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Section 1

Introduction

All varieties are defined over ℂ\mathbb C. A smooth projective variety is Fano if its anticanonical divisor is ample. The classification of smooth Fano threefolds by Iskovskikh, Mori and Mukai gives 105105 deformation families; we use the usual numbering, whose first integer is the Picard rank. Determining their K-polystable members is a finer problem, related to the existence of Kähler–Einstein metrics and not constant in every deformation family. We consider the following families; see [3]. Each family is treated in a separate part.

  1. In Family 1.9, X⊂ℙ11X\subset\mathbb P^{11} is a codimension-two linear section of the five-dimensional adjoint G2G_2-variety in ℙ13\mathbb P^{13}. It is a prime Fano threefold of genus ten, with Pic(X)=ℤ[−KX]\operatorname{Pic}(X)=\mathbb Z[-K_X] and (−KX)3=18(-K_X)^3=18. We prove K-stability for every smooth member; the final assembly is in Section ??.

  2. In Family 1.10, XX is the zero locus of three sections of ⋀2𝒰∨\bigwedge^2\mathcal U^\vee on Gr(3,7)\operatorname{Gr}(3,7), where 𝒰\mathcal U is the tautological rank-three bundle. It is a prime Fano threefold of genus twelve with (−KX)3=22(-K_X)^3=22. Part ?? contains a symmetric counterexample to the unrestricted anticanonical-singularity formulation of Donaldson’s conjecture in [3, Conjecture 7.1], and partial classification results, including local estimates from ordinary point and line blow-ups, a nodal reduction for terminal Gorenstein degenerations, an exclusion of a nonterminal boundary family, strict monomial-valuation estimates, and an exact ribbon description of the section ring under the transverse width-two hypotheses.

  3. In Family 2.5, XX is the blow-up of a smooth cubic threefold V⊂ℙ4V\subset\mathbb P^4 along a smooth plane cubic C=V∩ℙ2C=V\cap\mathbb P^2. The hyperplanes containing this plane give a cubic-surface fibration X→ℙ1X\to\mathbb P^1, and (−KX)3=12(-K_X)^3=12.

  4. In Family 2.9, XX is the blow-up of ℙ3\mathbb P^3 along a smooth curve of degree seven and genus five whose ideal sheaf is generated by three cubics. The cubic net gives a conic bundle X→ℙ2X\to\mathbb P^2, and (−KX)3=16(-K_X)^3=16.

  5. In Family 2.10, XX is the blow-up of a smooth complete intersection of two quadrics V⊂ℙ5V\subset\mathbb P^5 along the smooth elliptic quartic C=V∩ℙ3C=V\cap\mathbb P^3. The hyperplanes containing this linear subspace give a quartic del Pezzo fibration X→ℙ1X\to\mathbb P^1, and (−KX)3=16(-K_X)^3=16.

  6. In Family 2.11, XX is the blow-up of a smooth cubic threefold V⊂ℙ4V\subset\mathbb P^4 along a line ℓ\ell. Projection from the line gives a conic bundle X→ℙ2X\to\mathbb P^2, and (−KX)3=18(-K_X)^3=18. Both possible normal bundles, 𝒪ℓ⊕2\mathcal O_\ell^{\oplus2} and 𝒪ℓ(1)⊕𝒪ℓ(−1)\mathcal O_\ell(1)\oplus\mathcal O_\ell(-1), are included.

  7. In Family 2.12, XX is a smooth complete intersection of three divisors of bidegree (1,1)(1,1) in ℙ3×ℙ3\mathbb P^3\times\mathbb P^3. Each projection blows up a smooth nonhyperelliptic sextic curve of genus three, and (−KX)3=20(-K_X)^3=20.

  8. In Family 2.13, XX is the blow-up of a smooth quadric Q⊂ℙ4Q\subset\mathbb P^4 along a smooth sextic curve of genus two cut out on QQ by quadrics. The quadrics give a conic bundle X→ℙ2X\to\mathbb P^2, and (−KX)3=20(-K_X)^3=20.

  9. In Family 2.14, XX is the blow-up of the quintic del Pezzo threefold V5⊂ℙ6V_5\subset\mathbb P^6 along the smooth elliptic quintic cut out by two hyperplanes. Their pencil gives a quintic del Pezzo fibration X→ℙ1X\to\mathbb P^1, and (−KX)3=20(-K_X)^3=20.

  10. In Family 2.16, XX is the blow-up of a smooth intersection of two quadrics V4⊂ℙ5V_4\subset\mathbb P^5 along a smooth conic. Projection from the plane of the conic gives a conic bundle X→ℙ2X\to\mathbb P^2, and (−KX)3=22(-K_X)^3=22.

  11. In Family 2.17, XX is the blow-up of ℙ3\mathbb P^3 along a smooth elliptic quintic. Its second contraction is the blow-up of a smooth quadric along a smooth elliptic normal quintic, and (−KX)3=24(-K_X)^3=24. Write E,E′E,E' for the exceptional divisors over ℙ3\mathbb P^3 and the quadric, respectively. For a point p∈Sing(E∩E′)p\in\mathop{\mathrm{Sing}}(E\cap E'), let ℓ′p\ell'_p be the fibre of E′E' through pp, and put ΣX={p∈Sing(E∩E′):E|ℓ′p=3p}\Sigma_X=\{p\in\mathop{\mathrm{Sing}}(E\cap E'):E|_{\ell'_p}=3p\}.

