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The Ain are meridian generators of the forgetful free kernel

Statement

Assume the Axiom of Choice and let n≥2, with the notation PBn, PBn−1, Fn−1, φ and κ of The Fadell-Neuwirth short exact sequence for pure braids, and the standard geometric generators Aij of Standard geometric pure braid generators A_ij. Then, under the identification Fn−1≅ker⁡φ given by κ, the n−1 elements Ψ([A1n]),…,Ψ([An−1,n]) are a free basis of ker⁡φ. There is a compatible system of pairwise interior-disjoint stems from qn to small circles around q1,…,qn−1 such that, if γi is the counterclockwise based meridian of qi along the i-th stem, then Ψ([Ain])=(κ∗[γi])−1(1≤i<n). Thus each displayed element is the clockwise based meridian in the fibre.

Facts & Assumptions

Given: AC, n≥2, the equally spaced base configuration Q=(q1,…,qn), positive half twists σi with supports Ui, the first-under-second stacking convention, the fibre Yn=int⁡D2∖{q1,…,qn−1} based at qn, and the notation Ψ,κ,φ of the cited braid and forgetting maps.

[A1]

The Axiom of Choice holds (The Axiom of Choice).

[F1]
[F2]

Under AC the last-coordinate forgetful map gives the short exact sequence 1→Fn−1→κPBn→φPBn−1→1, where Fn−1=π1(Yn,qn), κ is induced by x↦(q1,…,qn−1,x) followed by the open-to-closed configuration isomorphism, and φ is induced by dropping the last coordinate (The Fadell-Neuwirth short exact sequence for pure braids, The Fadell-Neuwirth forgetful map: local triviality, constant fibre, and numerability for configurations in the disk).

[F3]

The space Yn is homotopy equivalent to a wedge of n−1 circles; its fundamental group is free of rank n−1, and it has a counterclockwise meridian free basis for some choice of stems (A finitely punctured open disk has the homotopy type of a finite wedge of circles). The regular-neighborhood argument in step 4.1 establishes the basis property for the particular compatible stems used here.

[F4]

The positive half twist σi is supported in the open disc Ui of radius 3h/2 centered at mi, where qi=mi−(h,0), qi+1=mi+(h,0), and all other base points lie outside Ui; the discs satisfy Ui∩Uj=∅ when ∣i−j∣>1 (The elementary geometric half twist, its support disc, and its opposite).

[F5]

The standard generator is Ain=σn−1⋯σi+1σi2σi+1−1⋯σn−1−1, with the rightmost factor traversed first under first-under-second stacking (Standard geometric pure braid generators A_ij, Stacking of geometric braids is a well-defined associative operation on isotopy classes, The isotopy classes of geometric braids based at Q form a group, and the endpoint permutation is a homomorphism).

[F6]

The pure geometric braid group is identified with PBn by Ψ([β])=(ι∗F[zβ])−1, where zβ is the ordered coordinate loop of β (Pure geometric braids and ordered configuration loops).

[F7]

The braid-to-mapping-class isomorphism sends σi to the class of an orientation-preserving homeomorphism Hi supported in Ui and exchanging qi,qi+1 (Braid group as boundary-fixed punctured-disk mapping classes).

[F8]

For a based point-motion loop, the associated point-pushing mapping class is represented by the inverse endpoint of an ambient lift. For the last puncture, the point-pushing map satisfies Θn∘κ=Push⁡n, where Θn:PBn→PMod⁡(D2,Q;∂D2) is the isomorphism induced by the geometric-braid and mapping-class identifications; the evaluation fibration supplies ambient lifts for point motions (Point pushing the last puncture, Boundary map from point motions, Point pushing is the kernel of forgetting the last disk puncture, Evaluation boundary isomorphism for the disk).

[F9]

A braid word giσi2gi−1, with gi=σn−1⋯σi+1, maps under the braid-to-mapping-class homomorphism to hiΨnmc([σi2])hi−1, where hi=Hn−1∘⋯∘Hi+1; the rightmost homeomorphism acts first. This follows from the homomorphism and the ordinary composition law in the boundary-fixed mapping-class group (Braid group as boundary-fixed punctured-disk mapping classes, Boundary-fixed mapping class group of a punctured disk).

