Section 120
Anticanonical sections and the distinguished surface
For local calculations write and . Let , , and . The ambient realization of Lemma 117.1 has equation in . The homogeneous coordinates of have classes , respectively. The three plane coordinates have class . The irrelevant loci on are and . The distinguished surface is , of class .
Let be the exceptional divisor of and let be its defining section. The global sections and satisfy and their divisor classes are These identities are identities of actual global sections. They will suffice for the inclusions used in the refined series.
Lemma 120.1. For every , ambient sections restrict surjectively onto . More explicitly, this space is spanned by the restrictions of Its dimension is .
Proof. The anticanonical class is , while the hypersurface has class . Its restriction sequence has kernel For , the factor has no cohomology. For , pushing the first factor down to gives line bundles of degrees , all nonnegative. Künneth’s formula therefore gives zero first cohomology in either case, proving surjectivity. Comparing the two degrees on gives precisely the displayed monomials.
The dimensions of the ambient space and the kernel are respectively. Their difference is the asserted dimension. This proof uses the homogeneous coordinates of the ambient product and its hypersurface equation; it requires no assertion about generators of the whole Cox ring of . ◻
120.1 A flag on E
The surface has two ruling classes , where and . Thus , , and .
We also need the following calculation for a particular singular central fibre. It remains valid when the graph curve in degenerates to a reduced curve with one vertical component, provided that the flag ruling does not meet that component.
Lemma 120.2. Let be a smooth member, or the nodal central member obtained from the net Let and let be the ruling through . In the nodal case, suppose that is disjoint from the vertical component of . Then Consequently .
Proof. For , the decomposition of is The positive parts are nef, since are pullbacks of globally generated divisors. The second row is the fixed-part decomposition: on a general exceptional fibre of , the original divisor has degree , so every effective representative contains each component of with coefficient at least . After this part is removed, the remainder is pulled back from and is nef. The same argument applies to the nodal member, whose centre is a reduced union of two smooth components. Their exceptional divisors are both generically ordinary blow-ups, so the coefficient bound applies to each. For the residual plane degree is negative, proving that the threshold is . The common intersection numbers give
Write , where For the divisor is nef; it has volume and intersection with . Since is not a component of , there is no primary fixed contribution. Therefore The moving point contribution is The curve meets transversally at one point. For a smooth member this is the graph property. For the nodal member its other component is disjoint from by assumption, and its graph component has the same property. The only possible fixed point contribution is consequently This proves the three claimed values and bounds. The nodal singularity is disjoint from , so the same adjunction inequality applies there. Finally, ◻
120.2 Adjunction for a curve extraction
We recall explicitly the local form of the refinement inequality that we use for curves. A local threshold always takes the infimum over divisors whose centres contain the specified point.
Lemma 120.3. Let be a plt extraction of a smooth curve in a smooth Fano threefold, with exceptional divisor . Write Put , and let be the image of the restriction map from to For one has The restriction of to is retained in this definition. In particular, it need not be trivial for a curve extraction.
Proof. This is the local refinement inequality of [4, Theorem 3.3]. We recall its basis-divisor argument. Choose an anticanonical basis compatible with the order along and with a valuation being tested. Removing the powers of a local equation of gives bases of the spaces . The pullback basis divisor has the form where does not contain and its restriction is a basis divisor of with the usual normalization by . If a positive number is smaller than both quantities on the right, the proof of [4, Lemma 2.21] gives for all valuations of finite discrepancy and all sufficiently large , with the bound on independent of . Thus the same strict inequalities hold for the basis thresholds simultaneously over the proper fibre . Then adjunction makes log canonical over . Inversion of adjunction applies to there. The coefficient of in the pullback of the corresponding pair on is Decreasing the coefficient of therefore gives log canonicity of the original basis pair at . Taking the infimum over the valuations and the limit of the basis thresholds proves the inequality. Equivalently, this is the same refinement argument as for a point extraction, with the whole fibre over retained. ◻
The elementary decompositions along the distinguished surface and the del Pezzo fibres have already been displayed. In all point and curve extractions below, we do not compute a Zariski decomposition on the extracted threefold. We identify the actual refined sections, or embed them in complete series with the same asymptotic total dimension. The remaining decompositions and blow-ups occur on the exceptional surface.