Lissajous knot

Source: Wikipedia, the free encyclopedia.

In

parametric equations
of the form

A Lissajous 821 knot

where , , and are

phase shifts
, , and may be any real numbers.[1]

The projection of a Lissajous knot onto any of the three coordinate planes is a Lissajous curve, and many of the properties of these knots are closely related to properties of Lissajous curves.

Replacing the cosine function in the parametrization by a triangle wave transforms every Lissajous knot isotopically into a billiard curve inside a cube, the simplest case of so-called billiard knots. Billiard knots can also be studied in other domains, for instance in a cylinder[2] or in a (flat) solid torus (Lissajous-toric knot).

Form

Because a knot cannot be self-intersecting, the three integers must be pairwise

relatively prime
, and none of the quantities

may be an integer multiple of pi. Moreover, by making a substitution of the form , one may assume that any of the three phase shifts , , is equal to zero.

Examples

Here are some examples of Lissajous knots,[3] all of which have :

  • Three-twist knot '"`UNIQ--postMath-0000000F-QINU`"' '"`UNIQ--postMath-00000010-QINU`"'
    Three-twist knot

  • Stevedore knot '"`UNIQ--postMath-00000011-QINU`"' '"`UNIQ--postMath-00000012-QINU`"'
    Stevedore knot

  • Square knot '"`UNIQ--postMath-00000013-QINU`"' '"`UNIQ--postMath-00000014-QINU`"'
    Square knot

  • 821 knot '"`UNIQ--postMath-00000015-QINU`"' '"`UNIQ--postMath-00000016-QINU`"'
    821 knot

There are infinitely many different Lissajous knots,[4] and other examples with 10 or fewer crossings include the 74 knot, the 815 knot, the 101 knot, the 1035 knot, the 1058 knot, and the composite knot 52* # 52,[1] as well as the 916 knot, 1076 knot, the 1099 knot, the 10122 knot, the 10144 knot, the granny knot, and the composite knot 52 # 52.[5] In addition, it is known that every twist knot with Arf invariant zero is a Lissajous knot.[6]

Symmetry

Lissajous knots are highly symmetric, though the type of symmetry depends on whether or not the numbers , , and are all odd.

Odd case

If , , and are all odd, then the point reflection across the origin is a symmetry of the Lissajous knot which preserves the knot orientation.

In general, a knot that has an orientation-preserving point reflection symmetry is known as strongly plus

amphicheiral.[7] This is a fairly rare property: only seven or eight prime knots with twelve or fewer crossings are strongly plus amphicheiral (1099, 10123, 12a427, 12a1019, 12a1105, 12a1202, 12n706).[8]
Since this is so rare, ′most′ prime Lissajous knots lie in the even case.

Even case

If one of the frequencies (say ) is even, then the 180° rotation around the x-axis is a symmetry of the Lissajous knot. In general, a knot that has a symmetry of this type is called 2-periodic, so every even Lissajous knot must be 2-periodic.

Consequences

A Lissajous knot with three factors: ,

The symmetry of a Lissajous knot puts severe constraints on the Alexander polynomial. In the odd case, the Alexander polynomial of the Lissajous knot must be a perfect square.[9] In the even case, the Alexander polynomial must be a perfect square modulo 2.[10] In addition, the Arf invariant of a Lissajous knot must be zero. It follows that:

References