[F10]

Every finite polygonal disk admits a piecewise-linear parametrization, and any piecewise-linear boundary homeomorphism extends over it (Finite polygonal disk parametrizations and boundary surgery).

Proof

technique · direct
1.1A1F1F2F3F6

The free kernel to be identified. By [F1] the choice hypothesis [A1] supplies DC, so [F2] gives an injection κ with image ker⁡φ. The fibre Yn has free fundamental group of rank n−1 by [F3]. It remains to identify the individual Ain with a single coherent meridian basis, with the inverse sign from [F6].

1.2F4F7F8

The two-point winding calculation. For any 0<ϵi≤h/10, let Ci={z:∣z−qi∣=ϵi}, and let ci=qi+(ϵi,0) on it. For any simple local stem τi from qi+1 to ci in Ui∖{qi}, let λi be the based loop that follows τi, goes once counterclockwise around Ci, and returns along τˉi. The straight segment is one possible stem. For a pair in Ui=B(mi,R), R=3h/2, write u=(z2−z1)/∣z2−z1∣∈S1, r=∣z2−z1∣>0, and w=uˉ((z1+z2)/2−mi). Then F2(Ui)≅S1×C,C={(w,r)∈C×(0,∞):∣w−r/2∣<R, ∣w+r/2∣<R}. The inverse coordinate map is (u,w,r)↦(mi+u(w−r/2),mi+u(w+r/2)), so the displayed coordinates give a homeomorphism. The condition r>0 and the two inverse images of the convex disk B(0,R) make C convex and nonempty. Hence the winding of u induces an isomorphism π1(F2(Ui))≅Z. During the first positive half twist, the relative vector z2−z1 starts at 2h, follows the upper half of the diamond path to −2h, and its argument increases by π. In the second positive half twist, stacking matches the exchanged endpoints, so the same ordered pair follows the lower half of the diamond from −2h to 2h; its argument increases by another π. Thus the ordered loop of σi2 has relative winding +1. The point motion that fixes qi and moves qi+1 out along the stem to Ci, once counterclockwise around Ci, and back along the stem also has relative winding +1: the outgoing and return stem paths cancel in winding and the circle contributes +1. These two loops therefore have the same class in π1(F2(Ui)). Inserting all other stationary points gives the same equality in the full ordered configuration space, because Ui contains no other base point. By [F7] and the inverse-endpoint definition in [F8], the braid-to-mapping-class isomorphism Ψnmc:Gn→Mod⁡(D2,Q;∂D2) satisfies Ψnmc([σi2])=Push⁡qi+1([λi])−1.

