An integral homology 3-sphere YY may or may not bound a smooth, homologically 1-connected, definite (positive- or negative-definite), spin 4-manifold; when it does, the intersection form is an even unimodular definite lattice — a multiple of the E8E_8 lattice in rank 8, but in higher rank also lattices such as D16+D_{16}^+ or the Niemeier lattices. Tange (Topology and its Applications 202 (2016) 160–182) introduced the invariants ds(Y)≥ds‾(Y)\mathfrak{ds}(Y)\ge\overline{\mathfrak{ds}}(Y), the maximum and minimum of b2(X)/8b_2(X)/8 over such boundings, and the E8E_8-genera g8(Y)≥g8‾(Y)g_8(Y)\ge\overline{g_8}(Y), the maximum and minimum multiplicity of the E8E_8 form; he computed them for infinite Brieskorn families and posed a consolidated list of open questions: which homology spheres admit definite spin boundings; whether finiteness of ds\mathfrak{ds} forces an E8E_8-bounding; when the sharp comparisons with the Ozsváth–Szabó correction term dd, the Neumann–Siebenmann invariant μˉ\bar\mu, and the Bohr–Lee invariants m,m‾m,\overline m hold; bounding-genus inequalities for explicit Brieskorn families equivalent to instances of Matsumoto's (11/8)-conjecture; the constructive problem of producing E8E_8-boundings; additivity under connected sum; and an a priori bound on the fiber-minus-section classes k[f]−[s]k[f]-[s] in elliptic surfaces E(n)E(n) representable by embedded 2-spheres. One strict-inequality facet was resolved affirmatively by Aceto–Golla–Larson (2017); the characterization, (11/8)-linked, constructive, and additivity questions remain open.

Background

Let YY be an integral homology 3-sphere, i.e. a closed oriented 3-manifold with the same integer homology as S3S^3. Every 3-manifold bounds smooth spin 4-manifolds, but whether YY bounds one whose intersection form QXQ_X (the unimodular symmetric bilinear form on H2(X;Z)H_2(X;\mathbb{Z})) is definite, meaning b2(X)=∣σ(X)∣b_2(X)=|\sigma(X)|, is a subtle question controlled by gauge theory. A spin structure (w2(X)=0w_2(X)=0) forces QXQ_X to be even (all self-intersections even), so the intersection form of a homologically 1-connected (connected with H1(X)=0H_1(X)=0) definite spin bounding of a homology sphere is an even definite unimodular lattice, whose rank is divisible by 8. Such lattices are not unique beyond rank 8: besides the E8E_8 lattice (unique in rank 8), rank 16 also admits D16+D_{16}^+, rank 24 admits the 24 Niemeier lattices, and the number grows rapidly with rank. Following Tange, a definite spin bounding whose form is a multiple ±nE8\pm nE_8 is called an E8E_8-bounding.

The classical constraints are: Donaldson's diagonalization theorem (a closed smooth definite 4-manifold has diagonal form, so no closed definite form can be E8E_8; it also implies a homology sphere cannot admit both a positive- and a negative-definite spin bounding, which makes Tange's sign invariant ϵ(Y)∈{1,−1,0,∞}\epsilon(Y)\in\{1,-1,0,\infty\} well defined); the Ozsváth–Szabó correction term d(Y)d(Y), a Z\mathbb{Z}-valued homology-cobordism invariant from Heegaard Floer homology, which for a spin negative-definite bounding XX gives b2(X)≤4d(Y)b_2(X)\le 4d(Y); the Neumann–Siebenmann invariant μˉ\bar\mu of Seifert homology spheres, for which Ue proved b2(X)≡−8μˉ(Y)(mod16)b_2(X)\equiv -8\bar\mu(Y)\pmod{16} together with explicit rank bounds; and Matsumoto's (11/8)-conjecture — still open — which states that a closed spin 4-manifold with intersection form 2k(−E8)⊕lH2k(-E_8)\oplus lH (with HH the hyperbolic plane) must satisfy l≥3∣k∣l\ge 3|k|; Furuta's 10/8 theorem, which gives only b2(X)≥108∣σ(X)∣+2b_2(X)\ge\frac{10}{8}|\sigma(X)|+2 (i.e. l≥2∣k∣+1l\ge 2|k|+1 in this normalization), remains the best general result toward it.

