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A Distance for Circular Heegaard Splittings

Kevin Lamb, Patrick Weed

Abstract

For a knot $K\subset S^3$, its exterior $E(K) = S^3\backslashη(K)$ has a singular foliation by Seifert surfaces of $K$ derived from a circle-valued Morse function $f\colon E(K)\to S^1$. When $f$ is self-indexing and has no critical points of index 0 or 3, the regular levels that separate the index-1 and index-2 critical points decompose $E(K)$ into a pair of compression bodies. We call such a decomposition a circular Heegaard splitting of $E(K)$. We define the notion of circular distance (similar to Hempel distance) for this class of Heegaard splitting and show that it can be bounded under certain circumstances. Specifically, if the circular distance of a circular Heegaard splitting is too large: (1) $E(K)$ can't contain low-genus incompressible surfaces, and (2) a minimal-genus Seifert surface for $K$ is unique up to isotopy.

A Distance for Circular Heegaard Splittings

Abstract

For a knot , its exterior has a singular foliation by Seifert surfaces of derived from a circle-valued Morse function . When is self-indexing and has no critical points of index 0 or 3, the regular levels that separate the index-1 and index-2 critical points decompose into a pair of compression bodies. We call such a decomposition a circular Heegaard splitting of . We define the notion of circular distance (similar to Hempel distance) for this class of Heegaard splitting and show that it can be bounded under certain circumstances. Specifically, if the circular distance of a circular Heegaard splitting is too large: (1) can't contain low-genus incompressible surfaces, and (2) a minimal-genus Seifert surface for is unique up to isotopy.

Paper Structure

This paper contains 18 sections, 24 theorems, 20 equations, 14 figures.

Key Result

Theorem 2.1

For any knot $K\subset S^3$, $\pi_n(E(K))$ is trivial for $n\geq2$.

Figures (14)

  • Figure 1: A compression of the surface $F$ via the compressing disk $D$.
  • Figure 2: A $\partial$-compression of the surface $F$ via the compressing disk $D$.
  • Figure 3: Using the cores of 1-handles to define a spine of a 3-dimensional handlebody.
  • Figure 4: The four types of 3-dimensional handles and their attaching regions (in red).
  • Figure 5: A handlebody $H$ and a compression body $W$ with representative spines for each.
  • ...and 9 more figures

Theorems & Definitions (53)

  • Theorem 2.1: Asphericity
  • Theorem 2.2: cf. Jaco
  • Theorem 2.3: ScTom
  • Definition 2.1
  • Definition 2.2
  • Definition 2.3
  • Theorem 2.4: Fab
  • Theorem 2.5: Fab
  • Definition 2.4
  • Definition 2.5
  • ...and 43 more