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Torus-knot exterior group and peripheral system

Statement

Assume the full Axiom of Choice. Let p,q be coprime nonzero integers, let K=T(p,q) be the oriented primitive slope curve in the standard Heegaard torus, and let ρt(z1,z2)=(e2πiptz1,e2πiqtz2) be the weighted circle action on the unit S3⊂C2. Choose N(K) to be a sufficiently small closed metric tube around the orbit K for the round metric; this tube is invariant because ρt is isometric and preserves K. Set EK=S3∖int⁡N(K). Let x and y be based generators of the fundamental groups of the two solid-torus pieces obtained by cutting EK along the annulus left on the Heegaard torus, oriented so that the annulus core maps to xp and yq. Then

π1(EK)=⟨x,y∣xp=yq⟩.

The common element h=xp=yq is central and represents a regular fiber of a Seifert fibration of EK over a disk. The fibration has two distinguished core fibers of multiplicities ∣p∣ and ∣q∣; a fiber of multiplicity one is regular, and a fiber of multiplicity greater than one is exceptional. Thus there are exactly two exceptional fibers when ∣p∣,∣q∣>1, and one is regular when one absolute parameter is 1.

For any integers α,β with pα+qβ=1, compatible based paths identify the positive normal-disk meridian and preferred longitude in the peripheral system as

μ=yαxβ,λ=hμ−pq.

Here the positive meridian is the oriented boundary of a normal disk, and the preferred longitude has degree one around K and maps to zero in H1(EK;Z). Their homology classes form a basis of H1(∂EK;Z), so both classes are primitive.

Facts & Assumptions

Given: Full AC, coprime nonzero integers p,q, the chosen knot exterior and based paths, and the specified Heegaard torus.

[A1]

Full AC is the axiom that every family of nonempty sets has a choice function (The Axiom of Choice).

[L1]

Full AC implies the Axiom of Countable Choice, which is the hypothesis of the exterior and peripheral-system definitions (AC implies DC implies countable choice, The Axiom of Countable Choice (ACω)).

[F1]

Coprime torus knot identifies K with the oriented primitive slope pα+qβ on the standard unknotted Heegaard torus.

[F2]

Knot exterior sets EK=S3∖int⁡N(K) with its boundary torus, and Meridian and preferred longitude defines the positive meridian by the normal-disk boundary and the preferred longitude by degree one and zero exterior homology.

[F3]

Under full AC, Homology and preferred longitude of a knot exterior proves H1(EK;Z)≅Z generated by the positive meridian, proves existence and uniqueness of the preferred-longitude class, and proves that their boundary classes form a basis of H1(∂EK;Z).

[F4]

Seifert–van Kampen identifies the fundamental group with a group pushout identifies the fundamental group of a union from a path-connected open cover with the pushout of the two inclusion-induced maps from the intersection.

[F5]

The smooth inverse function theorem says that a smooth map with invertible differential at a point is a diffeomorphism between suitable open neighbourhoods of that point and its image (The smooth inverse function theorem on manifolds).

Proof

Given: The knot, exterior, Heegaard splitting and AC hypotheses in the Statement.

1.1A1L1F2F5givenconstructalgebra

The round-metric tube is an admissible invariant tube. Full AC supplies the countable-choice hypothesis for the smooth normal-bundle structure by [L1]. Regard S3 as the unit sphere in R4 with its round metric, and identify each quotient normal plane TxS3/TxK with its orthogonal complement to TxK in TxS3. For v∈νx(K) let v^ be that representative and define Φ(x,v)=cos⁡(∥v∥)x+sin⁡(∥v∥)∥v∥v^, with Φ(x,0)=x. This is the round normal exponential map. Its differential along the zero section sends a tangent-normal pair (u,w) to u+w, an isomorphism. By [F5] it is a local diffeomorphism at every zero vector. Compactness of K gives a uniform disk neighbourhood on which its differential stays invertible. After shrinking that radius, Φ is injective there: otherwise there would be distinct (xn,vn),(yn,wn) with ∥vn∥,∥wn∥→0 and equal images; compactness gives subsequences converging to (x,0),(y,0), equality gives x=y, and a local inverse near (x,0) contradicts distinctness. Thus, for some R>0, Φ is a diffeomorphism from the open normal disk bundle of radius R onto an open neighbourhood of K. Choose 0<ϵ<R/2 also smaller than π and than the distance from K to either coordinate circle. The closed metric ϵ-neighbourhood of K equals Φ({v:∥v∥≤ϵ}): a nearest point of K exists for every point in that neighbourhood, and minimizing round distance is equivalent to maximizing the Euclidean dot product with that point; differentiating along K shows the corresponding short great-circle segment is normal to K. Conversely, each normal vector of length at most ϵ gives a geodesic of that length, and injectivity on the radius-R disk bundle rules out a closer nearest point. Hence this N(K) is the closed tubular neighbourhood required by [F2], is disjoint from the two coordinate circles, and is invariant under ρt, since these maps are orthogonal and preserve K. Finally, the local product charts of Φ and compactness of K allow ϵ to be decreased so that N(K)∩Tr is an annular neighbourhood of K in the Heegaard torus; its two halves are boundary collars on the two solid-torus sides.