2.1F5F7F8F9step 1.2

Conjugation transports the local point push. Fix radii and local stems satisfying step 1.2. For a marked point p∈Q and a based loop α in int⁡D2∖(Q∖{p}) at p, let Push⁡p([α]) be the mapping class of F1−1, where Ft is an ambient isotopy starting at the identity, fixing the boundary and every point of Q∖{p}, and satisfying Ft(p)=α(t). This class is well defined: it is the inverse-endpoint boundary-map value of the full configuration loop with the other marked points fixed, as in [F8]. It agrees with [F8] when p=qn. If h represents a mapping class preserving Q setwise and taking p to p′, then hFth−1 is an ambient lift of h∘α fixing every other marked point; its endpoint inverse is hF1−1h−1. Therefore, with the paths typed in the respective puncture complements, h Push⁡p([α]) h−1=Push⁡p′([h∘α]). Now put gi=σn−1⋯σi+1 and hi=Hn−1∘⋯∘Hi+1. The rightmost factor acts first: Hi+1 takes qi+1 to qi+2, then Hi+2 takes it to qi+3, and so on, while every Hj fixes qi and the circle Ci. Since ∣mi−qi∣=h and ϵi≤h/10, Ci⊂Ui. For j≥i+2, the supports Uj and Ui are disjoint by [F4]. For j=i+1, the center of Ui+1 is at distance 3h from qi, so every point of Ci is at distance at least 3h−h/10>3h/2 from that center; hence this circle too is outside the support. Thus all the stated fixes are pointwise. In particular hi(qi+1)=qn, hi(qi)=qi, and hi(Ci)=Ci. If τi is the local stem used in step 1.2, put τ^i:=hi∘τi; this is a stem from qn to Ci in Yn. Let γ^i be the based loop following τ^i, going counterclockwise around Ci, and returning along its reverse. The first-under-second word order in [F5] and the mapping-class homomorphism [F9] give the following. Put Θn:=Ψnmc∣Gnpure∘Ψ−1, the isomorphism PBn→PMod⁡(D2,Q;∂D2) of [F8]. The conjugation naturality just proved yields Θn(Ψ([Ain]))=Ψnmc([Ain])=hi Push⁡qi+1([λi])−1hi−1=Push⁡n([γ^i])−1. By [F8], this is Θn((κ∗[γ^i])−1). Injectivity of Θn proves Ψ([Ain])=(κ∗[γ^i])−1 for each i<n.

3.1

A coherent noncrossing system of transported stem classes. For 2≤m≤n and i<m, put hi(m):=Hm−1∘⋯∘Hi+1, with the empty composition for i=m−1, and let τ^i(m):=hi(m)∘τi be the transported stem of step 2.1 at rank m. Here the local stem τ1 is chosen at the base case, and each τm is chosen when the rank-m+1 fan is added; thus the same coherent family is used in steps 1.2 and 2.1. We construct, by induction on m, a fan of embedded arcs η1(m),…,ηm−1(m) whose relative endpoint-fixed homotopy classes are exactly those of τ^1(m),…,τ^m−1(m). At m=2, take C1 of radius h/10 and the straight stem from q2 to c1.

Suppose such a fan has been built at rank m<n. Its stems lie in ⋃j<mUj, and the new support Um is disjoint from all earlier supports except Um−1. Thus its intersections with Um lie in the convex lens L:=Um−1∩Um, which contains no marked point other than the root qm; the adjacent points qm−1,qm+1 lie outside L. Each target circle Ci, i<m, is outside Um: its center qi is at distance (2(m−i)+1)h≥3h from the center of Um, and its radius is at most h/10. Choose finite polygonal representatives of the existing embedded fan, perturbing them jointly so they remain pairwise disjoint away from the root, are in general position with ∂L, and have distinct boundary intersection points. Any portion of an old stem in Um lies in L. Remove each boundary-to-boundary excursion in L by the usual outermost-disk slide: an innermost such subarc cuts off the side not containing qm, a disk in the puncture-free lens with no other stem arc in its interior. Sliding across that disk removes two boundary intersections and preserves the relative class and disjointness; finitely many slides leave no return excursion. The target circles are outside Um. Moreover, the only side of ∂L through which an old stem can continue in the union of the old supports is the ∂Um side into Um−1∖Um; the other side enters the part of Um outside every old support. Thus the remaining initial segment of each old stem runs from qm to one point of ∂Um, and these exit points are distinct.

Replace these initial arcs by a radial fan in L with the same boundary endpoints in the same boundary order. Cutting the lens along the old arcs and this fan gives polygonal disks whose corresponding boundary maps extend over the disks by [F10]. Gluing the extensions gives a homeomorphism supported in L, fixing its boundary and qm, that carries the old initial arcs to the fan. Since L is convex with root qm, the Alexander isotopy centered at qm makes this a homotopy relative to the root and the exits on ∂L. This changes representatives but not the transported stem classes. The re-routing lies in L, which avoids qm+1, and fixes qm. The old fan also avoids qm+1 because it lies in ⋃j<mUj. Since Hm−1(qm)=qm+1, the re-routing and old fan map to paths and a homotopy in the next fiber, which has the new puncture qm removed. The supported map Hm now carries this fan to a fan rooted at qm+1, with exits fixed on ∂Um; it fixes q1,…,qm−1 and takes qm to qm+1, so it carries each transported class at rank m to its specified class at rank m+1.