Tange (2016) introduced, for a homology 3-sphere YY, the invariants ds(Y)\mathfrak{ds}(Y) and ds‾(Y)\overline{\mathfrak{ds}}(Y) — the maximum and minimum of b2(X)/8b_2(X)/8 over homologically 1-connected definite spin boundings — and the E8E_8-genera g8(Y)g_8(Y) and g8‾(Y)\overline{g_8}(Y) — the maximum and minimum ∣n∣|n| over E8E_8-boundings with QX=nE8Q_X=nE_8 (each set to +∞+\infty when no such bounding exists; note the unbarred variant is the maximum). Furuta's inequality gives ds(Y)≤9ds‾(Y)+8\mathfrak{ds}(Y)\le 9\overline{\mathfrak{ds}}(Y)+8 whenever ds‾(Y)<ds(Y)\overline{\mathfrak{ds}}(Y)<\mathfrak{ds}(Y), and ∣Y∣≥ds(Y)+1|Y|\ge\mathfrak{ds}(Y)+1 whenever ds(Y)\mathfrak{ds}(Y) is even, where ∣Y∣=min⁡{n∣∂X=Y, QX=nH}|Y|=\min\{n\mid \partial X=Y,\ Q_X=nH\} is the bounding genus, defined when the Rokhlin invariant μ(Y)=σ(W)/8 mod 2\mu(Y)=\sigma(W)/8\bmod 2 (for any spin bounding WW) vanishes; the conjectured inequality ∣Y∣≥32ds(Y)|Y|\ge\frac{3}{2}\mathfrak{ds}(Y) is equivalent to the (11/8)-conjecture. The paper also relates ds\mathfrak{ds} to the Bohr–Lee invariants, m(Y)m(Y) and m‾(Y)\overline m(Y), defined as the maximum and minimum of 54σ(X)−b2(X)\frac54\sigma(X)-b_2(X) over spin boundings XX of YY (with σ\sigma the signature). Among its computations: ds=n\mathfrak{ds}=n for the four Brieskorn families Σ(4n−2,4n−1,8n−3)\Sigma(4n-2,4n-1,8n-3), Σ(4n−1,4n,8n−1)\Sigma(4n-1,4n,8n-1), Σ(4n−2,4n−1,8n2−4n+1)\Sigma(4n-2,4n-1,8n^2-4n+1), and Σ(4n−1,4n,8n2−1)\Sigma(4n-1,4n,8n^2-1), where Σ(a,b,c)\Sigma(a,b,c) is the Brieskorn homology sphere given as the link of the complex surface singularity xa+yb+zc=0x^a+y^b+z^c=0; g8=1g_8=1 for Mn=Σ(2,3,6n−1)#(−Σ(2,3,6n−5))M_n=\Sigma(2,3,6n-1)\#(-\Sigma(2,3,6n-5)); and g8(Y2k+1−)=1g_8(Y^-_{2k+1})=1 for 0≤k≤120\le k\le 12 and k=14k=14, for the family of Brieskorn spheres Yn−:=Σ(2,3,6n−1)Y^-_n:=\Sigma(2,3,6n-1) (so Y1−=Σ(2,3,5)Y^-_1=\Sigma(2,3,5), the Poincaré sphere). These last E8E_8-boundings come from explicit handle decompositions embedded in the elliptic surface E(1)E(1) (the complex surface fibered over S2S^2 with torus fibers and 12 singular fibers, diffeomorphic to CP2#9CP‾2\mathbb{C}P^2\#9\overline{\mathbb{C}P}^2), with complements the standard simply connected pieces known as Gompf nuclei; as a by-product, the class ak=k[f]−[s]a_k=k[f]-[s] (fiber class minus section class, ak2=−2k−1a_k^2=-2k-1) is represented by a smoothly embedded 2-sphere in E(1)E(1) for those same kk. The paper compares this with Finashin–Mikhalkin's theorem that E(2)E(2), the K3 surface, contains an embedded sphere of square −86-86, which implies k[f]−[s]∈H2(E(2))k[f]-[s]\in H_2(E(2)) is spherical for k≤42k\le 42, and with Li–Li's computation of smooth minimal genera for all classes of square >−(n+7)>-(n+7) in CP2#nCP‾2\mathbb{C}P^2\#n\overline{\mathbb{C}P}^2 for n≤9n\le 9. Section 5 of the paper (together with Question 3.1) then poses the consolidated question list stated below.

