Artin's classical theorem embeds the n-strand braid group BnB_n faithfully into the automorphism group Aut⁡(Fn)\operatorname{Aut}(F_n) of a free group, via the conjugation action of braids on the fundamental group of the punctured disk. Bardakov and Bellingeri (2007, published 2011) extended this construction to surface braid groups: inside a suitable mixed braid group there is a naturally defined free subgroup on which the surface braid group acts by conjugation, yielding representations into automorphism or outer automorphism groups of free groups. They proved faithfulness for oriented surfaces with boundary, both into Aut⁡(Un−1,g,p)\operatorname{Aut}(U_{n-1,g,p}) and, after projection, into Out⁡(Un−1,g,p)\operatorname{Out}(U_{n-1,g,p}) (the latter for p>0p > 0 when g>0g > 0 and for p>2p > 2 when g=0g = 0). Two cases were left explicitly open: (i) the representation ρW:Bn(Ng,p)→Aut⁡(Wn,g,p)\rho_W: B_n(N_{g,p}) \to \operatorname{Aut}(W_{n,g,p}) for non-orientable surfaces Ng,pN_{g,p} of genus g≥1g \ge 1 with p≥1p \ge 1 boundary components and n>1n > 1 strands; and (ii) the representation ρ~V:Bn−1(Σg)→Out⁡(Vn−1,g)\tilde\rho_V: B_{n-1}(\Sigma_g) \to \operatorname{Out}(V_{n-1,g}) for closed orientable surfaces Σg\Sigma_g of genus g≥1g \ge 1 with n>1n > 1. This problem asks to determine, in each of the two remaining surface classes, whether the Bardakov-Bellingeri representation is faithful, and to describe the kernel when it is not.

Background

Let FnF_n denote the free group of rank nn and Aut⁡(Fn)\operatorname{Aut}(F_n), Out⁡(Fn)\operatorname{Out}(F_n) its automorphism group and its outer automorphism group, the quotient of Aut⁡(Fn)\operatorname{Aut}(F_n) by the subgroup of inner automorphisms (conjugations). Artin's theorem represents BnB_n as the subgroup of Aut⁡(Fn)\operatorname{Aut}(F_n) sending each generator xix_i to a conjugate of some xs(i)x_{s(i)} and fixing the product x1x2⋯xnx_1x_2\cdots x_n; geometrically BnB_n is the mapping class group of the disk with nn marked points (the group of isotopy classes of orientation-preserving homeomorphisms preserving the marked set) and acts on π1\pi_1 of the punctured disk, which is free. This problem concerns the extension of this picture to braid groups of surfaces.

For a surface Σ\Sigma, the nn-strand surface braid group Bn(Σ)B_n(\Sigma) is the fundamental group of the configuration space of nn unordered points on Σ\Sigma. Finite presentations are known: for a closed orientable surface Σg\Sigma_g of genus g≥1g \ge 1, Bn(Σg)B_n(\Sigma_g) is generated by σ1,…,σn−1\sigma_1,\dots,\sigma_{n-1} and x1,…,x2gx_1,\dots,x_{2g} (the latter take a point around the handles), subject to braid relations, mixed relations, and the surface relation [x1−1,x2][x3−1,x4]⋯[x2g−1−1,x2g]=σ1σ2⋯σn−12⋯σ2σ1[x_1^{-1},x_2][x_3^{-1},x_4]\cdots[x_{2g-1}^{-1},x_{2g}] = \sigma_1\sigma_2\cdots\sigma_{n-1}^2\cdots\sigma_2\sigma_1; for a compact non-orientable surface Ng,pN_{g,p} of genus g≥1g \ge 1 with p≥1p \ge 1 boundary components, Bn(Ng,p)B_n(N_{g,p}) is generated by σ1,…,σn−1\sigma_1,\dots,\sigma_{n-1}, the crosscap loops a1,…,aga_1,\dots,a_g and boundary loops z1,…,zp−1z_1,\dots,z_{p-1} of the fundamental group of Ng,pN_{g,p}, with analogous relations (Bellingeri 2004).