  12. In Family 2.20, XX is the blowup of V5V_5 along a smooth twisted cubic. Projection from its span gives a conic bundle over ℙ2\mathbb P^2, and (−KX)3=26(-K_X)^3=26. Its K-stable, K-polystable and strictly K-semistable members are classified in Part XI.

  13. In Family 3.2, XX is a divisor of class 2ξ+𝒪(2,3)2\xi+\mathcal O(2,3) in ℙℙ1×ℙ1(𝒪⊕𝒪(−1,−1)⊕2)\mathbb P_{\mathbb P^1\times\mathbb P^1} (\mathcal O\oplus\mathcal O(-1,-1)^{\oplus2}), where ξ\xi is the tautological class and its restriction to XX is irreducible. The projection is a conic bundle with cubic and sextic del Pezzo pencils, and (−KX)3=14(-K_X)^3=14.

  14. In Family 3.5, XX is the blow-up of ℙ1×ℙ2\mathbb P^1\times\mathbb P^2 along the graph of a degree-five morphism η:ℙ1→ℙ1\eta:\mathbb P^1\to\mathbb P^1, with the source embedded as a smooth conic in ℙ2\mathbb P^2. Here (−KX)3=20(-K_X)^3=20. The stability of its smooth members is classified below.

  15. In Family 3.6, XX is the blow-up of ℙ3\mathbb P^3 along a smooth elliptic quartic and a disjoint line. The plane and quadric pencils give del Pezzo fibrations of degrees five and six, and their product is a conic bundle over ℙ1×ℙ1\mathbb P^1\times\mathbb P^1. Here (−KX)3=22(-K_X)^3=22.

  16. In Family 3.7, XX is the blow-up of a smooth divisor V⊂ℙ2×ℙ2V\subset\mathbb P^2\times\mathbb P^2 of bidegree (1,1)(1,1) along a smooth complete intersection of two members of |𝒪V(1,1)||\mathcal O_V(1,1)|. The resulting pencil consists of sextic del Pezzo surfaces, and (−KX)3=24(-K_X)^3=24.

  17. In Family 3.8, XX is the blow-up of ℙ1×ℙ2\mathbb P^1\times\mathbb P^2 along the graph of a degree-four morphism ℙ1→ℙ1\mathbb P^1\to\mathbb P^1, with its source embedded as a smooth conic in ℙ2\mathbb P^2. Equivalently, the centre is the intersection of divisors of bidegrees (0,2)(0,2) and (1,2)(1,2). Here (−KX)3=24(-K_X)^3=24. Its K-polystable members are classified in Part XVI.

Theorem 1.1. Every smooth Fano threefold in Families 1.9, 2.5, 2.9, 2.10, 2.11, 2.12, 2.13, 2.14, 2.16, 2.17, 3.2, 3.6 and 3.7 is K-stable.

Every smooth member XX of Families 2.20, 3.5 and 3.8 is K-semistable. Their K-stable and K-polystable members are characterized as follows.

  1. In Family 2.20, let U=⟨f,g⟩U=\langle f,g\rangle be the pencil of binary quartics corresponding to the twisted cubic, as in Section 69, and let wU=fxgy−fygxw_U=f_xg_y-f_yg_x be its Wronskian sextic. Then XX is K-stable if and only if every root of wUw_U has multiplicity at most two. It is K-polystable if and only if this holds or wUw_U has two distinct triple roots.

  2. In Families 3.5 and 3.8, let η:ℙ1→ℙ1\eta:\mathbb P^1\to\mathbb P^1 be the morphism whose graph is the blow-up centre, of degree five and four, respectively. Then XX is K-stable if and only if η\eta has no totally ramified point. It is K-polystable if and only if η\eta has either no totally ramified point or two such points.

In each of these three families there is, up to isomorphism, exactly one K-polystable member which is not K-stable. The strictly K-semistable members are precisely those with exactly one triple root in (1), or exactly one totally ramified point in (2).

Proof. The universal K-stability assertions for Families 1.9, 2.11, 2.13, 2.16, 2.17, 3.2, 3.6 and 3.7 are respectively Theorems ??, 23.1, 38.1, 53.1, 61.1, 83.1, 103.1 and 108.1. For Family 2.5, combine Lemma 7.1 with Theorems 7.2 and 7.3. Family 2.9 follows from Proposition 10.2. The proofs for Families 2.10, 2.12 and 2.14 are completed in Sections 21, 37 and 52, respectively.

The three classifications are Theorems 69.1, 101.1 and 128.1. ◻

1.1 Description of the results

Every smooth Fano threefold in Family 1.9 is K-stable. We prove δp(X)≥6/5\delta_p(X)\ge6/5 away from all lines and δp(X)≥72/71\delta_p(X)\ge72/71 at every point on an ordinary line, and exclude all curve centres. The remaining points lie on special lines. At a marked point with nonzero quadratic coefficient μ\mu, an ordinary point extraction gives δp(X)≥9/8\delta_p(X)\ge9/8. When μ=0\mu=0, the weight-(1,2,2)(1,2,2) extraction has expected order 287/72287/72. A surface estimate treats one sector of valuations. For the other sector, we blow up the strict transform of the line and apply adjunction with both exceptional divisors. A normal-jet bound makes the boundary effective, and the resulting inequality AX(v)−(288/245)SX(v)≥11v(a)/35>0A_X(v)-(288/245)S_X(v)\ge11v(a)/35>0 completes the proof. These point extractions require no threefold Zariski decomposition.