Problem Statement

The problem is the consolidated research program posed in Section 5 (with its auxiliary Question 3.1) of Tange's paper. The common objective is to characterize the definite spin and E8E_8-boundings of integral homology 3-spheres — existence, extremal sizes, comparison with the classical gauge-theoretic invariants, behavior under connected sum — together with the constructive question of producing such boundings and the embedded-sphere question extracted from the paper's constructions. The numbered questions below are independent. Numbering follows the published version (arXiv numbers in parentheses where they differ):

(Q5.1) For an integral homology 3-sphere YY: (1) determine when YY admits a homologically 1-connected definite spin bounding, i.e. when ds(Y)<∞\mathfrak{ds}(Y)<\infty; (2) if ds(Y)<∞\mathfrak{ds}(Y)<\infty, must YY admit an E8E_8-bounding, i.e. can the bounding always be chosen with intersection form a multiple of ±E8\pm E_8 rather than another even definite unimodular lattice such as D16+D_{16}^+ or a Niemeier lattice? (3) determine when the equalities m(−Y)/2=ds(Y)m(-Y)/2=\mathfrak{ds}(Y) and m‾(−Y)/2=ds‾(Y)\overline{m}(-Y)/2=\overline{\mathfrak{ds}}(Y) hold for the Bohr–Lee invariants m,m‾m,\overline m.

(Q5.2, remaining part) Does there exist a homology 3-sphere YY with ds(Y)≠g8(Y)\mathfrak{ds}(Y)\ne g_8(Y) or ds‾(Y)≠g8‾(Y)\overline{\mathfrak{ds}}(Y)\ne\overline{g_8}(Y) — that is, a definite spin bounding whose lattice is not an E8E_8-multiple, with no E8E_8-bounding of matching size? (The companion strict-inequality question — whether g8‾(Y)<g8(Y)\overline{g_8}(Y)<g_8(Y) can occur — was answered affirmatively by Aceto–Golla–Larson and is no longer part of what remains.)

(Q5.3) For a Brieskorn homology 3-sphere YY with 4d(Y)=−8μˉ(Y)>04d(Y)=-8\bar\mu(Y)>0: does the maximal even definite spin bounding attain the Ozsváth–Szabó bound, i.e. is 8 ds(Y)=4d(Y)8\,\mathfrak{ds}(Y)=4d(Y) (equivalently ds(Y)=d(Y)/2\mathfrak{ds}(Y)=d(Y)/2)?

(Q5.4) If a Brieskorn homology 3-sphere has finite E8E_8-genus, is g8(Y)=g8‾(Y)g_8(Y)=\overline{g_8}(Y), i.e. is the E8E_8-multiplicity unique?

(Q5.5, arXiv Problem 5.1) Do the (11/8)-conjecture-linked bounding-genus inequalities hold for the four explicit infinite Brieskorn families — the even-parameter subfamilies of the four families with ds=n\mathfrak{ds}=n listed above, i.e. those with ds=2n\mathfrak{ds}=2n: ∣Σ(8n−2,8n−1,16n−3)∣≥3n|\Sigma(8n-2,8n-1,16n-3)|\ge 3n, ∣Σ(8n−1,8n,16n−1)∣≥3n|\Sigma(8n-1,8n,16n-1)|\ge 3n, ∣Σ(8n−2,8n−1,32n2−8n+1)∣≥3n|\Sigma(8n-2,8n-1,32n^2-8n+1)|\ge 3n, and ∣Σ(8n−1,8n,32n2−1)∣≥3n|\Sigma(8n-1,8n,32n^2-1)|\ge 3n? (Here ∣⋅∣|\cdot| is the bounding genus; the failure of any one inequality would refute Matsumoto's (11/8)-conjecture.)

