorability: the trefoil is tricolorable, but the unknot is not. In addition, virtually every major knot polynomial distinguishes the trefoil from an unknot, as do most other strong knot invariants.

Classification

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In knot theory, the trefoil is the first nontrivial knot, and is the only knot with crossing number three. It is a prime knot, and is listed as 31 in the Alexander-Briggs notation. The Dowker notation for the trefoil is 4 6 2, and the Conway notation is [3].

The trefoil can be described as the (2,3)-torus knot. It is also the knot obtained by closing the braid σ13.

The trefoil is an alternating knot. However, it is not a slice knot, meaning 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. Another proof is that its Alexander polynomial does not satisfy the Fox-Milnor condition.

The trefoil is a fibered knot, meaning that its complement in is a fiber bundle over the circle . The trefoil K may be viewed as the set of pairs of complex numbers such that and . Then this fiber bundle has the Milnor map as the fibre bundle projection of the knot complement to the circle . The fibre is a once-punctured torus. Since the knot complement is also a Seifert fibred with boundary, it has a horizontal incompressible surface—this is also the fiber of the Milnor map. (This assumes the knot has been thickened to become a solid torus Nε(K), and that the interior of this solid torus has been removed to create a compact knot complement .)

Invariants

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The Alexander polynomial of the trefoil knot issince is a possible Seifert matrix (for the left-hand one), or because of its Conway polynomial,[2] which isThe Jones polynomial isand the Kauffman polynomial of the trefoil isThe HOMFLY polynomial of the trefoil is

The knot group of the trefoil is given by the presentationor equivalently[3]This group is isomorphic to the braid group with three strands.

In religion and culture

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As the simplest nontrivial knot, the trefoil is a common motif in iconography and the visual arts. For example, the common form of the triquetra symbol is a trefoil, as are some versions of the Germanic Valknut.

In modern art, the woodcut Knots by M. C. Escher (1965) depicts three trefoil knots whose solid forms are twisted in different ways.[4]

See also

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References

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  1. ^ Shaw, George Russell (MCMXXXIII). Knots: Useful & Ornamental, p.11. ISBN 978-0-517-46000-9.
  2. ^ "3_1", The Knot Atlas.
  3. ^ Weisstein, Eric W. "Trefoil Knot". MathWorld. by Wolfram. Accessed: May 5, 2013.
  4. ^ The Official M.C. Escher Website — Gallery — "Knots" www.mcescher.com In black/green/brown via 3 woodcuts. Catalogue nr 444. The Hague, Municipal Museum (1981).
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Category:Topology