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Section 109

The pencil of sextic del Pezzo surfaces

Write V={y𝗍x=0}⊂ℙx2×ℙy2,C={y𝗍x=y𝗍Ax=y𝗍Bx=0}.V=\{y^{\mathsf t}x=0\}\subset\mathbb P^2_x\times\mathbb P^2_y, \qquad C=\{y^{\mathsf t}x=y^{\mathsf t}Ax=y^{\mathsf t}Bx=0\}. Here AA and BB are 3×33\times3 matrices, and the three displayed bilinear forms are linearly independent. Put N=⟨I,A,B⟩N=\langle I,A,B\rangle. We assume throughout this section that CC is smooth. Let π:X→V\pi\colon X\to V be its blow-up, let EE be the exceptional divisor, and let ϕ:X→ℙ1\phi\colon X\to\mathbb P^1 be the morphism defined by the pencil spanned by y𝗍Axy^{\mathsf t}Ax and y𝗍Bxy^{\mathsf t}Bx.

Lemma 109.1. The curve CC is connected of genus one. Both projections of CC to ℙ2\mathbb P^2 are embeddings onto smooth plane cubics.

Proof. The Koszul resolution for three divisors of bidegree (1,1)(1,1) gives H0(C,𝒪C)=ℂH^0(C,\mathcal O_C)=\mathbb C, and adjunction gives KC∼0K_C\sim0. Thus CC is a smooth connected curve of genus one. For fixed xx, its fibre under the first projection is the projectivized kernel of the matrix with rows x𝗍x^{\mathsf t}, (Ax)𝗍(Ax)^{\mathsf t} and (Bx)𝗍(Bx)^{\mathsf t}. If this matrix had rank at most one at a point of the image, CC would contain a projective line, contrary to irreducibility and genus one. Its rank is therefore exactly two everywhere over the image. Its kernel is consequently a line bundle locally on the determinant cubic. This identifies CC, as a scheme, with that cubic. The second projection is treated in the same way. Alternatively, the degree of either image is 𝒪C(1,0)=𝒪C(0,1)=3\mathcal O_C(1,0)=\mathcal O_C(0,1)=3, by intersection theory. ◻

Lemma 109.2. The plane cubic D={det(λI+μA+νB)=0}⊂ℙ(N)D=\{\det(\lambda I+\mu A+\nu B)=0\}\subset\mathbb P(N) is smooth. Every nonzero matrix in NN has rank at least two.

Proof. A rank-one matrix in NN would give a bilinear form l(x)m(y)l(x)m(y) vanishing identically on the irreducible curve CC. Hence one of its plane cubic images would lie in a line, which is impossible by Lemma 109.1. A nonzero rank-zero matrix is impossible. Suppose that [M][M] is a singular point of DD. Then MM has rank two. Choose generators xx and yy of its right and left kernels. The derivative of the determinant in a direction T∈NT\in N is a nonzero constant times y𝗍Txy^{\mathsf t}Tx. Thus (x,y)∈C(x,y)\in C. But both partial gradients of y𝗍Mxy^{\mathsf t}Mx vanish at (x,y)(x,y), since Mx=0Mx=0 and y𝗍M=0y^{\mathsf t}M=0. This gives a nontrivial linear dependence among the gradients of the three defining equations of CC, contradicting its smoothness. ◻

Lemma 109.3. Every fibre of ϕ\phi is a normal del Pezzo surface of degree six. It is either smooth, has precisely one A1A_1 singularity, or has precisely one A2A_2 singularity. Every singular point is disjoint from EE. If n1n_1 and n2n_2 count the singular fibres of the last two types, then n1+2n2=6n_1+2n_2=6.

Proof. A fibre is isomorphic to SM={y𝗍x=y𝗍Mx=0},M=μA+νB,S_M=\{y^{\mathsf t}x=y^{\mathsf t}Mx=0\},\qquad M=\mu A+\nu B, since blowing up the Cartier divisor CC on SMS_M changes neither SMS_M nor its scheme structure. The description below also verifies normality, so this observation does not presuppose it. No eigenvalue of MM can have a two-dimensional eigenspace: otherwise M−λIM-\lambda I would be a nonzero matrix in NN of rank at most one. Consequently MM is cyclic. Up to conjugation and an affine change M↦aM+bIM\mapsto aM+bI, its Jordan type is one of the following: three distinct eigenvalues; a block of size two and a distinct eigenvalue; a single block of size three.