(Q5.6, arXiv Question 5.5) Do these same Brieskorn spheres admit E8E_8-boundings with g8=2ng_8=2n?

(Q5.7, arXiv Question 5.6) For the classes ak=k[f]−[s]∈H2(E(n))a_k=k[f]-[s]\in H_2(E(n)) (fiber class minus section class in the elliptic surface E(n)E(n)): is there an a priori upper bound on kk for which aka_k can be represented by a smoothly embedded S2S^2? (Known: k≤12k\le 12 and k=14k=14 in E(1)E(1); k≤42k\le 42 in E(2)E(2).)

(Q5.8, arXiv Question 5.7) For homology 3-spheres X1,X2X_1,X_2 with ds(Xi)<∞\mathfrak{ds}(X_i)<\infty and ds~(Y):=ϵ(Y)ds(Y)\tilde{\mathfrak{ds}}(Y):=\epsilon(Y)\mathfrak{ds}(Y), characterize when the signed additivity ds~(X1)+ds~(X2)=ds~(X1#X2)\tilde{\mathfrak{ds}}(X_1)+\tilde{\mathfrak{ds}}(X_2)=\tilde{\mathfrak{ds}}(X_1\#X_2) holds (the paper records the nontrivial example X1=Σ(2,3,17)X_1=\Sigma(2,3,17), X2=Σ(2,3,13)#(−Σ(2,3,17))X_2=\Sigma(2,3,13)\#(-\Sigma(2,3,17)) and expects additivity to be rare).

(Problem 5.1, arXiv Problem 5.2) Find more general constructions producing positive or negative E8E_8-boundings for many homology 3-spheres.

(Q3.1) In the plumbing 4-manifold SkS_k with intersection form −E8⊕H-E_8\oplus H and boundary Y2k+1−=Σ(2,3,12k+5)Y^-_{2k+1}=\Sigma(2,3,12k+5) (where Yn−:=Σ(2,3,6n−1)Y^-_n:=\Sigma(2,3,6n-1)): can a separating homology 3-sphere Y⊂SkY\subset S_k that splits the form as −E8⊕H-E_8\oplus H (i.e. the HH-summand piece XX with ∂X=Y\partial X=Y) be taken so as to bound an acyclic 4-manifold — that is, can such a YY be taken with trivial class in the homology cobordism group ΘZ3\Theta^3_{\mathbb{Z}} (the abelian group of integral homology 3-spheres modulo homology cobordism, i.e. modulo together bounding a homology product Y×[0,1]Y\times[0,1])? The source notes this question is equivalent to ds(Y2k+1−)=1\mathfrak{ds}(Y^-_{2k+1})=1 for any kk.