We prove K-stability of every smooth Fano threefold in Mori–Mukai Families 2.5, 2.9, 2.10, 2.11, 2.12, 2.13, 2.14, 2.16, 2.17, 3.2, 3.6 and 3.7. We obtain δ(X)≥96/95\delta(X)\ge96/95 in Family 2.9, δ(X)≥320/319\delta(X)\ge320/319 in Family 2.13, and δ(X)≥176/171\delta(X)\ge176/171 in Family 2.16. The proofs use Abban–Zhuang refinement on del Pezzo fibres, cubic surfaces, and exceptional surfaces of point or curve extractions. We compute expected vanishing orders from filtered section rings or bound them by explicit spaces containing the refined sections. Each family is treated in a separate part, after Part I, which gives the definitions, adjunction tools and worked examples. In Family 2.11 we treat both normal-bundle types of the blown-up line. Weak cubic sections handle the special reduced fibre. At the remaining smooth tangencies, a weight-(1,1,2)(1,1,2) point extraction and a valuation centred on the ramification ruling give the exact local threshold 216/167216/167. Double conic fibres have local threshold at least 144/127144/127. For Family 2.12, the published reduction to points of the intersection of the two exceptional divisors is completed using ordinary point blow-ups and a weight-(2,1,1)(2,1,1) extraction. Exact initial rings and monomial moment certificates control all tangent configurations. The weighted calculations identify the actual refined section spaces and do not require a Zariski decomposition on an extracted threefold. For Family 2.13, quartic del Pezzo sections treat reduced conic fibres. Blowing up the node on such a section gives the bound 160/159160/159. For double fibres, the actual weighted refinement consists of ideal-power series for a length-two subscheme of ℙ1×ℙ1\mathbb P^1\times\mathbb P^1. A degeneration preserving the different, together with an explicit correction for the dimensions of these series, gives the bound 320/319320/319. For Family 2.14, the quintic del Pezzo pencil reduces the proof to four types of singular points and to lines on singular fibres. We treat both normal-bundle types of lines and both positions of their intersection with the elliptic quintic. The refined threshold can equal one in the A3A_3 case; a positive discrepancy term completes that case. For Family 2.16, the known reduced-fibre estimates leave double lines. Their weighted extraction has expected order 57/2257/22. The refined series consists of powers of the ideal of one point on the different, and a degeneration preserving that different gives the local bound 88/8588/85 on every double fibre. An independent GIT proof for Family 2.16 computes the CM class 6ζ+20ξ+66η6\zeta+20\xi+66\eta, proves stability of every smooth pair by the Hilbert–Mumford criterion, and uses relative reconstruction and CM-degree minimization to obtain K-stability.

For Family 2.17, two line extractions reduce the problem to a finite triple-contact locus. A weight-(1,1,2)(1,1,2) point extraction at every remaining point has expected order 29/829/8. Its actual refined section ring is identified by an integral initial divisor in a symplectic flag variety. A second degeneration gives complete binary spaces on ℙ(1,1,2)\mathbb P(1,1,2), whose moments yield δp(X)≥64/59\delta_p(X)\ge64/59. This completes the proof for all smooth members, without a threefold Zariski decomposition on the weighted point blow-up. For Families 3.6 and 3.2, weighted curve extractions above double conics have expected orders 243/88243/88 and 135/56135/56, respectively. Exact section spaces give refined thresholds at least one, with the different retained. The positive discrepancy remainders complete both proofs, including the special double-conic configurations. Every smooth member of Family 3.5 is K-semistable. It is K-stable exactly when its associated degree-five map has no totally ramified point; the K-polystable members are also classified. For Family 3.7, sextic fibres and quintic sections reduce the proof to finitely many point configurations. Exact section algebras on ordinary and weighted point blow-ups complete the proof for every smooth member.

For Family 2.20 we identify every nonclosed smooth GIT orbit by a pencil of binary quartics and its Wronskian sextic. These give a one-parameter collection of strictly K-semistable threefolds with a common K-polystable smooth limit. Abban–Zhuang estimates exclude every divisor centre and every point on a smooth conic-bundle fibre. Exact singular-fibre surface calculations isolate the remaining valuative problem. At every double fibre the weighted extraction has expected order 297/104297/104 and discrepancy three. We determine its complete refined series by multiplication and a dimension count. Ordinary and weighted surface blowups prove δp(X)≥104/99\delta_p(X)\ge104/99 along every double fibre of a GIT-stable member. For reduced fibres, two flops give the expected order 43/2643/26 for the extraction of a component. Its complete refinement yields the same local bound along ordinary components when the fibre node is outside the original exceptional divisor. Negative-section flags and a retained discrepancy treat special-line components. The possible nonpositive-beta centres on a GIT-stable member reduce to at most three fibre nodes on the original exceptional divisor. Their ordinary point extractions have SX(J)=11/4<3=AX(J)S_X(J)=11/4<3=A_X(J). We identify their complete initial section algebras in every degree. Surface flags, including an extra fixed line in the degenerate-conic case, give δp(X)≥104/103\delta_p(X)\ge104/103 at all remaining nodes. This proves that a smooth member of Family 2.20 is K-stable exactly when its quartic pencil is GIT-stable, and K-polystable exactly when that pencil is GIT-polystable.

