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Very general K3 sections in the specified Fano regimes have the primitive ambient Picard group

Statement

Assume AC. In each of the following two cases, a very general smooth surface S in the specified system has Pic(S)=Z(A∣S), integrally. Here very general means outside a countable union of proper closed algebraic subvarieties of the smooth-member parameter space.

(i) Y is a smooth connected complex projective threefold, A is ample, Pic(Y)=ZA and H2,0(Y)=0; L is VERY AMPLE and its smooth members are K3 surfaces; the system is |L|.

(ii) Y is a smooth degree-one del Pezzo threefold in the weighted normal form {w2=z3+f4(x)z+f6(x)} in P(1,1,1,2,3), with Pic(Y)=ZA, A=OY(1), −KY=2A, and H0(Y,2A)=span⁡{xixj,z}. The system is |2A|. Its general smooth members are double-plane K3 surfaces, and (A∣S)2=2. This system is not assumed very ample.

In particular in either case every divisor D on such S satisfies (A|S)² divides D·(A|S). Application of (i) to a high-degree Fano ladder requires the actual very-ampleness and smooth-ladder supplier; the lemma does not infer very-ampleness from a Picard-number hypothesis or include excluded double-quadric regimes.

Facts & Assumptions

Given: Exactly one of the two explicit geometric regimes in the Statement. The weighted normal form, full section system and Picard group are inputs in case(ii); its K3 and monodromy assertions are proved below. No Noether–Lefschetz theorem or irreducibility theorem for vanishing cohomology is assumed.

[F1]

Ample divisor relative handles and primitive integral restriction gives the actual relative handle presentation for a smooth AMPLE divisor, including π1 isomorphism in dimension at least three and primitive integral H² restriction in dimension three. Its proof works without very-ampleness of that divisor.

[F2]

Bertini smoothness away from the base locus applies to arbitrary basepoint-free characteristic-zero systems. Compact Kähler Hodge decomposition from elliptic harmonic forms supplies Hodge decomposition. Gauss–Manin connection and Griffiths transversality supplies holomorphic periods for the smooth projective family. The local differentiable triviality needed below is constructed by vector-field lifting.

[F3]

General Thom isomorphism from the relative Serre spectral sequence applies to the complex oriented normal bundles over the compact base curve. Mayer–Vietoris sequence in singular homology and Poincaré duality for oriented topological manifolds give the displayed gluing and intersection duality. The latter is used on closed compact oriented manifolds. Cohomological Serre spectral sequence is used only for the hypothetical smooth K3 fibration over P1, where it has no degree-two outgoing differential.

[F4]

Local morse sublevel pair is a handle pair gives the compact-band real three-handle used after the explicitly proved holomorphic quadratic normalization. Its argument is not a vanishing-cycle or Picard–Lefschetz theorem; those statements are constructed below.

[F5]

Cattani–Deligne–Kaplan algebraicity of Hodge loci is the actual proved CDK theorem for smooth projective families over smooth quasi-projective complex bases, applied at weight two. Its analytic prerequisites are not re-proved or changed here. Assuming dependent choice, every locally compact Hausdorff space is a Baire space supplies Baire for the complex parameter open set.

[F6]

The Axiom of Choice is the ambient choice convention and implies the dependent/countable choice in F1,F4,F5. Singular homology and cohomology coefficients are explicitly Z or Q below. H² denotes cohomology, while H2 denotes homology, also when plain-text expressions spell out the distinction.

Proof

technique · explicit relative handles, discriminant and local quadratic monodromy, then CDK and the integral index argument
1.1givenF1F2F3F4F5F6algebra

