In mathematics, a Seifert surface is a surface whose boundary is a given knot or link. Such surfaces can be used to study the properties of the associated knot or link. For example, many knot invariants are most easily calculated using a Seifert surface. Seifert surfaces are also interesting in their own right, and the subject of considerable research.
Specifically, let L be a tame oriented knot or link in Euclidean 3-space (or in the 3-sphere). A Seifert surface is a compact, connected, oriented surface S embedded in 3-space whose boundary is L such that the orientation on L is just the induced orientation from S, and every connected component of S has non-empty boundary.
Note that any compact, connected, oriented surface with nonempty boundary in Euclidean 3-space is the Seifert surface associated to its boundary link. A single knot or link can have many different inequivalent Seifert surfaces. It is important to note that a Seifert surface must be oriented. It is possible to associate unoriented (and not necessarily orientable) surfaces to knots as well.
The "checkerboard" coloring of the minimal crossing projection of the trefoil knot gives a Mobius strip with three half twists. As with the previous example, this is not a Seifert surface as it is not orientable. Applying Seifert's algorithm to this diagram, as expected, does produce a Seifert surface; in this case, it is a punctured torus of genus g=1, and the Seifert matrix is
| A = |
|
It is a theorem that there always exists a Seifert surface. This theorem was first published by F. Frankl and Lev Pontrjagin in 1930. A different proof was published in 1934 by Herbert Seifert and relies on what is now called the Seifert algorithm. The algorithm produces a Seifert surface , given a projection of the knot or link in question. Suppose that link has m components (m=1 for a knot), the diagram has d crossing points, and resolving the crossings yields f circles. Then the surface is constructed from f disjoint disks by attaching d bands. The homology group is free abelian on 2g generators, where g=(2+d-f-m)/2 is the genus of . The 2g2g integer Seifert matrix A of the linking numbers of 2g linearly independent cycles generating has entry the linking number in Euclidean 3-space (or in the 3-sphere) of the ith cycle and the pushoff of the jth cycle out of the surface. The Alexander polynomial may now be computed from the Seifert matrix.
One example of a knot invariant which is computed from a Seifert surface is the genus of a knot. The genus of a knot K is defined as minimal genus g of all Seifert surfaces for K.
For instance:
A fundamental property of the genus is that it is additive with respect to the knot sum:
Every knot K in 3-space bounds a compact, connected non-orientable surface of genus . The minimum of such is called the Crosscap Number or non-orientable genus of K.
For instance:
The formula for the knot sum is
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