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Section 10

Geometry and the local estimates

Family 2.9: conic bundles

Let C⊂ℙ3C\subset\mathbb P^3 be a smooth curve of degree 77 and genus 55, scheme-theoretically cut out by three cubics, and let π:X=BlCℙ3→ℙ3\pi:X=\mathop{\mathrm{Bl}}_C\mathbb P^3\to\mathbb P^3. These are the smooth members of Mori–Mukai Family 2.9; see [3, Sections 5.2 and 6]. Write EE for the exceptional divisor and H=π*𝒪ℙ3(1)H=\pi^*\mathcal O_{\mathbb P^3}(1). Set B=3H−E,L=−KX=4H−E=H+B.B=3H-E,\qquad L=-K_X=4H-E=H+B. The net |B||B| gives the conic bundle φ:X→ℙ2\varphi:X\to\mathbb P^2. One has L3=16L^3=16.

Theorem 10.1. For every smooth member of Family 2.9, SX(H)=2564,SX(B)=91192,SX(E)=65432.S_X(H)=\frac{25}{64},\qquad S_X(B)=\frac{91}{192},\qquad S_X(E)=\frac{65}{432}. Every prime divisor DD on XX satisfies βX(D)>0\beta_X(D)>0.

There is a point p0∈Cp_0\in C determined by CC itself: it is the common zero of the three linear forms in the linear syzygy between its cubic generators. The syzygy is unique up to a scalar, and the span of its three coefficients is independent of the generators, as proved in Lemma 10.4. This is why we call p0p_0 distinguished. Put f0=π−1(p0)≅ℙ1f_0=\pi^{-1}(p_0)\cong\mathbb P^1. Let Σ⊂ℙ2\Sigma\subset\mathbb P^2 be the finite set of points whose conic fibres are nonreduced, and set T=f0∪⋃y∈Σφ−1(y)red.T=f_0\cup\bigcup_{y\in\Sigma}\varphi^{-1}(y)_{\mathrm{red}}.

Proposition 10.2. If PP belongs to a reduced singular conic fibre, then δP(X)≥96/95\delta_P(X)\ge96/95. If P∉f0P\notin f_0 belongs to a smooth conic fibre, then δP(X)≥96/91\delta_P(X)\ge96/91. If P∈f0P\in f_0 belongs to a smooth conic fibre, then δP(X)≥512/453\delta_P(X)\ge512/453. Consequently, every point on a reduced conic fibre satisfies δP(X)≥96/95\delta_P(X)\ge96/95. If PP belongs to a double conic fibre, then δP(X)≥128/123\delta_P(X)\ge128/123. These estimates prove the Family 2.9 assertion of Theorem 1.1. At a point of f0f_0 on a smooth conic fibre, Proposition 12.4 gives the stronger bound δP(X)≥6912/5335\delta_P(X)\ge6912/5335.

The proof proceeds as follows. Section 12 treats every reduced conic fibre, using a curve flag or the blow-up of a point on a smooth cubic surface. Sections 14–17 give an independent proof at the smooth-fibre points of f0f_0 by a threefold point extraction; the complete transverse-position decomposition is included as an additional calculation. Section 18 treats double conic fibres by a weighted curve extraction and completes the proof. In the two exceptional-surface arguments, necessary vanishing conditions suffice to bound the refined series. We do not assume completeness of those series, or a threefold Zariski decomposition that has not been proved.

10.1 The two contractions and the distinguished point

Lemma 10.3. A general cubic surface S0S_0 containing CC is smooth. For each fixed smooth such surface, writing A=−KS0A=-K_{S_0}, there is a unique line ℓ=ℓS0⊂S0\ell=\ell_{S_0}\subset S_0 such that C∼2A+ℓ,A2=3,A⋅ℓ=1,ℓ2=−1.C\sim2A+\ell,\qquad A^2=3,\quad A\cdot\ell=1,\quad\ell^2=-1. The strict transform S⊂XS\subset X is isomorphic to S0S_0. Identifying AA and ℓ\ell with their pullbacks to SS and putting CS=(π|S)−1(C)C_S=(\pi|_S)^{-1}(C), one has H|S=A,E|S=CS∼2A+ℓ,B|S=F:=A−ℓ.H|_S=A,\qquad E|_S=C_S\sim2A+\ell,\qquad B|_S=F:=A-\ell. The pencil |F||F| is the conic bundle on SS obtained by restricting φ\varphi. The line ℓS0\ell_{S_0} varies with S0S_0; their images in ℙ3\mathbb P^3 all pass through the fixed point p0p_0, as shown in the proof of Lemma 10.6.