Apply F1 to a smooth member S: its ample line bundle is L in case(i) and 2A in case(ii). It gives the integral relative cells and primitive restriction described there; very-ampleness is not needed for this step. The weighted case's smooth K3 input follows by the following direct construction. For S avoiding λ=0, eliminate z to obtain w2+g6(x)=0. Smoothness makes the sextic branch curve smooth. The ordinary sextic T=u6+g6(x)=0 in P3 is smooth by its Jacobian, and F1 gives π1(T)=π1(P3)=0. Scaling u by μ3 has quotient S via w=u3 and has a nonempty fixed curve u=0. Perturb a loop of S off the branch curve and lift it to T; its endpoint differs by a deck element g. A path from the starting point to a fixed point, followed by the reverse of its g-translate, projects to a backtracking contractible loop with the same endpoint deck transformation. Removing that loop makes the lift close, so it contracts in T and its projection contracts the original loop. Thus S is simply connected. The double-plane canonical formula follows directly from the residue dx∧dy/w in the local equation; its transition degree is −3+3=0, so KS is trivial. The finite algebra OP2 direct-sum OP2(−3) computes H1(OS)=0 by the projective-plane Čech complex. Connectedness follows from F1. Hence S is a K3 and h20(S)=1, without assuming a Fano simple-connectivity theorem or a double-plane Picard theorem. In our situation H1(S;Z)=0, so H1(Y;Z)=0. The Kähler decomposition gives H1(OY)=0, and H2,0(Y)=0 gives H2(OY)=0. The exponential sequence consequently identifies Pic(Y) with H2(Y;Z) in COHOMOLOGY. Thus its generator a=c1(A) is primitive. The surjection on integral HOMOLOGY above shows h=a∣S is primitive too: the primitive cohomology character a evaluates to 1 on some homology class, which lifts from S. No Picard-group rank argument has silently omitted a possible finite index.

2.1givenF1F2F3F4F5F6step 1.1algebra

For later use the intersection form on H2(S;Q) in cohomology is nondegenerate, and h2>0. Define V=h perpendicular. It is a nondegenerate rational subspace. The ambient rational H2 of Y is one-dimensional, by Pic(Y)=ZA and H20(Y)=0. The holomorphic two-form of the K3 lies in VC and is nonzero.

3.1givenF1F2F3F4F5F6step 2.1algebra

For a basepoint-free ample system on Y, choose a general pencil with smooth connected base curve B. Smoothness follows from two successive characteristic-zero Bertini applications; connectedness follows from Section1 on a smooth member, since B is an ample curve there. Blow up B to get p:Z→Y and a projective morphism f:Z→P1. Each original member is unchanged as a surface: blowing up its Cartier base curve is the identity. This also identifies its fibre cohomology and polarization without an auxiliary resolution of the surface.

4.1givenF1F2F3F4F5F6step 3.1algebra

The topological facts needed about this blowup are explicit. Replace a tubular rank-two complex disk bundle over B by the disk bundle of the tautological line over its P1 bundle. Their common outer boundary is the same sphere bundle. The Thom exact sequences, or the cellular decomposition of that P1 fibre, give

5.1givenF1F2F3F4F5F6step 4.1algebra

H2(Z;Q) in cohomology=p*H2(Y;Q) direct-sum Q[E],

6.1givenF1F2F3F4F5F6step 5.1algebra

where E is the exceptional divisor; no H1(B) term occurs in degree two. On a pencil fibre S, E restricts to the base divisor B, whose class is c1(L|S). Since L is a multiple of A, the image of H2(Z;Q) on S is precisely Qh. Also H20(Z)=H20(Y): a holomorphic two-form on Z restricts away from E to Y minus B and extends across B by the coefficientwise Hartogs theorem on the smooth threefold. Pullback gives the inverse extension. The same Hartogs argument follows from the two-variable Cauchy integral on a polydisc, so birational invariance of H20 is not a separate premise.

7.1givenF1F2F3F4F5F6step 6.1algebra

Suppose the pencil's only critical fibres have one ordinary quadratic singularity. For completeness a nondegenerate holomorphic critical point has local form z1²+z2²+z3². Solve ∂F/∂z1=0 by the implicit-function theorem, shift to its graph, factor the remaining z1² coefficient, and take its nonvanishing holomorphic square root. The residual Hessian is its nondegenerate Schur complement; repeating gives the displayed form. Thus no holomorphic Morse normal-form theorem is assumed without its argument.