For Family 3.8, a smooth member is determined by a basepoint-free pencil of binary quartics. It is K-stable exactly when the associated degree-four morphism has no totally ramified point. There is one K-polystable member which is not K-stable; all other smooth members are strictly K-semistable and are parametrized by ℙ(2,3)\mathbb P(2,3). The proof treats every singular del Pezzo fibre by explicit surface flags and point or curve extractions. The actual refined sections, or complete containing series with the same asymptotic dimension, replace Zariski decompositions on the extracted threefolds.

For Family 1.10, we construct a symmetric counterexample to the unrestricted anticanonical-singularity formulation of Donaldson’s conjecture, stated as Conjecture 7.1 in The Calabi Problem for Fano Threefolds. A small deformation of the Mukai–Umemura threefold in the stable binary-octic direction uv(u6+v6)uv(u^6+v^6) is K-stable with finite automorphism group and has two points on no line exchanged by an 𝔖3\mathfrak S_3-action. Each point has an anticanonical divisor with exact germ y2=x3+t4xy^2=x^3+t^4x; the involution exchanges the two divisors. We compute a central pencil, impose j=1728j=1728 at a simple root, and prove equivariant persistence. The additional hypothesis that a bad point lies on a line still implies failure of K-stability. We identify the exact bad-point-on-line locus with the locus of members having a special line meeting no other line, and with the complement of affine GIT-stable Mukai nets. In particular this locus is closed, and every member on it has δ(X)=1\delta(X)=1. The line-incidence and closed-net revisions are therefore equivalent. We prove the revised criterion near Mukai–Umemura; the global implication from GIT stability to K-stability remains open. We also obtain the following partial classification results. Nonclosed smooth Mukai-net orbits yield strictly K-semistable members with the prescribed anticanonical singularity. The ordinary point blow-up gives δp(X)≥264/259\delta_p(X)\ge264/259 at every point on no line, including all nonordinary conic flops. We give sharper bounds according to the singularities of the associated cubic surface, and exhibit a smooth pointed member with one double conic parameter. For ordinary lines we classify all resolving-surface configurations and compute their fibre flags. In particular, δp(X)≥88/83\delta_p(X)\ge88/83 if exactly one line passes through pp and it is ordinary. The same bound holds along lines with smooth or nodal associated quintic surface and in further configurations treated by a point extraction on the exceptional surface. By changing the chosen line, the surface estimates reduce the points away from special lines to two explicit incidence configurations. A new point-jet estimate settles the directed three-line cycle for all divisorial valuations, giving δp(X)≥270336/269791\delta_p(X)\ge270336/269791. A weighted extraction also gives a strict bound along the special lines satisfying the explicit hypotheses of Definition ??. This includes all ramification cases on their exceptional surfaces. The proof retains actual fixed parts, differents and total-pullback corrections throughout. We also prove that every special test configuration with factorial terminal central fibre has zero Donaldson–Futaki invariant. Every terminal Gorenstein limit is nodal, with divisor-class rank one plus its number of nodes. We exclude all four one-nodal families as smooth test-configuration limits. An explicit fixed-point obstruction excludes the nonterminal boundary family obtained from smooth bidegree-(4,1)(4,1) curves on a quadric in ℙ3\mathbb P^3. For the two exceptional ordinary-line configurations we obtain AX/SX≥132/125A_X/S_X\ge132/125 and AX/SX≥264/229A_X/S_X\ge264/229, respectively, for valuations monomial in coordinates straightening the lines. Under the transverse width-two hypotheses, the full anticanonical ring is described by powers of the ideal of a rational ribbon on a smooth quadric. The special-line links have four conductor configurations. Double conductor contact on 𝔽1\mathbb F_1 now has δp(X)≥88/83\delta_p(X)\ge88/83 along the entire special line, with the infinitely near conditions retained. On the GIT-stable locus, the remaining local cases are the mutually width-three ordinary pair and the distinguished point in the 𝔽3\mathbb F_3 width-two case. These results do not complete the global classification for Family 1.10, which is not included in the Main Theorem.

The three classifications confirm the conjectures in [3, Sections 7.2, 7.5 and 7.6].

We also construct a counterexample to Donaldson’s conjecture in The Calabi Problem for Fano Threefolds [3, Conjecture 7.1]. It concerns smooth prime Fano threefolds of genus twelve and predicts K-polystability from the absence of certain singular anticanonical divisors, apart from the members admitting a torus action. Our example contradicts the necessary direction of that prediction.

Theorem 1.2. There exists a smooth K-stable threefold XX in Family 1.10 with finite automorphism group and an anticanonical divisor having the analytic singularity y2=x3+t4xy^2=x^3+t^4x. In particular, Donaldson’s conjecture in [3, Conjecture 7.1] is false as stated.

Proof. Theorem ?? constructs such threefolds as small nonzero deformations of the Mukai–Umemura threefold in the binary-octic direction uv(u6+v6)uv(u^6+v^6). Their automorphism groups are finite, so the torus alternative in the conjecture does not apply. ◻

The construction has an 𝔖3\mathfrak S_3-action exchanging two points on no line and two anticanonical divisors with the prescribed germs. A single such divisor already contradicts the conjecture. At these points the space of sections of weighted order at least six has dimension two, whereas the torus degeneration giving the known obstruction has dimension eight. Thus the analytic equation does not determine the global anticanonical filtration. Subsection ?? discusses possible revisions. Theorem ?? identifies the exact bad-point-on-line locus with the complement of affine GIT-stable Mukai nets and proves that it is closed. Every member of this locus has δ(X)=1\delta(X)=1. The line-incidence and closed-net conjectures are equivalent, and both hold near Mukai–Umemura. The global implication from a smooth GIT-stable net to a K-stable threefold remains unproved.