2.1givenA1F1F2L1step 1.1construct

The primitive slope pα+qβ is essential on the Heegaard torus. Removing a small annular neighborhood of K from that torus leaves a closed annulus A. On either side, removing the corresponding half of the tube from a solid torus only removes a boundary collar, so the two pieces retract to solid tori Wx,Wy and their overlap retracts to A. Thicken the pieces by half-collars to obtain path-connected open sets covering EK whose intersection retracts to A. The core of A winds p times around the core generator x on one side and q times around y on the other. Full AC [A1] supplies the countable-choice hypothesis of [F2] by [L1].

2.2F1givenstep 1.1construct

The generic orbits of ρt have slope (p,q) and trivial stabilizer: if both coordinates are nonzero, a stabilizing parameter t∈R/Z satisfies pt,qt∈Z, hence t=0 because gcd⁡(p,q)=1. The stabilizer orders on the coordinate circles z1=0 and z2=0 are ∣q∣ and ∣p∣, respectively. The orbit space is a sphere: on each intermediate torus ∣z1∣=r with 0<r<1, quotienting by the primitive circle orbit leaves a circle, and at r=0,1 that quotient circle collapses to the corresponding coordinate-orbit point. The invariant tube from step 1.1 lies in the free-orbit region, and its quotient is a disk: every orbit in its normal disk bundle meets the fiber over one chosen point of K exactly once. Removing its interior therefore removes a disk from the orbit sphere, leaving a disk. The quotient map is a Seifert fibration of EK with the two stated core multiplicities. Multiplicity one is regular; multiplicity greater than one is exceptional.

3.1F4step 2.1algebra

The three fundamental groups in this cover are π1(Wx)=⟨x⟩≅Z, π1(Wy)=⟨y⟩≅Z, and π1(A)=⟨a⟩≅Z, with inclusion maps a↦xp and a↦yq. By [F4], π1(EK) is their pushout. A group receiving maps from the two cyclic factors is determined by images of x,y; the maps agree on the intersection exactly when xp=yq. Hence the pushout has presentation ⟨x,y∣xp=yq⟩.

4.1step 3.1step 2.2algebra

A regular orbit parallel to K represents the annulus core xp=yq=h. This element commutes with x because it is xp, and commutes with y because it is yq; as x,y generate the group from step 3.1, h is central.

4.2A1L1F1F2F3step 3.1algebraconstruct

Choose integers c,d with pd−qc=1 and let L=cα+dβ. With the coordinate orientation determined by α followed by β, the ordered intersection number K⋅L=pd−qc=1, so L is a simple curve meeting K once. At the intersection, the boundary m of a small normal disk splits into arcs γx,γy on the two solid-torus sides, while L splits into its crossing arc and complementary arc L1. Inserting L1L1−1 into m=γxγy gives m=(γxL1)(L1−1γy). The first factor winds c times around the x core and the second winds −d times around the y core, hence m=xcy−d. To calibrate signs geometrically, the positively oriented coordinate cores representing x and y bound the hemispherical disks Dx={Im⁡z2=0, Re⁡z2≥0}∩S3 and Dy={Im⁡z1=0, Re⁡z1≥0}∩S3, oriented by their respective core boundaries. The knot meets Dx transversely in ∣q∣ points, each with intersection sign sgn⁡(q), and meets Dy in ∣p∣ points, each with sign sgn⁡(p). For the first sign, at a point where z2 is positive real, the ambient orientation is the complex z1 orientation followed by increasing Im⁡z2; the component of the knot tangent transverse to Dx has sign q. For the second, at positive real z1, the ambient orientation is increasing Im⁡z1 followed by the complex z2 orientation, and the transverse tangent component has sign p. Deleting small disks about these intersections gives oriented surfaces in the knot complement with boundary relations [x]=q[μ] and [y]=p[μ], where μ is the positive normal-disk meridian. Thus the abelianization x↦q, y↦p sends this geometric meridian to 1: [F3] makes [μ] a generator, and the displayed relations and gcd⁡(p,q)=1 fix its sign. The disk-boundary curve m has abelianization cq−dp=−1, so its orientation is opposite to that positive meridian. Thus μ=m−1=ydx−c. Setting α=d and β=−c gives pα+qβ=1 and the stated word; another Bezout solution changes the exponents by (qk,−pk), so the word is unchanged because yqk=hk=xpk and h is central.

5.1L1F2F3step 1.1step 3.1step 4.1step 4.2algebra∎

Abelianizing the presentation in step 3.1 gives the relation p[x]=q[y]. The map x↦q, y↦p is surjective because gcd⁡(p,q)=1, and its kernel in Z2 is generated by (p,−q), exactly the relation vector; hence it identifies this quotient with Z. Step 4.2 sends the positive meridian to 1, so by [F3] it is the positive generator of H1(EK;Z). Thus [h]=p[x]=pq[μ]. The regular orbit h is a degree-one parallel of K under the equivariant normal-bundle projection from step 1.1, and μ has degree zero there, so λ=hμ−pq has degree one and zero image in H1(EK). Uniqueness in [F3] identifies it with the preferred longitude; [F3] also proves that [μ],[λ] form a basis of H1(∂EK;Z), so each is primitive.

Diagram

The square records the annulus-to-solid-torus inclusions used in steps 2.1 and 3.1. Its two composites agree on the annulus core precisely when xp=yq; the proof applies Seifert–van Kampen to establish that the lower-right group is the pushout and does not rely on the drawing.

¼1(A)=hai¼1(Wx)=hxi¼1(Wy)=hyi¼1(EK)a7!xpa7!yqinclusioninclusion

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