8.1givenF1F2F3F4F5F6step 7.1algebra

Choose disjoint arcs from a regular value to all critical values in a disk D containing them. Proper submersions away from the critical points are locally differentiably trivial: a metric gives lifts of coordinate vector fields; properness makes their flows exist uniformly on each compact base chart, and a boundary collar makes the same construction relative to a boundary. Cut along the arcs and contract the regular base corridors. At each critical end the real function Re F=Σ Re(zi)2−Σ Im(zi)2 has index three. Its compact-band handle has core D3 and attaching sphere the real vanishing S2 in a neighbouring fibre. Accordingly f inverse(D) is obtained, up to relative homotopy, from a regular fibre S by adjoining these three-cells. In particular the kernel of H2(S;Q)→H2(f inverse(D);Q) is the span of their vanishing spheres δi.

9.1givenF1F2F3F4F5F6step 8.1algebra

Over the complementary disk the fibration is a product. In Mayer–Vietoris for Z=f inverse(D) union (S times D'), the intersection is S times S1. Since H1(S)=0, its degree-two homology is just H2(S), mapping by (q,−identity). Its cokernel injects into H2(Z) and identifies with H2(f inverse(D)). Consequently the kernel of H2(S)→H2(Z) is exactly spanδi; the additional base two-class in H2(Z) makes no new relation in H2(S). By the preceding description of the image of H2(Z) in cohomology and perfect intersection duality, that kernel is exactly V. Hence the vanishing cycles span the ENTIRE nondegenerate primitive rational space V, not an unspecified vanishing subspace.

10.1givenF1F2F3F4F5F6step 9.1algebra

The local monodromy is also explicit. In Σzi2=t>0 write z=x+iy: x⋅y=0 and ∣x∣2−∣y∣2=t. The map (u,y)↦sqrt(t+|y|²)u+iy identifies the local fibre with a disk cotangent bundle of S2. Its zero sphere δ has self-intersection −2: J identifies its normal with its tangent, but the complex orientation differs from tangent-then-normal orientation by one interchange, so its normal Euler number is −χ(S2). As t circles zero, the square-root continuation sends δ to its antipodal sphere, of degree −1. Trivialize the family outside the Milnor ball over the full parameter disk; its monodromy is the identity there. Excision therefore makes T(x)−x a multiple of δ. Intersection preservation and Tδ=−δ force that multiple to be x·δ. Thus

11.1givenF1F2F3F4F5F6step 10.1algebra

Tδ(x)=x+(x⋅δ)δ, δ²=−2.

12.1givenF1F2F3F4F5F6step 11.1algebra

This derives exactly the required Picard–Lefschetz reflection and its sign from the local model.

13.1givenF1F2F3F4F5F6step 12.1algebra

Embed Y by the COMPLETE very ample system |L| in PN. Its conormal incidence C={(y,H):H contains the projective tangent space at y} is a projective bundle over the irreducible Y, irreducible of dimension N−1. Its image D in the dual projective space is the discriminant, irreducible and proper by Bertini.

14.1givenF1F2F3F4F5F6step 13.1algebra

D is a hypersurface. Otherwise a general projective line avoids it, so the preceding pencil is a smooth K3 fibration Z→P1. Its degree-two Leray calculation gives a surjection H2(Z;Q)→H2(S;Q) in cohomology: the local system is constant since P1 is simply connected; H1(S)=0 eliminates the possible differential to H2(P1,R1), and H3(P1)=0 eliminates the next one. Equivalently use the cellular two-disk cover of P1 and the same obstruction calculation. Restriction is a morphism of the Kähler Hodge decompositions, so this surjection is incompatible with H20(Z)=0 and H20(S)=C. This proves nondefect rather than importing a classification of dual-defective varieties.

15.1givenF1F2F3F4F5F6step 14.1algebra

The generic discriminant member has one quadratic singularity. The map C→D is generically finite and separable, hence its differential is an isomorphism at a generic point. Its kernel in the y direction is the kernel of the Hessian of the hyperplane section, so that Hessian is nondegenerate. Moreover a generic smooth point of D has only one contact point: a contact at y gives tangent space to D equal to the hyperplane of variations η with η(y)=0. Two distinct contact points would give two different tangent hyperplanes, because the embedding separates points, making the discriminant singular there. Thus there is a dense smooth open D° of members with precisely one quadratic singularity. Its complement has codimension at least two in the whole dual projective space. A general pencil meets only D°, transversely, and has the smooth base required in Section2.