The valuative approach of Fujita and Li replaces test configurations by inequalities between log discrepancies and expected vanishing orders [18, 22]. The stability threshold, introduced through basis divisors and developed systematically by Blum–Jonsson [6], packages these inequalities in the invariant δ\delta. Its relation to K-stability and the existence of Kähler–Einstein metrics is described in [21]. Abban and Zhuang [4] developed refinement by admissible flags, allowing threefold estimates to be reduced to series on surfaces and curves. We use this method throughout.

Table 1 records the seventeen families for which a complete classification of K-polystable smooth members remained unresolved before the results of this paper, with the qualification concerning Family 3.5 below. Theorem 1.1 summarizes our results. The entry for Family 1.10 records partial results only; its global classification remains open. The geometric descriptions follow the classification in [3, Section 6]. All varieties and blow-up centres in the table are smooth, and the usual Fano conditions on the centres are understood.

In the table, V3⊂ℙ4V_3\subset\mathbb P^4 is a cubic, V4⊂ℙ5V_4\subset\mathbb P^5 is an intersection of two quadrics, V5⊂ℙ6V_5\subset\mathbb P^6 is a three-dimensional linear section of Gr(2,5)⊂ℙ9\operatorname{Gr}(2,5)\subset\mathbb P^9, and Q⊂ℙ4Q\subset\mathbb P^4 is a quadric. For Family 1.10, 𝒰\mathcal U is the tautological rank-three subbundle on Gr(3,7)\operatorname{Gr}(3,7). For Family 3.2, put π:ℬ=ℙℙ1×ℙ1(𝒪⊕𝒪(−1,−1)⊕2)→ℙ1×ℙ1,ξ=𝒪ℬ(1),\pi:\mathcal B=\mathbb P_{\mathbb P^1\times\mathbb P^1} \bigl(\mathcal O\oplus\mathcal O(-1,-1)^{\oplus2}\bigr) \longrightarrow\mathbb P^1\times\mathbb P^1, \qquad \xi=\mathcal O_{\mathcal B}(1), using the quotient convention, and let DD be the unique divisor in |ξ||\xi|.

Table 1. Families with an incomplete classification before the present results.
Family Geometric description This paper
1.9 Codimension-two linear section of the five-dimensional adjoint G2G_2-variety in ℙ13\mathbb P^{13}. Part ??
1.10 Zero locus of a section of (⋀2𝒰∨)⊕3(\bigwedge^2\mathcal U^\vee)^{\oplus3} on Gr(3,7)\operatorname{Gr}(3,7). Part ?? (partial)
2.5 Blow-up of V3V_3 along a plane cubic. Part II
2.9 Blow-up of ℙ3\mathbb P^3 along a degree-seven, genus-five curve whose ideal sheaf is generated by three cubics. Part III
2.10 Blow-up of V4V_4 along an elliptic quartic cut out by a ℙ3\mathbb P^3. Part IV
2.11 Blow-up of V3V_3 along a line. Part V
2.12 Complete intersection of three (1,1)(1,1)-divisors in ℙ3×ℙ3\mathbb P^3\times\mathbb P^3. Part VI
2.13 Blow-up of QQ along a genus-two sextic. Part VII
2.14 Blow-up of V5V_5 along an elliptic quintic cut out by two hyperplanes. Part VIII
2.16 Blow-up of V4V_4 along a conic. Part IX
2.17 Blow-up of QQ along an elliptic quintic. Part X
2.20 Blow-up of V5V_5 along a twisted cubic. Part XI
3.2 A divisor X∈|2ξ+π*𝒪(2,3)|X\in|2\xi+\pi^*\mathcal O(2,3)| in ℬ\mathcal B, with X∩DX\cap D irreducible. Part XII
3.5*3.5^{*} Blow-up of ℙ1×ℙ2\mathbb P^1\times\mathbb P^2 along a (5,2)(5,2)-curve embedded by projection to ℙ2\mathbb P^2. Part XIII
3.6 Blow-up of ℙ3\mathbb P^3 along a disjoint line and elliptic quartic. Part XIV
3.7 Blow-up of a (1,1)(1,1)-divisor W⊂ℙ2×ℙ2W\subset\mathbb P^2\times\mathbb P^2 along the intersection of two members of |𝒪W(1,1)||\mathcal O_W(1,1)|. Part XV
3.8 Blow-up of ℙ1×ℙ2\mathbb P^1\times\mathbb P^2 along the intersection of (0,2)(0,2)- and (1,2)(1,2)-divisors. Part XVI

*^{*}Family 3.5 is retained in this historical list; its smooth classification is proved in Part XIII. Denisova–Papazachariou’s announced manuscript is listed under “In Preparation”, with a PDF available upon request, on Papazachariou’s research page, consulted on 30 September 2026 [15]. We have not used that manuscript as a theorem. Part XIII proves K-semistability for every smooth member and K-stability whenever there is no totally ramified point, including all mixed fibres.