The Bardakov-Bellingeri construction uses the mixed braid group Dn(Σ)=π−1(Sn−1)D_n(\Sigma) = \pi^{-1}(S_{n-1}), the subgroup of Bn(Σ)B_n(\Sigma) of braids whose underlying permutation fixes the last point (the last strand returns to its starting position), where π:Bn(Σ)→Sn\pi: B_n(\Sigma) \to S_n records the underlying permutation. A Reidemeister-Schreier computation (the standard algorithm that produces generators for a subgroup of a presented group from coset representatives) on Dn(Σ)D_n(\Sigma) produces distinguished generators: elements τ1,…,τn−1\tau_1,\dots,\tau_{n-1} (conjugated forms of the squares σk2\sigma_k^2, geometrically loops of a moving point around the fixed point), together with conjugated forms wrw_r of the handle (or crosscap) loops and ξj\xi_j of the boundary loops. The subgroups they generate are free and carry the representation: Un−1,g,p=⟨τ1,…,τn−1,w1,…,w2g,ξ1,…,ξp−1⟩U_{n-1,g,p} = \langle\tau_1,\dots,\tau_{n-1}, w_1,\dots,w_{2g}, \xi_1,\dots,\xi_{p-1}\rangle of rank n+2g+p−2n+2g+p-2 in the orientable-with-boundary case, Wn,g,p=⟨τ1,…,τn−1,w1,…,wg,ξ1,…,ξp−1⟩W_{n,g,p} = \langle\tau_1,\dots,\tau_{n-1}, w_1,\dots,w_g, \xi_1,\dots,\xi_{p-1}\rangle of rank n+g+p−2n+g+p-2 in the non-orientable case (a subgroup of Dn+1(Ng,p)D_{n+1}(N_{g,p})), and Vn−1,g=⟨τ2,…,τn−1,w1,…,w2g⟩V_{n-1,g} = \langle\tau_2,\dots,\tau_{n-1}, w_1,\dots,w_{2g}\rangle of rank 2g+n−22g+n-2, normal in Dn(Σg)D_n(\Sigma_g), in the closed orientable case. The relevant surface braid group acts on each free subgroup by conjugation, with explicit generator-wise formulas.