The Jacobian criterion says that a singular point of SMS_M is a pair of right and left eigenvectors with the same eigenvalue, satisfying y𝗍x=0y^{\mathsf t}x=0. Three distinct eigenvalues give no such pair. For the second Jordan type take M=(010000001).M=\begin{pmatrix}0&1&0\\0&0&0\\0&0&1\end{pmatrix}. There is one singular point, namely ([1:0:0],[0:1:0])([1:0:0],[0:1:0]). On the chart x0=y1=1x_0=y_1=1, put a=x1a=x_1, b=x2b=x_2, and c=y2c=y_2. Eliminating y0y_0 gives bc(1−a)=a2bc(1-a)=a^2, which is an A1A_1 singularity. For the last Jordan type take M=(010001000).M=\begin{pmatrix}0&1&0\\0&0&1\\0&0&0\end{pmatrix}. The only singular point is ([1:0:0],[0:0:1])([1:0:0],[0:0:1]). On the chart x0=y2=1x_0=y_2=1, put a=x1a=x_1, c=y1−ac=y_1-a, and d=x2−a2d=x_2-a^2. Eliminating y0y_0 gives cd=a3cd=a^3, which is an A2A_2 singularity. This proves normality and the asserted list. Adjunction gives −KSM=𝒪SM(1,1)-K_{S_M}=\mathcal O_{S_M}(1,1) and KSM2=6K_{S_M}^2=6. If a singular point of SMS_M lay on CC, the two equations defining CC inside the smooth threefold VV would have dependent gradients. Thus all singular points avoid CC, and their lifts avoid EE.

Projection of the smooth cubic DD from [I]∉D[I]\notin D gives a finite map D→ℙ1D\to\mathbb P^1 of degree three. Its fibre over [μ:ν][\mu:\nu] records the eigenvalues of μA+νB\mu A+\nu B. Ordinary ramification gives the second Jordan type, and ramification of index three gives the third. Riemann–Hurwitz therefore gives n1+2n2=6n_1+2n_2=6. ◻

Lemma 109.4. For an A1A_1 fibre, its minimal resolution is the blow-up of ℙ2\mathbb P^2 at a point p1p_1, a point p2p_2 infinitely near p1p_1, and an ordinary point p3p_3 off the corresponding tangent line. Writing l,e1,e2,e3l,e_1,e_2,e_3 for the usual total-transform classes, its (−2)(-2)-curve has class e1−e2e_1-e_2, and its four (−1)(-1)-curves have classes e2,e3,l−e1−e2,l−e1−e3.e_2,\quad e_3,\quad l-e_1-e_2,\quad l-e_1-e_3. The first projection contracts the first two lines and the second projection contracts the last two. The singular point lies on exactly the images of e2e_2 and l−e1−e3l-e_1-e_3.

For an A2A_2 fibre, the three blow-up centres form a curvilinear cluster whose third point is off the strict transform of its tangent line. The (−2)(-2)-curves have classes e1−e2e_1-e_2 and e2−e3e_2-e_3. There are exactly two (−1)(-1)-curves, of classes e3e_3 and l−e1−e2l-e_1-e_2. Their images pass through the singular point, and each projection contracts one of them.