Proof. The cubic equations generate the ideal sheaf of CC. At a point of CC, their differentials span its two-dimensional conormal space. The cubics singular at that point form one point of the parameter plane. Varying the point of CC gives a subset of dimension at most one. Bertini applies away from CC, so a general cubic in the net is smooth.

Adjunction on S0S_0 gives C2=2g(C)−2+A⋅C=15C^2=2g(C)-2+A\cdot C=15. Thus D=C−2AD=C-2A satisfies A⋅D=1A\cdot D=1 and D2=−1D^2=-1. Riemann–Roch gives χ(𝒪S0(D))=1\chi(\mathcal O_{S_0}(D))=1, while h2(D)=h0(−A−D)=0h^2(D)=h^0(-A-D)=0 by ampleness of AA. Hence DD is effective. Its AA-degree is one, so it is a line. Two distinct lines have nonnegative intersection and cannot both represent a class of square −1-1, proving uniqueness.

The blow-up of the Cartier divisor C⊂S0C\subset S_0 is S0S_0 itself. The restriction formulas follow. The planes through ℓ\ell cut out ℓ\ell plus a residual conic, giving the base point free pencil |A−ℓ||A-\ell|. ◻

Lemma 10.4 (The linear syzygy). There are independent linear forms l0,l1,l2l_0,l_1,l_2 and quadratic forms q0,q1,q2q_0,q_1,q_2 such that the cubic generators are the components of f=l×q,(l0q0l1q1l2q2).f=l\times q, \qquad \begin{pmatrix}l_0&q_0\\l_1&q_1\\l_2&q_2\end{pmatrix}. The ideal has resolution 0→𝒪ℙ3(−4)⊕𝒪ℙ3(−5)→𝒪ℙ3(−3)⊕3→ℐC→0.0\longrightarrow\mathcal O_{\mathbb P^3}(-4)\oplus\mathcal O_{\mathbb P^3}(-5) \longrightarrow\mathcal O_{\mathbb P^3}(-3)^{\oplus3} \longrightarrow\mathcal I_C\longrightarrow0. The space of linear syzygies is one dimensional. The three-dimensional subspace UC=⟨l0,l1,l2⟩⊂H0(ℙ3,𝒪ℙ3(1))U_C=\langle l_0,l_1,l_2\rangle\subset H^0(\mathbb P^3,\mathcal O_{\mathbb P^3}(1)) depends only on CC, and not on the choice of cubic generators or of their syzygy. Its common zero is a single point p0∈Cp_0\in C, and q(p0)≠0q(p_0)\ne0.

Proof. We include the algebra behind this familiar determinantal description. On a smooth cubic from Lemma 10.3, the hypersurface sequence reduces the vanishing of H1(ℐC(n))H^1(\mathcal I_C(n)) to that of H1(S0,tA−ℓ)H^1(S_0,tA-\ell) for every integer tt. For t≥0t\ge0, use 0→𝒪(tA−ℓ)→𝒪(tA)→𝒪ℓ(t)→00\to\mathcal O(tA-\ell)\to\mathcal O(tA)\to\mathcal O_\ell(t)\to0; the restriction of degree-tt polynomials to a line is surjective and H1(tA)=0H^1(tA)=0. For t<0t<0, Serre duality reduces the assertion to H1(kA+ℓ)=0H^1(kA+\ell)=0, k=−t−1≥0k=-t-1\ge0, and the sequence with quotient 𝒪ℓ(k−1)\mathcal O_\ell(k-1) gives this vanishing. Thus CC is arithmetically Cohen–Macaulay.