Abban–Zhuang prove K-stability for smooth prime Fano threefolds of degree at most 1616 in [44]; their argument does not cover degree 1818. The published proof of [23, Lemma 4.2] treats Family 1.9 under a fixed-point-free abelian symmetry hypothesis. Its multiplier-ideal argument excludes curve centres of degree at least two without using that symmetry. Xu–Zhuang still list the universal K-semistability assertion for Family 1.9 in [51, Problem 10], in the revision dated 1 June 2026.

Part ?? proves K-stability for every smooth member of Family 1.9. The exceptional divisor of an ordinary line blow-up has expected order 101/72101/72; the weighted extraction over a special line has expected order 43/1843/18. Surface flags and changes of projection line treat every point on an ordinary line. The special-line analysis reduces to marked points on higher-width special lines. At those points, two-divisor adjunction retains the positive term 11v(G)/1811v(G)/18 for valuations whose centres on the smooth model are contained in GG.

An ordinary point extraction gives δp(X)≥9/8\delta_p(X)\ge9/8 when the quadratic coefficient μ\mu is nonzero. If μ=0\mu=0, the actual initial sections of the weight-(1,2,2)(1,2,2) extraction split into binary spaces. Their fixed orders and full Hilbert mass give SX(F)=287/72S_X(F)=287/72 and a refined bound 144/119144/119 on C≠0C\ne0. The last valuations have centre P=[1:0:0]P=[1:0:0] on this extraction. The ordinary blowup of PP on FF has refined moment 115/72115/72, and its point moments on the required affine chart are at most 1/31/3. To lift these surface estimates to the threefold, we blow up the strict transform of the original line. The normal bundle gives ordF(s)≤m+4ordL(s)(0≠s∈H0(X,mH)).\operatorname{ord}_F(s)\le m+4\operatorname{ord}_L(s) \qquad (0\ne s\in H^0(X,mH)). This inequality controls the extra boundary on the surface and allows both applications of inversion of adjunction to use effective boundaries. Retaining the threefold discrepancy gives AX(v)−(288/245)SX(v)≥11v(a)/35>0A_X(v)-(288/245)S_X(v)\ge11v(a)/35>0. No Zariski decomposition on either extracted threefold enters this final calculation.

For Family 2.5, Cheltsov–Denisova–Fujita [8] proved K-stability under the assumption that the cubic-surface fibration has no singular point of type D5D_5 or E6E_6. Their local exclusions reduce the general case to these two singularities. Part II supplies the bounds 96/9596/95 and 16/1516/15 for the corresponding local thresholds and completes their reduction.

For Family 2.9, the argument in [3, Section 5.2] proves K-stability of a particular member using a cyclic group of order five and hence gives K-stability for a general member. Part III treats every smooth member. Flags on smooth cubic surfaces handle reduced conic fibres away from a distinguished exceptional fibre. At its remaining smooth-fibre points, blowing up the point on the cubic surface gives δp(X)≥6912/5335\delta_p(X)\ge6912/5335. We also give an independent proof using the exceptional plane of a threefold point blow-up. Double conic fibres require a weighted curve extraction; its exceptional surface is ℙ1×ℙ1\mathbb P^1\times\mathbb P^1 with different one half of a smooth (2,1)(2,1)-curve. The boundary is retained in the surface calculation.

For Family 2.10, Kaloghiros and Petracci proved K-stability of a general member [20, Theorem 1.3], and the equivariant results of [23] include special members. Part IV removes the generality and symmetry assumptions. Fibre estimates and nodal auxiliary sections treat the global reduction. Weighted point extractions treat D4D_4 and D5D_5 fibre singularities, while ordinary point blow-ups treat smooth points on the special lines of singular fibres. The latter computation requires an additional anticanonical section whose order exceeds the orders of its displayed summands.

The new exceptional-surface estimates do not require a complete Zariski decomposition on the extracted threefold. In Families 2.5 and 2.10, we identify the actual section filtrations, including cancellations, by regularity, localization and saturation. Weighted Hilbert functions and polynomial intervals then give the expected orders. In the exceptional-surface arguments for Family 2.9, explicit necessary vanishing conditions give spaces containing the refined sections. Their order sums provide upper bounds with the original normalization. We retain the volume calculations on the original threefolds, the Zariski decompositions on auxiliary surfaces, and the complete transverse-position calculation in Part III. Thus the absence of a full decomposition on an extracted threefold is justified by a description or comparison of section spaces, not assumed.

For Family 2.11, Part V treats both kinds of lines. The original exceptional divisor suffices for first-kind lines. For second-kind lines, its refined threshold is only 24/2924/29, so another argument is needed. A weak cubic section gives δp(X)≥36/35\delta_p(X)\ge36/35 on the special reduced fibre. After the curve centres and transverse points have been excluded, the remaining points lie on two ramification rulings over smooth conic fibres. A weight-(1,1,2)(1,1,2) blow-up at each such point has expected order 26/926/9 and refined surface threshold at least 216/167216/167. We calculate the latter from complete binary spaces with explicit fixed factors. A valuation centred on the ramification ruling has discrepancy three and expected order 167/72167/72, giving the matching upper bound. Thus the local threshold at each of these tangency points is exactly 216/167216/167; see Corollary 29.9. For double fibres, the two possible expected orders are 91/3691/36 and 169/72169/72, according to whether the reduced fibre lies in the original exceptional divisor; both refined surface thresholds are at least 144/127144/127. None of these weighted extractions requires a threefold Zariski decomposition.