For oriented surfaces with boundary the source proves: (Theorem 2) ρU:Bn−1(Σg,p)→Aut⁡(Un−1,g,p)\rho_U: B_{n-1}(\Sigma_{g,p}) \to \operatorname{Aut}(U_{n-1,g,p}) is faithful for g≥0g \ge 0, p>0p > 0, n≥3n \ge 3, by realizing the action as conjugation inside the mapping class group of the punctured surface and applying curve-intersection arguments; and (Theorem 3) the projected representation into Out⁡(Un−1,g,p)\operatorname{Out}(U_{n-1,g,p}) is faithful for p>0p > 0 when g>0g > 0 and for p>2p > 2 when g=0g = 0, using that elements acting by inner automorphisms are central and that the relevant braid groups have trivial center. As corollaries, Bm(Σg,p)B_m(\Sigma_{g,p}) with p>0p > 0 is residually finite (its nontrivial elements survive in some finite quotient), and Fox calculus (the free-differential calculus on group rings) yields a Burau-type linear representation from ρU\rho_U. Two constructions could not be settled. (i) For Ng,pN_{g,p} non-orientable with boundary, Bn(Ng,p)B_n(N_{g,p}) acts on Wn,g,pW_{n,g,p}, giving ρW:Bn(Ng,p)→Aut⁡(Wn,g,p)\rho_W: B_n(N_{g,p}) \to \operatorname{Aut}(W_{n,g,p}) with the formulas of the source's Theorem 4; every element of the image fixes the distinguished element A=τn−1−1⋯τ2−1τ1−1ξ1ξ2⋯ξp−1w12w22⋯wg2A = \tau_{n-1}^{-1}\cdots\tau_2^{-1}\tau_1^{-1}\xi_1\xi_2\cdots\xi_{p-1}w_1^2w_2^2\cdots w_g^2 (the source's Proposition 5). (ii) For closed Σg\Sigma_g, the subgroup Bˉn−1(Σg)=⟨σ1,…,σn−2,x1,…,x2g⟩\bar B_{n-1}(\Sigma_g) = \langle\sigma_1,\dots,\sigma_{n-2}, x_1,\dots,x_{2g}\rangle of Dn(Σg)D_n(\Sigma_g) acts by conjugation on Vn−1,gV_{n-1,g} by automorphisms (Proposition 7), but Bˉn−1(Σg)\bar B_{n-1}(\Sigma_g) is not Bn−1(Σg)B_{n-1}(\Sigma_g): the surface relation forces τ1=[w1−1,w2][w3−1,w4]⋯[w2g−1−1,w2g]τn−1−1⋯τ2−1\tau_1 = [w_1^{-1},w_2][w_3^{-1},w_4]\cdots[w_{2g-1}^{-1},w_{2g}]\tau_{n-1}^{-1}\cdots\tau_2^{-1} to lie in Vn−1,gV_{n-1,g}, and Bn−1(Σg)≃Bˉn−1(Σg)/⟨⟨τ1⟩⟩B_{n-1}(\Sigma_g) \simeq \bar B_{n-1}(\Sigma_g)/\langle\langle\tau_1\rangle\rangle. The action therefore descends only to the outer level, giving ρ~V:Bn−1(Σg)→Out⁡(Vn−1,g)\tilde\rho_V: B_{n-1}(\Sigma_g) \to \operatorname{Out}(V_{n-1,g}) (Proposition 8), whose formulas for the action of the generators σ1,…,σn−2,x1,…,x2g\sigma_1,\dots,\sigma_{n-2}, x_1,\dots,x_{2g} on the free generators are well-defined up to conjugacy. For comparison, already over the disk the projection Bn→Out⁡(Fn)B_n \to \operatorname{Out}(F_n) has kernel the infinite cyclic center of BnB_n.

Geometrically the free subgroups are point-pushing-type subgroups (their generators are bounding-pair braids — multitwists along two curves enclosing a single puncture, also called spin maps — in the mapping class group of the punctured surface), so the open questions ask whether the conjugation action of the remaining surface braid groups on such subgroups is faithful - a surface-braid analogue of Artin's theorem. Faithfulness would embed Bn(Ng,p)B_n(N_{g,p}) into Aut⁡(Fn+g+p−2)\operatorname{Aut}(F_{n+g+p-2}) and Bn−1(Σg)B_{n-1}(\Sigma_g) into Out⁡(F2g+n−2)\operatorname{Out}(F_{2g+n-2}), paralleling the classical characterization of mapping class groups as outer automorphism groups of surface groups.

Problem Statement

Determine whether the two Bardakov-Bellingeri conjugation representations of surface braid groups, left open by the source, are faithful, and describe their kernels.