For completeness, the three given cubic equations generate the ideal sheaf, so their kernel 𝒦\mathcal K is locally free of rank two. The preceding vanishing gives H2(𝒦(n))=0H^2(\mathcal K(n))=0 for every nn. Since det𝒦=𝒪(−9)\det\mathcal K=\mathcal O(-9), rank-two duality and Serre duality give H1(𝒦(n))=0H^1(\mathcal K(n))=0 as well. Horrocks’ splitting criterion [19] therefore writes 𝒦=𝒪(−a)⊕𝒪(−b)\mathcal K=\mathcal O(-a)\oplus\mathcal O(-b). There is no constant relation among the three cubics, and a+b=9a+b=9, so {a,b}={4,5}\{a,b\}=\{4,5\}. The Hilbert–Burch theorem [16] now gives the displayed matrix and its minors.

If the linear column had rank two, coordinates would make it (x,y,0)(x,y,0). Its minors would be yq2,−xq2,xq1−yq0yq_2,-xq_2,xq_1-yq_0. Unless q2=0q_2=0, irreducibility and nonplanarity of CC would force C⊂(q2=0)C\subset(q_2=0). But CC lies on no quadric: on S0S_0, such a quadric would give an effective divisor 2A−C∼−ℓ2A-C\sim-\ell. If q2=0q_2=0, the minors do not have codimension two. Rank at most one similarly forces a planar component or the wrong codimension. Thus the linear forms are independent. They vanish at a point p0p_0, which belongs to the determinantal curve. If also q(p0)=0q(p_0)=0, all the minors have zero differential there, contradicting smoothness of CC.

Twisting the resolution by 44 identifies the space of linear syzygies with H0(𝒪ℙ3⊕𝒪ℙ3(−1))=ℂH^0(\mathcal O_{\mathbb P^3}\oplus\mathcal O_{\mathbb P^3}(-1))=\mathbb C, so its nonzero element is unique up to a scalar. To check independence of the cubic generators, regard ff and ll as columns, so that the relation is l𝗍f=0l^{\mathsf t}f=0. If f′=Mff'=Mf for M∈GL3(ℂ)M\in\operatorname{GL}_3(\mathbb C), its linear syzygy is a nonzero scalar multiple of M−𝗍lM^{-\mathsf t}l. Invertible recombination and multiplication by a nonzero scalar preserve the span of the three coefficients. Hence UCU_C and its common zero p0p_0 are intrinsic to CC. In particular, their construction does not involve the choice of a cubic surface through CC. ◻

Lemma 10.5 (The incidence model). The morphism (π,φ)(\pi,\varphi) identifies XX with the complete intersection (10.1)∑i=02li(x)yi=0,∑i=02qi(x)yi=0in ℙx3×ℙy2.\label{f29:eq:incidence} \sum_{i=0}^2l_i(x)y_i=0,\qquad \sum_{i=0}^2q_i(x)y_i=0 \quad\text{in }\mathbb P^3_x\times\mathbb P^2_y. The divisors H,BH,B are the restrictions of 𝒪(1,0),𝒪(0,1)\mathcal O(1,0),\mathcal O(0,1), respectively. The first equation defines a plane bundle over ℙy2\mathbb P^2_y, and φ\varphi is a flat family of nonzero plane conics in this bundle.

Proof. Off CC, the two equations specify the point y=l×qy=l\times q. Along CC, their coefficient matrix has rank one: rank zero would make the differentials of all its minors vanish, contradicting smoothness of CC. Near any point of CC, a unit matrix entry allows row and column operations reducing the incidence equations to the usual equation for the blow-up of a two-generated ideal defining a smooth codimension-two centre. Thus (10.1) is the graph of the cubic net, including over CC. The restriction formulas follow.

For each yy, the linear form ly=∑liyil_y=\sum l_i y_i is nonzero because the lil_i are independent. Its zero plane is denoted by Πy\Pi_y. The quadratic qy=∑qiyiq_y=\sum q_i y_i does not vanish identically on Πy\Pi_y. Otherwise, after an invertible linear recombination of the three rows, ly=l0l_y=l_0 and qy=q0=l0rq_y=q_0=l_0r for a linear form rr. On Πy\Pi_y, two minors then vanish identically and the remaining one is a cubic. Their common zero scheme contains a plane curve, contradicting the fact that CC is irreducible and nonplanar. Hence the second equation cuts out a nonzero conic on every plane fibre. It is a relative effective Cartier divisor of degree two in the plane bundle, and its equation remains a nonzerodivisor on every fibre. This proves flatness. ◻