Proof. The first projection is the graph of the rational map x↦x×Mxx\mapsto x\mathbin{\times}Mx, so its centres are the eigenscheme of MM. In the A1A_1 normal form, near [1:0:0][1:0:0] its ideal is (b,a2)(b,a^2), and the other centre is [0:0:1][0:0:1]. In the A2A_2 normal form its ideal is (b−a2,a3)(b-a^2,a^3). Successive ordinary blow-ups give the stated clusters. The curve classes and their intersections follow directly. To check completeness, a (−1)(-1)-curve on the resolution is either an exceptional curve or has class dl−m1e1−m2e2−m3e3dl-m_1e_1-m_2e_2-m_3e_3 with nonnegative integers mim_i. The equations 3d−∑mi=13d-\sum m_i=1 and d2−∑mi2=−1d^2-\sum m_i^2=-1 give d≤1d\le1 by Cauchy–Schwarz. The degree-one possibilities are then exactly the lines specified above. The second projection and the incidences with the singularities follow either by transposition or by intersecting these classes with the (−2)(-2)-curves. ◻

Example 109.5. Take A=(010001000),B=(000001100).A=\begin{pmatrix}0&1&0\\0&0&1\\0&0&0\end{pmatrix},\qquad B=\begin{pmatrix}0&0&0\\0&0&1\\1&0&0\end{pmatrix}. Then det(λI+μA+νB)=λ3+μν(μ+ν).\det(\lambda I+\mu A+\nu B) =\lambda^3+\mu\nu(\mu+\nu). This cubic is smooth: its three partial derivatives have no common projective zero. The first projection identifies CC with x02x2−x0x12+x1x22=0x_0^2x_2-x_0x_1^2+x_1x_2^2=0, which is also a smooth plane cubic. There are three singular fibres, over μν(μ+ν)=0\mu\nu(\mu+\nu)=0, and each has an A2A_2 singularity. Thus the worst singular-fibre case really occurs for smooth members of Family 3.7.

Lemma 109.6. The automorphism group of XX is finite.

Proof. Put H1=π*𝒪V(1,0)H_1=\pi^*\mathcal O_V(1,0), H2=π*𝒪V(0,1)H_2=\pi^*\mathcal O_V(0,1), and F=ϕ*𝒪ℙ1(1)F=\phi^*\mathcal O_{\mathbb P^1}(1). These are independent nef classes. The exceptional fibre of π\pi has intersections (0,0,1)(0,0,1) with them. The strict transform of a fibre of the first projection of VV meeting CC has intersections (0,1,0)(0,1,0): the two pencil sections restrict to linear polynomials with the same zero, so their ratio is constant after blowing up. The second projection similarly supplies a curve with intersections (1,0,0)(1,0,0). Hence the nef cone is generated by H1,H2,FH_1,H_2,F. The connected automorphism group fixes these rays and their integral primitive classes. It therefore descends via both plane projections, and via π\pi, to an automorphism of VV preserving CC. Its action on CC preserves the degree-three line bundle 𝒪C(1,0)\mathcal O_C(1,0). The group of automorphisms of an elliptic curve preserving a positive-degree line bundle is finite: its translation subgroup is contained in the kernel of the associated isogeny, and the subgroup fixing an origin is finite. The kernel of this action fixes both plane cubic images pointwise, hence is the identity on both planes and on XX. Thus the connected automorphism group is trivial. Since the automorphism group of a Fano variety is an algebraic group of finite type, it is finite. ◻

Lemma 109.7. Write H=π*𝒪V(1,1)H=\pi^*\mathcal O_V(1,1) and F=ϕ*𝒪ℙ1(1)F=\phi^*\mathcal O_{\mathbb P^1}(1). Then −KX=H+F,(−KX)3=24,h0(X,−mKX)=4m3+6m2+4m+1(m≥0).-K_X=H+F,\qquad (-K_X)^3=24,\qquad h^0(X,-mK_X)=4m^3+6m^2+4m+1\quad(m\ge0). If f,g∈H0(V,𝒪V(1,1))f,g\in H^0(V,\mathcal O_V(1,1)) generate the pencil, the fifteen anticanonical sections are the products of the eight bilinear sections on VV with the two base coordinates, modulo the single relation defining the graph of the pencil.