Component (1) - non-orientable surfaces with boundary. Let Ng,pN_{g,p} be a compact connected non-orientable surface of genus g≥1g \ge 1 with p≥1p \ge 1 boundary components and let n>1n > 1. Inside the mixed braid group Dn+1(Ng,p)D_{n+1}(N_{g,p}) consider the free group Wn,g,p=⟨τ1,…,τn−1,w1,…,wg,ξ1,…,ξp−1⟩W_{n,g,p} = \langle\tau_1,\dots,\tau_{n-1}, w_1,\dots,w_g, \xi_1,\dots,\xi_{p-1}\rangle of rank n+g+p−2n+g+p-2 generated by the Reidemeister-Schreier-type elements (τk\tau_k conjugated forms of σk2\sigma_k^2; wrw_r, ξj\xi_j conjugated forms of the crosscap and boundary generators ara_r, zjz_j), as defined in Section 4 of the source [1, 2]. The group Bn(Ng,p)B_n(N_{g,p}) acts on Wn,g,pW_{n,g,p} by conjugation, giving the representation ρW:Bn(Ng,p)→Aut⁡(Wn,g,p)≅Aut⁡(Fn+g+p−2)\rho_W: B_n(N_{g,p}) \to \operatorname{Aut}(W_{n,g,p}) \cong \operatorname{Aut}(F_{n+g+p-2}) defined on the generators σi\sigma_i (1≤i≤n−11 \le i \le n-1), ara_r (1≤r≤g1 \le r \le g), zjz_j (1≤j≤p−11 \le j \le p-1) by the explicit formulas of the source's Theorem 4. Question: is ρW\rho_W injective? A complete answer determines the set of triples (g,n,p)(g,n,p) with g≥1g \ge 1, n>1n > 1, p≥1p \ge 1 for which ρW\rho_W is faithful and describes ker⁡ρW\ker\rho_W otherwise; note that every element of the image fixes the element A=τn−1−1⋯τ2−1τ1−1ξ1ξ2⋯ξp−1w12w22⋯wg2A = \tau_{n-1}^{-1}\cdots\tau_2^{-1}\tau_1^{-1}\xi_1\xi_2\cdots\xi_{p-1}w_1^2w_2^2\cdots w_g^2, which constrains the possible image.

Component (2) - closed orientable surfaces. Let Σg\Sigma_g be a closed orientable surface of genus g≥1g \ge 1 and let n>1n > 1. In Dn(Σg)D_n(\Sigma_g) consider the free group Vn−1,g=⟨τ2,…,τn−1,w1,…,w2g⟩V_{n-1,g} = \langle\tau_2,\dots,\tau_{n-1}, w_1,\dots,w_{2g}\rangle of rank 2g+n−22g+n-2, normal in Dn(Σg)D_n(\Sigma_g) and containing the element τ1=[w1−1,w2][w3−1,w4]⋯[w2g−1−1,w2g]τn−1−1⋯τ2−1\tau_1 = [w_1^{-1},w_2][w_3^{-1},w_4]\cdots[w_{2g-1}^{-1},w_{2g}]\tau_{n-1}^{-1}\cdots\tau_2^{-1}. With Bˉn−1(Σg)=⟨σ1,…,σn−2,x1,…,x2g⟩\bar B_{n-1}(\Sigma_g) = \langle\sigma_1,\dots,\sigma_{n-2}, x_1,\dots,x_{2g}\rangle acting on Vn−1,gV_{n-1,g} by conjugation (the source's Proposition 7) and Bn−1(Σg)≃Bˉn−1(Σg)/⟨⟨τ1⟩⟩B_{n-1}(\Sigma_g) \simeq \bar B_{n-1}(\Sigma_g)/\langle\langle\tau_1\rangle\rangle, the action descends to the representation ρ~V:Bn−1(Σg)→Out⁡(Vn−1,g)≅Out⁡(F2g+n−2)\tilde\rho_V: B_{n-1}(\Sigma_g) \to \operatorname{Out}(V_{n-1,g}) \cong \operatorname{Out}(F_{2g+n-2}) given, up to conjugacy, on the generators of Bn−1(Σg)B_{n-1}(\Sigma_g) by the formulas (S1)-(S11) of the source's Proposition 8. Question: is ρ~V\tilde\rho_V injective? A complete answer determines the pairs (g,n)(g,n) with g≥1g \ge 1, n>1n > 1 for which it is faithful and describes ker⁡ρ~V\ker\tilde\rho_V otherwise; in particular it identifies which nontrivial surface braids act as inner automorphisms of Vn−1,gV_{n-1,g}.

The two components share one objective: completing the faithfulness picture begun by Artin for the disk and by the source for oriented surfaces with boundary, for the Bardakov-Bellingeri representations of surface braid groups as (outer) automorphisms of free groups, in the source's natural generality. Answers may treat the components separately; partial resolutions (specific genera or strand numbers) count insofar as they contribute to the complete regime determination.

References

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