Lemma 10.6 (Smooth members of a constrained pencil). Let y∈ℙ2y\in\mathbb P^2 have reduced conic fibre. A general line M⊂ℙ2M\subset\mathbb P^2 through yy has the following properties: S=φ−1(M)S=\varphi^{-1}(M) is a smooth cubic surface under π\pi, and the image π(ℓ)\pi(\ell) of the line in Lemma 10.3 passes through p0p_0. If P∈φ−1(y)P\in\varphi^{-1}(y) and π(P)≠p0\pi(P)\ne p_0, MM can be chosen so that P∉ℓP\notin\ell.

Proof. Write a cubic of the net as Sa=(a⋅f=0)S_a=(a\cdot f=0), where a∈ℙ2a\in\mathbb P^2 is a coefficient vector. The condition that it contains the conic over yy is a⋅y=0a\cdot y=0, a line in the parameter plane. For c∈C\{p0}c\in C\setminus\{p_0\}, the relation q(c)∥l(c)q(c)\parallel l(c) and the rank-two Jacobian of CC show that the unique cubic singular at cc has coefficient a=l(c)a=l(c). At p0p_0 its coefficient is q(p0)q(p_0). This defines the extension of the projection c↦l(c)c\mapsto l(c). Its image is not a line, since otherwise CC would lie in a plane through p0p_0. Hence only finitely many members of our parameter line are singular along CC.

On XX, Bertini makes a general member of the pencil smooth away from its base fibre. Along a smooth point of that fibre, φ\varphi is smooth. If the fibre is a union of two lines, it has one node; locally the conic equation has a nonzero derivative in a base direction there, since XX is smooth. Choosing MM transverse to that direction makes its inverse image smooth at the node. Thus a general SS is smooth, and the preceding paragraph ensures that its cubic image is smooth along CC too.

For a=[a0:a1:a2]a=[a_0:a_1:a_2], let ℓa⊂ℙ3\ell_a\subset\mathbb P^3 be the line defined by li(x)aj−lj(x)ai=0l_i(x)a_j-l_j(x)a_i=0 for 0≤i<j≤20\le i<j\le2. Independence of the lil_i shows that this is a line through p0p_0. Its equations imply a⋅(l×q)=0a\cdot(l\times q)=0, so it lies in SaS_a. If SaS_a is smooth, this line cannot meet CC away from p0p_0, for such an intersection would give a=l(c)a=l(c) and make SaS_a singular at cc. At p0p_0 it is transverse to CC: the tangent direction of CC in the ll-coordinates is q(p0)q(p_0), and a∦q(p0)a\not\parallel q(p_0). Its intersection with CC is therefore one. It is the line ℓ=ℓSa\ell=\ell_{S_a} of Lemma 10.3, since any other line has intersection at least two with 2A+ℓ2A+\ell. Distinct coefficient vectors a∈ℙ2a\in\mathbb P^2 give distinct lines ℓa\ell_a: projection from p0p_0 sends ℓa\{p0}\ell_a\setminus\{p_0\} to aa. Thus the line depends on the chosen cubic SaS_a, whereas their common point p0p_0 depends only on CC.

If P∉EP\notin E and π(P)≠p0\pi(P)\ne p_0, at most one coefficient aa, namely a=l(π(P))a=l(\pi(P)), makes ℓ\ell pass through PP. Avoid that coefficient. If P∈EP\in E lies above c≠p0c\ne p_0, the line ℓ\ell avoids PP automatically, as it meets CC only at p0p_0. ◻

Lemma 10.7. The set Σ\Sigma of nonreduced conic fibres is finite.

Proof. A nonreduced plane conic is a double line. If the rank-one locus of the conic equation contained a curve in the base, work at its general point and write the equation as x2+uq(y,z)+x^2+u q(y,z)+ higher terms in the transverse base parameter uu. Differentiation in the direction tangent to the rank-one locus vanishes along x=u=0x=u=0. The binary quadratic qq has a zero on the double line. At that zero the other base derivative vanishes as well, making the total space singular. This contradicts smoothness of XX. The rank-one locus is closed and hence is finite on the projective surface ℙ2\mathbb P^2. ◻