The image fan cuts Um into sectors whose closures contain qm+1. The point qm lies in one such sector: it is not on the transported fan, since its preimage qm+1 lies outside ⋃j<mUj. Choose 0<ϵm≤h/10 so the closed disk about qm of radius ϵm is contained in that sector and misses the old fan; set Cm={∣z−qm∣=ϵm} and cm=qm+(ϵm,0). In the chosen sector's closure minus the open disk, take a simple arc from qm+1 to cm whose interior lies in the sector outside the closed disk and misses the old fan. This region is path connected: a closed disk contained in the interior of a disk sector removes only an interior disk, leaving a connected annular sector. The arc can be chosen simple by deleting loops from a polygonal path. This is a local stem τm⊂Um∖{qm} meeting Cm only at cm. It misses every older circle Ci because those circles lie outside Um. Adding it to the transported old fan gives a fan rooted at qm+1, with pairwise interior-disjoint stems, and all stems lie in ⋃j≤mUj.

The old circles remain fixed by Hm: for i≤m−2, Ui∩Um=∅; for i=m−1, every point of Cm−1 is within h/10 of qm−1, whose distance from the center of Um is 3h, while Um has radius 3h/2. Consequently the new fan arcs still end at the same ci and represent the classes [hi(m+1)∘τi] for i<m, together with the local class [τm] for i=m. At m=n the resulting disjoint fan stems have exactly the relative homotopy classes of the transported stems hi∘τi in step 2.1, so their based meridian classes are the [γ^i] there. Homotopic stems give homotopic based meridians; the conjugation identity just proved therefore gives Ψ([Ain])=(κ∗[γ^i])−1 for these compatible tree stems, rather than for an unrelated choice of meridians. [F4, F10, step 2.1]

4.1F2F3step 2.1step 3.1

These meridians are a free basis. Let T be the final fan tree formed by the stems from qn to ci. It is an embedded tree whose stems have pairwise disjoint interiors, and it meets each Ci only at ci. Take a closed regular neighborhood N of T∪C1∪⋯∪Cn−1 in Yn. It is a disk with n−1 holes: the tree joins the n−1 disjoint inner circles and has no cycles, so thickening it adds no further hole. Write Bi for its i-th inner boundary and B0 for its outer boundary. The puncture qi lies inside Bi, and Bi is parallel to Ci through an annular collar in N. The part of Yn inside each Bi is a punctured disk and radially deformation retracts onto Bi; the outside complement between B0 and ∂D2 is an annular collar that deformation retracts onto B0. These retractions are the identity on the corresponding boundary circles, so they glue to a deformation retraction of Yn onto N. Choose N as vertex disks and edge strips for the finite polygonal graph; collapsing each strip across its width to its core and each vertex disk onto its incident radial arcs gives a deformation retraction onto T∪C1∪⋯∪Cn−1. Collapsing the tree gives a wedge of n−1 circles. Each counterclockwise loop on Ci is homotopic in its collar in N to the counterclockwise loop on Bi, and the based loop that follows the i-th stem, traverses Ci counterclockwise, and returns therefore follows the corresponding circle summand once. Thus [γ^1],…,[γ^n−1] form a free basis of Fn−1; their inverses form a free basis as well. Since κ identifies this group with ker⁡φ by [F2], steps 2.1 and 3.1 prove both the free-basis assertion and the clockwise sign in the Statement.

5.1F2F6step 1.2step 2.1step 4.1

The sign and conclusion. For n=2, the calculation in step 1.2 says that the raw ordered loop of A12=σ12 has relative winding +1; the published identification [F6] inverts that loop, so its image is the clockwise meridian of winding −1. The same inverse is exactly the inverse-endpoint convention in steps 1.2 and 2.1, and no injectivity of an Artin presentation is used. This completes the proof. ∎

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