For Family 2.12, Cheltsov–Li–Ma’u–Pinardin [1] reduced every possible nonpositive-beta valuation to a closed point of E∩E′E\cap E' and proved stability for several special members. Part VI completes the point analysis. Smoothness of the determinant quartic forces the coprimality needed for an exact ordinary initial ring. Three cases on its exceptional plane are treated by explicit monomial moment certificates. In one of them the refined threshold equals one, but the extraction discrepancy retains a strictly positive term. Proportional residual directions require weights (2,1,1)(2,1,1); the expected order is 13/413/4 and the refined threshold is at least 40/3740/37. We compute both ordinary and weighted expected orders in a separate Hilbert-weight lemma. These computations, too, require no Zariski decomposition on an extracted threefold.

For Family 2.13, the symmetric construction in [3, Section 5.5] proves K-stability of a particular member and hence of a general member. The smooth-conic estimate in the proof of [24, Lemma 5.6] gives δp(X)≥80/77\delta_p(X)\ge80/77. Part VII treats all remaining fibres. The ordinary blow-up of a node on a quartic del Pezzo section improves the polarized surface estimate to δp(S,−KS+tF)≥4/(3+2t)\delta_p(S,-K_S+tF)\ge4/(3+2t). For a double conic, the blow-up of its scheme-theoretic fibre ideal is a weight-(1,2)(1,2) curve extraction. Its expected vanishing is 5/25/2, and its exceptional pair is (ℙ1×ℙ1,12D)(\mathbb P^1\times\mathbb P^1,\tfrac12D) with DD a smooth (2,1)(2,1)-curve. We identify the actual weighted initial ring and its refined ideal-power spaces before estimating their thresholds. A degeneration keeps DD fixed. The limiting spaces can be smaller than the natural monomial spaces containing them; the resulting dimension correction is essential for the strict inequality. This weighted argument uses no Zariski decomposition on the extracted threefold.

For Family 2.14, the symmetric construction in [3, Section 4.3] proves K-stability of a particular member, and hence of a general member. Part VIII treats every smooth member. Every pencil fibre is a normal quintic del Pezzo surface with Du Val singularities. The exact fibre refinement reduces possible nonpositive-beta centres to certain lines and singular points. Ordinary line blow-ups and weight-(1,2)(1,2) line extractions treat the two normal-bundle types. The latter require separate calculations at the intersection with the original exceptional divisor. Point extractions treat A1,A2,A3,A4A_1,A_2,A_3,A_4. Prime Pfaffian initial rings and full-volume section certificates account for all cancellations. A restriction lemma retains the zeros on a second divisor, giving the complementary point bounds. At an A3A_3 point, the first extraction has expected order 71/1671/16 and discrepancy five; its positive margin completes the argument even when the refined threshold equals one. None of these extractions requires a threefold Zariski decomposition.

For Family 2.16, Cheltsov–Hwang–Küronya–Laface–Mangolte–Massarenti–Park–Zhao [28] prove strict local estimates at every point on a reduced conic fibre. Their main theorem consequently proves K-stability when the discriminant is smooth, and more generally under an explicit equivariant condition. Kaloghiros–Liu–Petracci–Zhao [34, Appendix A, Theorem A.1] describe the geometry of all K-semistable degenerations of this family; that result does not by itself prove stability of every smooth member. Part IX treats the remaining double fibres. Blowing up their fibre ideals gives a plt exceptional surface F≅ℙ1×ℙ1F\cong\mathbb P^1\times\mathbb P^1 with different D/2D/2 of bidegree (2,1)(2,1). A prime initial complete intersection identifies the actual refined spaces as H0(ℐPk(m−ϵ,r))H^0(\mathcal I_P^k(m-\epsilon,r)) for one point P∈DP\in D. Their dimensions give SX(F)=57/22S_X(F)=57/22. Moving PP to a ramification point while preserving DD gives the exact monomial spaces used for the bound 88/8588/85. The reduced-fibre estimates then give δ(X)≥176/171\delta(X)\ge176/171. This proof also uses no Zariski decomposition on the weighted extracted threefold. A second proof in Sections 57–60 uses GIT. We compute the CM polarization on the incidence space of a conic and a pencil of quadrics and prove a strict Hilbert–Mumford inequality for every smooth pair. The relative reconstruction of [34, Proposition A.13], together with CM-degree minimization, then gives K-stability. This argument is independent of the local threshold estimates and does not assume the conjectural description of the entire K-moduli space as a GIT quotient.

For Family 2.17, Cheltsov–Pokora [40] reduce possible nonpositive-beta centres to points of E∩E′E\cap E'. Part X uses the two contracted lines to reduce further to ΣX\Sigma_X. The remaining triple-contact points are treated by a weight-(1,1,2)(1,1,2) blow-up. The exact initial section ring gives SX(G)=29/8S_X(G)=29/8, and a second degeneration gives refined threshold at least 64/5964/59. The exact Hilbert count ensures that no higher-order sections are lost. This completes K-stability for every smooth member. No Zariski decomposition on this weighted point blow-up is required.

For Family 3.6, Cheltsov [42] proves K-stability when the conic bundle has reduced fibres. Part XIV treats the omitted double conics. The blow-up of their fibre ideals gives a weighted curve extraction of discrepancy three and expected order 243/88243/88. We compute its actual refined spaces, retain the different D/2D/2, and prove that the refined threshold is at least one. The positive remainder 21/8821/88 then proves strict K-stability. The argument includes the case where the line passes through a quadric-cone vertex and the corresponding sextic fibre is nonnormal. As in the preceding weighted arguments, no threefold Zariski decomposition is used at this extraction.

