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In knot theory, a Lissajous knot is a knot defined by parametric equations of the form

$x=\cos(n_{x}t+\phi _{x}),\qquad y=\cos(n_{y}t+\phi _{y}),\qquad z=\cos(n_{z}t+\phi _{z}),$

A Lissajous 8₂₁ knot

where $n_{x}$, $n_{y}$, and $n_{z}$ are integers and the phase shifts $\phi _{x}$, $\phi _{y}$, and $\phi _{z}$ may be any real numbers.

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.

Form

Because a knot cannot be self-intersecting, the three integers $n_{x},n_{y},n_{z}$ must be pairwise relatively prime, and none of the quantities

$n_{x}\phi _{y}-n_{y}\phi _{x},\quad n_{y}\phi _{z}-n_{z}\phi _{y},\quad n_{z}\phi _{x}-n_{x}\phi _{z}$

may be an integer multiple of pi. Moreover, by making a substitution of the form $t'=t+c$, one may assume that any of the three phase shifts $\phi _{x}$, $\phi _{y}$, $\phi _{z}$ is equal to zero.

Examples

Here are some examples of Lissajous knots, all of which have $\phi _{z}=0$:

• 

  Three-twist knot
  $(n_{x},n_{y},n_{z})=(3,2,7)$
  $(\phi _{x},\phi _{y})=(0.7,0.2)$

• 

  Stevedore knot
  $(n_{x},n_{y},n_{z})=(3,2,5)$
  $(\phi _{x},\phi _{y})=(1.5,0.2)$

• 

  Square knot
  $(n_{x},n_{y},n_{z})=(3,5,7)$
  $(\phi _{x},\phi _{y})=(0.7,1.0)$

• 

  8₂₁ knot
  $(n_{x},n_{y},n_{z})=(3,4,7)$
  $(\phi _{x},\phi _{y})=(0.1,0.7)$

There are infinitely many different Lissajous knots, 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, 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. In addition, it is known that every twist knot with Arf invariant zero is a Lissajous knot.

Symmetry

Lissajous knots are highly symmetric, though the type of symmetry depends on whether or not the numbers $n_{x}$, $n_{y}$, and $n_{z}$ are all odd.

Odd case

If $n_{x}$, $n_{y}$, and $n_{z}$ are all odd, then the point reflection across the origin $(x,y,z)\mapsto (-x,-y,-z)$ 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. This is a fairly rare property: only three prime knots with twelve or fewer crossings are strongly plus amphicheiral prime knot, the first of which has crossing number ten. Since this is so rare, most Lissajous knots lie in the even case.

Even case

If one of the frequencies (say $n_{x}$) is even, then the 180° rotation around the x-axis $(x,y,z)\mapsto (x,-y,-z)$ 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

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. In the even case, the Alexander polynomial must be a perfect square modulo 2. In addition, the Arf invariant of a Lissajous knot must be zero. It follows that:

• The trefoil knot and figure-eight knot are not Lissajous.
• No torus knot can be Lissajous.
• No fibered 2-bridge knot can be Lissajous.

References

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