16.1givenF1F2F3F4F5F6step 15.1algebra

All its vanishing cycles are conjugate, up to sign, under monodromy of the full smooth-member family. The smooth dense D° of an irreducible complex algebraic variety is path connected. Move a small positively oriented normal circle along such a path in its tubular neighbourhood; after joining it to a fixed smooth-member base point these meridians are conjugate. Their reflections have one-dimensional minus-one eigenspaces Qδ, so conjugation transports δ to ±δ. This proves the conjugacy assertion without assuming that a pencil's own critical values are interchangeable.

17.1givenF1F2F3F4F5F6step 16.1algebra

Now use the separate weighted normal form in the Statement. The second-Veronese map of P(1,1,1,2) identifies it with the projective cone C over the Veronese P2, with coordinates (xi xj,z). The map φ:Y→C forgetting w is finite of degree two. Its vertex has a single preimage p, since at x=0 one has w2=z3. Its branch surface is the image of R=w=0.

18.1givenF1F2F3F4F5F6step 17.1algebra

R avoids the vertex: x=0 would give z3=0, impossible in projective coordinates. It is smooth, because on w=0 the smoothness of Y is exactly the nonvanishing of d(z³+f4z+f6) on the smooth part of the cone. It is connected and hence irreducible: it is the smooth ample divisor of the section w of 3A, so Section1 makes H0(R;Z)→H0(Y;Z) an isomorphism. The restriction φ|R is a closed embedding onto its smooth branch surface in P6; it is the explicit second-Veronese closed embedding of the weighted cone restricted away from its vertex.

19.1givenF1F2F3F4F5F6step 18.1algebra

Also H20(Y)=0. The weighted polynomial Čech complex has no intermediate cohomology Hq(P(1,1,1,2,3),O(k)) for 0<q<4: separate it by Laurent monomials, each of which gives the simplex complex on its negative-coordinate set and contributes only at the extremes. The hypersurface sequence 0→O(−6)→O→OY→0 therefore gives H1(OY)=H2(OY)=0; Kähler conjugation gives H20(Y)=0. The anticanonical system is basepoint free and its sections are λz+q2(x). It maps Y by φ. Let Dv=λ=0, a HYPERPLANE in its parameter P6. Every member there is singular at p. In the chart z=1 choose the local branch w near 1 of w2=1+f4(x)+f6(x). The weighted μ2 chart interchanges w near1 and w near−1, so this branch is an honest smooth coordinate chart at p with coordinates x. The section is EXACTLY λ+q2(x). A generic member of Dv therefore has one quadratic singularity at p.

20.1givenF1F2F3F4F5F6step 19.1algebra

Every other singular member is a hyperplane tangent to R. Away from R and p the double cover is a local isomorphism. A hyperplane with λ≠0 has nonzero derivative along the cone's z direction, so it is smooth there. At R the differential of the double cover has image T R; the singularity condition is exactly tangency of the hyperplane to that embedded surface. Consequently the full discriminant is Dv union DR, where DR is the image of the irreducible conormal incidence of R.

21.1givenF1F2F3F4F5F6step 20.1algebra

These are distinct. At a point of R with 3z²+f4(x)≠0, the vertical cone direction is not tangent to R, so some tangent hyperplane to R has λ≠0. Such a point exists: the irreducible polynomial defining R, cubic in z, cannot divide its nonzero degree-two z derivative in characteristic zero. Thus DR is not contained in Dv.

22.1givenF1F2F3F4F5F6step 21.1algebra

DR is a hypersurface. If it had codimension at least two, a general pencil would avoid it and have exactly one singular fibre, its transverse intersection with Dv. That fibre has the single quadratic singularity at p just calculated. Its monodromy would be a nontrivial reflection, since δv2=−2. But the base P1 minus a single critical value is simply connected, so its monodromy is the identity. This contradiction proves the assertion.