Proof. The blow-up is the complete intersection of divisors of multidegrees (1,1,0)(1,1,0) and (1,1,1)(1,1,1) in ℙ2×ℙ2×ℙ1\mathbb P^2\times\mathbb P^2\times\mathbb P^1. Indeed, the ideal (f,g)(f,g) is a regular sequence on VV, so its blow-up is its usual incidence graph. Adjunction gives −KX=𝒪X(1,1,1)-K_X=\mathcal O_X(1,1,1), which is ample. Its cube is 2424 by intersection in this product. The Koszul resolution, twisted by 𝒪(m,m,m)\mathcal O(m,m,m), has no higher cohomology contributing to its space of sections. It gives h0(X,−mKX)=(m+1)(m+22)2−(2m+1)(m+12)2+m(m2)2=4m3+6m2+4m+1.h^0(X,-mK_X)= (m+1)\binom{m+2}{2}^{\!2} -(2m+1)\binom{m+1}{2}^{\!2} +m\binom m2^{\!2} =4m^3+6m^2+4m+1. For m=0,1m=0,1 the same formula follows directly, with the zero binomial terms omitted. Finally, h0(V,𝒪V(1,1))=8h^0(V,\mathcal O_V(1,1))=8; the graph equation is the unique relation among its sixteen products with the base coordinates. This proves the last assertion. ◻

Lemma 109.8. Put H1=π*𝒪V(1,0)H_1=\pi^*\mathcal O_V(1,0), H2=π*𝒪V(0,1)H_2=\pi^*\mathcal O_V(0,1), and F=ϕ*𝒪ℙ1(1)F=\phi^*\mathcal O_{\mathbb P^1}(1). The morphisms given by (F,Hi)(F,H_i) are blow-ups of smooth elliptic curves in ℙ1×ℙ2\mathbb P^1\times\mathbb P^2. Their exceptional divisors are D1=F+2H1−H2=3H1−E,D2=F+2H2−H1=3H2−E.D_1=F+2H_1-H_2=3H_1-E,\qquad D_2=F+2H_2-H_1=3H_2-E. The divisor DiD_i is also the strict transform of the inverse image of the plane cubic CiC_i under the iith projection of VV.

Proof. Consider (ϕ,p1)(\phi,p_1). Over ([μ:ν],x)([\mu:\nu],x) the remaining coordinate yy satisfies y𝗍x=y𝗍(μA+νB)x=0y^{\mathsf t}x=y^{\mathsf t}(\mu A+\nu B)x=0. There is a unique solution except along the eigencurve Z1={([μ:ν],x):x×(μA+νB)x=0}.Z_1=\{([\mu:\nu],x):x\mathbin{\times}(\mu A+\nu B)x=0\}. The smooth determinant cubic in Lemma 109.2 maps isomorphically to Z1Z_1 by taking the right kernel of λI+μA+νB\lambda I+\mu A+\nu B. The kernel is a line everywhere. Conversely, the eigenvalue is recovered regularly on a chart where a coordinate of xx is nonzero. This proves that Z1Z_1 is smooth and that the indicated map is a closed immersion.

The two-row matrix with rows x𝗍x^{\mathsf t} and ((μA+νB)x)𝗍((\mu A+\nu B)x)^{\mathsf t} has rank one along Z1Z_1 and rank two elsewhere. Locally a unit entry reduces its incidence equations to the usual graph of two generators of the ideal of Z1Z_1. Since Z1Z_1 is smooth of codimension two, this graph is its blow-up. This proves the assertion about the morphism. The canonical divisor formula gives D1=(2F+3H1)−(−KX)=F+2H1−H2.D_1=(2F+3H_1)-(-K_X)=F+2H_1-H_2. Here −KX=H1+H2+F-K_X=H_1+H_2+F.

The projection of Z1Z_1 to the first plane is C1C_1: its determinant equation is det(x,Ax,Bx)=0\det(x,Ax,Bx)=0, the equation of that plane cubic. Over x∈C1x\in C_1, the two pencil equations restrict proportionally to the first-projection fibre, so its strict transform is contracted by (ϕ,p1)(\phi,p_1). The inverse image of C1C_1 in VV contains CC with multiplicity one. Its strict transform therefore has class 3H1−E3H_1-E and is the exceptional divisor just described. The second assertion is obtained by transposing the matrices. ◻