For Family 3.2, Belousov–Loginov [43] prove K-stability when the cubic fibre containing each double conic has only A1A_1 singularities along it. We use their corrected third version: its reduced-conic estimate is non-strict, and we retain the positive remainder in the first Abban–Zhuang step. Part XII treats the omitted double conics. Their weighted extraction has expected order 135/56135/56. An exact dimension count identifies its refined sections with monomial spaces. A second degeneration, with the different retained, gives refined threshold at least one. The finite-level equality at one weighted surface point is exact; the threefold discrepancy remainder 33/5633/56 gives strict K-stability. No Zariski decomposition on the weighted threefold is used.

For Family 3.5, Denisova [14] proves K-stability when all ramification is simple. The totally ramified cases are described in [3, Section 7.5]. Part XIII gives their explicit degeneration and its Abban–Zhuang input. It also computes SX(G)=(91r+25)/80S_X(G)=(91r+25)/80 for the weight-(1,2,r−2)(1,2,r-2) extraction at a fibre singularity of ramification index r=3,4,5r=3,4,5. These first moments do not by themselves prove the required exceptional-surface inequalities. For r=3r=3, an exact normal basis and an explicit surface log resolution now give δ(G;WG)≥160/151\delta(G;W^G)\ge160/151 and δp(X)≥160/151\delta_p(X)\ge160/151. For r=4r=4, a conic refinement with its different gives δ(G,Δ;WG)≥80/77\delta(G,\Delta;W^G)\ge80/77 and the exact local threshold δp(X)=400/389\delta_p(X)=400/389. Explicit line refinements cover the other centres outside the joining line of a mixed fibre. Ordinary point extractions then give 240/221240/221 at its A1A_1 endpoint and 32/2932/29 at its interior points. Their exact initial algebras and conic or cubic pencil resolutions complete the proof for every smooth member without a totally ramified point. The fibre-refinement calculation at an A2A_2 point is audited separately: the displayed surface volumes in [14] give 91/8091/80, rather than the stated 83/8083/80. The general semistability assertion for Family 3.5 and its complete smooth classification are included in the main theorem.

Section 102 applies the CM and GIT calculations in Liu’s moduli-continuity approach. The graph parameter space has anticanonical CM line 𝒪(22)\mathcal O(22), and a smooth graph is GIT-stable exactly when its degree-five map has no totally ramified point. Liu–Zhao’s volume theorem applies to K-semistable limits of volume 2020; the anticanonical K3 lattice on a smooth member is U⊕⟨−28⟩U\oplus\langle-28\rangle. The independent local proof above establishes the smooth classification. Reconstructing contractions on arbitrary limits remains a question for the K-moduli compactification.

For Family 3.7, [3, Section 4.3] treats symmetric examples, while [23, Lemma 4.3] imposes an additional group-action hypothesis. Part XV treats every such centre. The matrix pencil has only smooth fibres and fibres with one A1A_1 or A2A_2 singularity. Fibre refinements reduce the problem to the two lines through these singularities. Quintic del Pezzo sections treat their open parts. Ordinary and weighted point extractions treat the singular points, the intersections with the original exceptional divisor, and the remaining smooth corner. Their actual initial section spaces are proved complete by exact Hilbert counts. No Zariski decomposition on an extracted threefold is used.

For Family 2.20, [3, Section 7.2] gives GIT-semistable smooth parameters whose orbits are not closed and whose associated threefolds are strictly K-semistable. Its Proposition 5.43 proves K-polystability of the unique member with infinite automorphism group. Part XI rewrites the parameter classification intrinsically using binary quartics and a sextic Wronskian, constructs the smooth special degenerations, and gives Abban–Zhuang reductions to singular conic fibres. The complete weighted refinement treats all double fibres on the GIT-stable locus. Component extractions treat reduced fibres away from finitely many nodes on EE. The full point refinements at these nodes give δp(X)≥104/103\delta_p(X)\ge104/103 and prove the GIT-stable converse. This completes the smooth classification.

For Family 3.8, [3, Section 7.6] formulates the classification in terms of the degree-four cover and proves the total ramification cases. Part XVI completes the K-stable case. The quartic pencil can have fibres of types (2,1,1)(2,1,1), (2,2)(2,2) or (3,1)(3,1), and each type is included. Exact initial algebras treat the A1A_1 and A2A_2 points. Weighted curve extractions, surface flags and a marked specialization treat the exceptional rulings and the joining lines, including their endpoints. The final criterion is stated in Section 128.

Part I collects the Abban–Zhuang theory, the shared definitions and computational tools, and examples illustrating their later applications. The thirteen universal K-stability assertions of Theorem 1.1 are proved in Parts ??, II, III, IV, V, VI, VII, VIII, IX, X, XII, XIV and XV, respectively. The complete classification for Family 2.20 is proved in Part XI and summarized in Section 82. The classifications for Families 3.5 and 3.8 are treated in Parts XIII and XVI, respectively. The local theorems in those parts record the stronger estimates used in the proofs. In Part ?? we write H=−KXH=-K_X and use LL for a line. In the other parts we write L=−KXL=-K_X; the remaining geometric notation is introduced separately in each part. In particular, the letters denoting fibre and exceptional classes are local to that part. Every local stability threshold takes the infimum over divisors whose centres contain the specified point, including positive-dimensional centres.