References

  1. Motoo Tange, The E8-boundings of homology spheres and negative sphere classes in E(1), Topology and its Applications 202 (2016) 160–182, DOI: 10.1016/j.topol.2015.12.067, https://doi.org/10.1016/j.topol.2015.12.067 (author's preprint arXiv:1408.5528, https://arxiv.org/abs/1408.5528)
  2. Paolo Aceto, Marco Golla, Kyle Larson, Embedding 3-manifolds in spin 4-manifolds, Journal of Topology 10 (2017) 301–323, DOI: 10.1112/topo.12010, https://doi.org/10.1112/topo.12010 (preprint arXiv:1607.06388, https://arxiv.org/abs/1607.06388)
  3. Christopher Scaduto, On definite lattices bounded by a homology 3-sphere and Yang–Mills instanton Floer theory, Geometry & Topology 28 (2024) 1587–1628, DOI: 10.2140/gt.2024.28.1587, https://doi.org/10.2140/gt.2024.28.1587 (preprint arXiv:1805.07875, https://arxiv.org/abs/1805.07875)
  4. Christopher Scaduto, Niemeier lattices, smooth 4-manifolds and instantons, Mathematische Annalen 379 (2021) 549–568, DOI: 10.1007/s00208-020-02060-y, https://doi.org/10.1007/s00208-020-02060-y (preprint arXiv:1808.10321, https://arxiv.org/abs/1808.10321)
  5. Motoo Tange, Homology spheres with E_8-fillings and arbitrarily large correction terms, Indiana University Mathematics Journal 70 (2021) 985–1002, DOI: 10.1512/iumj.2021.70.8453, https://doi.org/10.1512/iumj.2021.70.8453 (preprint arXiv:1811.11831, https://arxiv.org/abs/1811.11831)
  6. Marco Golla, Christopher Scaduto, On definite lattices bounded by integer surgeries along knots with slice genus at most 2, Transactions of the American Mathematical Society 372 (2019) 7805–7829, DOI: 10.1090/tran/7823, https://doi.org/10.1090/tran/7823
  7. Soheil Azarpendar, Negative-definite spin filling and branched double covers, Algebraic & Geometric Topology 26 (2026) 1655–1680, DOI: 10.2140/agt.2026.26.1655, https://doi.org/10.2140/agt.2026.26.1655 (preprint arXiv:2308.08022, https://arxiv.org/abs/2308.08022)
  8. M. Furuta, Monopole equation and the 11/8-conjecture, Mathematical Research Letters 8 (2001) 279–291, DOI: 10.4310/MRL.2001.v8.n3.a5, https://doi.org/10.4310/MRL.2001.v8.n3.a5
  9. Peter Ozsváth, Zoltán Szabó, Absolutely graded Floer homologies and intersection forms for four-manifolds with boundary, Advances in Mathematics 173 (2003) 179–261, DOI: 10.1016/S0001-8708(02)00030-0, https://doi.org/10.1016/S0001-8708(02)00030-0
  10. C. Bohr, R. Lee, Homology cobordism and classical knot invariants, Commentarii Mathematici Helvetici 77 (2002) 363–382, DOI: 10.1007/s00014-002-8344-0, https://doi.org/10.1007/s00014-002-8344-0
  11. Paolo Aceto, Duncan McCoy, JungHwan Park, Definite fillings of lens spaces, Journal of Differential Geometry 131 (2025), DOI: 10.4310/jdg/1755541518, https://doi.org/10.4310/jdg/1755541518 (preprint arXiv:2208.02586, https://arxiv.org/abs/2208.02586)
  12. Ali Naseri Sadr, Classification of lattices bounded by large surgeries of knots, Mathematical Research Letters 32 (2025) 1993–2008, DOI: 10.4310/mrl.260123174909, https://doi.org/10.4310/mrl.260123174909 (preprint arXiv:2404.14633, https://arxiv.org/abs/2404.14633)
  13. Nobuo Iida, Anubhav Mukherjee, Masaki Taniguchi, An adjunction inequality for the Bauer–Furuta type invariants, with applications to sliceness and 4-manifold topology, Advances in Mathematics 466 (2025) 110134, DOI: 10.1016/j.aim.2025.110134, https://doi.org/10.1016/j.aim.2025.110134 (preprint arXiv:2102.02076, https://arxiv.org/abs/2102.02076)
  14. Sergey Finashin, Grigory Mikhalkin, A (−86)-Sphere in the K3 Surface, Turkish Journal of Mathematics 21 (1997) 129–131, https://journals.tubitak.gov.tr/math/vol21/iss1/13
  15. Bang-He Li, Tian-Jun Li, Smooth minimal genera for small negative classes in CP2#nCP2 with n≤9, Topology and its Applications 132 (2003) 1–15, DOI: 10.1016/S0166-8641(02)00357-7, https://doi.org/10.1016/S0166-8641(02)00357-7