23.1givenF1F2F3F4F5F6step 22.1algebra

The generic DR member is again one quadratic singularity. Its conormal map is generically finite/separable, and the same tangent-space argument as in Section3 gives one contact point with nondegenerate tangential Hessian on R. Take a generic contact away from 3z2+f4=0, and λ≠0. Locally the cover is v=w2 with R=v=0; the coefficient of v in the hyperplane equation is nonzero, because its value on the vertical cone direction is λ. The local Hessian on Y is the nondegenerate two-variable tangential Hessian plus a nonzero w² term. Thus it is nondegenerate in three variables. The dense nodal DR° is irreducible/path connected, so these cycles are conjugate under the smooth-member family, exactly as before. A general Dv member is not in DR and has no further singularity.

24.1givenF1F2F3F4F5F6step 23.1algebra

A general anticanonical pencil now has smooth connected base, all critical fibres quadratic, and EXACTLY ONE critical value from Dv. All other critical values come from DR°. Smooth members are K3 by the geometry input and adjunction; their primitive polarization is A|S, with square 2A3=2. Section1 applies because 2A is ample, even though it is not very ample. Thus the same integral primitive restriction conclusion and the thimble spanning V from Section2 apply here.

25.1givenF1F2F3F4F5F6step 24.1algebra

Let W be the span of the cycles δr from DR°. Each corresponding reflection acts as the identity on V/W and preserves W. The global relation of meridians in the pencil is

26.1givenF1F2F3F4F5F6step 25.1algebra

Tv times product(Tr)=identity.

27.1givenF1F2F3F4F5F6step 26.1algebra

It follows that (Tv−identity)V⊂W. In particular −2δv=(Tv−identity)δv belongs to W. Thus δv itself belongs to W over Q. Since ALL cycles span V by Section2, the conjugate ramification cycles ALONE span V. This is why the vertex hyperplane does not force an extra generic Picard class. Neither irreducibility of the full two-component discriminant nor an unjustified transitivity between its components is asserted.

28.1givenF1F2F3F4F5F6step 27.1algebra

In each branch we have a set of conjugate vanishing cycles spanning the nondegenerate space V and reflections Tδ(x)=x+(x⋅δ)δ. If a nonzero rational monodromy-invariant subspace W⊂V were orthogonal to every cycle, nondegeneracy and spanning would force W=0. Otherwise choose w∈W with w·δ≠0. Then (Tδ−identity)w is a nonzero multiple of δ, so δ∈W. Monodromy conjugacy puts every chosen cycle in W, and they span V. Hence W=V. This proves irreducibility directly from the constructed reflections.

29.1givenF1F2F3F4F5F6step 28.1algebra

Consider a flat integral class γ not in Qh on a simply connected smooth parameter chart. If it were type (1,1) on an open set, its period against a local holomorphic two-form would vanish there. The holomorphic identity theorem continues that vanishing along every path on the universal cover of the smooth parameter locus. Project γ rationally to V by subtracting (γ·h)/(h²)h. Its nonzero monodromy orbit would therefore consist of (1,1) classes at the reference fibre. Its rational span is an invariant nonzero subspace, hence V by irreducibility. This would make V entirely (1,1), contradicting its nonzero (2,0) line. No such class has an open Hodge locus.

30.1givenF1F2F3F4F5F6step 29.1algebra

Apply the ACTUAL thm-gts-cattanidelignekaplan-algebraicity-of-hodge-loci to the universal smooth divisor family over this smooth quasi-projective open parameter space, with weight two and p=1. It makes the loci of additional integral (1,1) classes a countable union of closed algebraic subvarieties. Every component is proper by the preceding argument. Baire on the complex parameter space shows their complement is dense and nonempty; equivalently this is the very-general complement of countably many proper closed algebraic loci. At a point of that complement the rational Picard space is Qh.

31.1givenF1F2F3F4F5F6step 30.1algebra∎

Finally on a K3 the exponential sequence and H1(O)=0 identify Pic with the integral (1,1) classes in its torsion-free H2. Since Section1 proved h primitive, Qh intersect H2(S;Z)=Zh. Hence Pic(S)=Zh, integrally. In particular every divisor D satisfies h² divides D·h, the exact divisibility interface requested by the curve-bound assembly; rank at least one alone would not have supplied it.

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