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Section 111

Quintic del Pezzo sections

Lemma 111.1. The degree-three line bundles L1=𝒪C(1,0)L_1=\mathcal O_C(1,0) and L2=𝒪C(0,1)L_2=\mathcal O_C(0,1) are not isomorphic.

Proof. Both plane embeddings are defined by their complete linear systems. If L1≃L2L_1\simeq L_2, a projective change of coordinates identifies these embeddings. The bilinear equation of VV then restricts on CC to a quadratic form in the coordinates of one plane. A nonzero quadratic form cannot vanish on a smooth plane cubic. Therefore this quadratic form vanishes identically, so the matrix of the bilinear equation is skew-symmetric. A skew-symmetric matrix of size three is singular. This contradicts the smoothness of VV. ◻

Lemma 111.2. Put H1=π*𝒪V(1,0)H_1=\pi^*\mathcal O_V(1,0) and H2=π*𝒪V(0,1)H_2=\pi^*\mathcal O_V(0,1). For every point p∈Xp\in X, a general member T∈|H1|T\in|H_1| containing pp is a smooth del Pezzo surface of degree five. The same holds with H1H_1 and H2H_2 interchanged. More precisely, TT is the blow-up of ℙy2\mathbb P^2_y at four points p0,p1,p2,p3p_0,p_1,p_2,p_3 in general position, and H1|T=l−e0,H2|T=l,F|T=2l−e0−e1−e2−e3,E|T=e1+e2+e3.H_1|_T=l-e_0,\qquad H_2|_T=l,\qquad F|_T=2l-e_0-e_1-e_2-e_3,\qquad E|_T=e_1+e_2+e_3. Here ll is the pull-back of a line and the eie_i are the exceptional curves.

Proof. Let qq be the first plane image of pp. Write CiC_i for the two smooth plane cubic images of CC. Choose a general line L⊂ℙx2L\subset\mathbb P^2_x through qq. It meets C1C_1 transversely in three distinct points x1,x2,x3x_1,x_2,x_3. We may also require that its point [L]∈ℙy2[L]\in\mathbb P^2_y does not belong to C2C_2: the pencil of lines through qq is a line in ℙy2\mathbb P^2_y, and cannot be contained in the smooth cubic C2C_2.

The surface VL=V∩(L×ℙy2)V_L=V\cap(L\times\mathbb P^2_y) is the incidence surface of points of LL and lines of ℙx2\mathbb P^2_x. Its second projection is the blow-up of ℙy2\mathbb P^2_y at p0=[L]p_0=[L]. Indeed, for y≠[L]y\ne[L] the unique point above yy is L∩yL\cap y, whereas the fibre over [L][L] is LL. Let ci=(xi,yi)c_i=(x_i,y_i) be the three points of C∩VLC\cap V_L. They are distinct and avoid this exceptional curve, by the choice [L]∉C2[L]\notin C_2. Since VLV_L meets CC transversely, its inverse image TT in the blow-up XX is the blow-up of VLV_L at c1,c2,c3c_1,c_2,c_3. In particular it is smooth and is the blow-up of ℙy2\mathbb P^2_y at p0,p1=y1,p2=y2,p3=y3p_0,p_1=y_1,p_2=y_2,p_3=y_3.

These four points are in general position. They are distinct because C→C2C\to C_2 is an embedding and p0∉C2p_0\notin C_2. If p0,pi,pjp_0,p_i,p_j were collinear, the three corresponding lines L,yi,yjL,y_i,y_j in ℙx2\mathbb P^2_x would be concurrent. As xi=L∩yix_i=L\cap y_i and xj=L∩yjx_j=L\cap y_j, this would give xi=xjx_i=x_j, a contradiction. If p1,p2,p3p_1,p_2,p_3 were collinear, the divisor c1+c2+c3c_1+c_2+c_3 on CC would belong to both |L1||L_1| and |L2||L_2|. This contradicts Lemma 111.1. Thus TT is a smooth del Pezzo surface of degree five. The displayed divisor classes follow from the two projections and F=H1+H2−EF=H_1+H_2-E.

This construction includes points on either component of every singular conic fibre of X→ℙx2X\to\mathbb P^2_x, as well as their intersection: the Cartier inverse image of every line through qq contains the entire fibre over qq. In particular there is no exception for p∈Ep\in E. Transversality of LL to C1C_1 at qq, when q∈C1q\in C_1, is compatible with all the preceding choices. ◻

Remark 111.3. For this surface TT, put D1=3H1−ED_1=3H_1-E and D2=3H2−ED_2=3H_2-E. The divisor D1|TD_1|_T is the union of the three disjoint exceptional lines of classes l−e0−eil-e_0-e_i, while D2|T∼3l−e1−e2−e3=−KT+e0.D_2|_T\sim3l-e_1-e_2-e_3=-K_T+e_0. The conic bundle T→LT\to L has precisely three singular fibres, ei+(l−e0−ei)e_i+(l-e_0-e_i). Thus the choice of TT does not remove points on the reducible conic fibres; it places all of them on an ordinary smooth del Pezzo surface with an explicit ten-line configuration.

Lemma 111.4. For the general surface TT chosen in Lemma 111.2, the curve (3H2−E)|T(3H_2-E)|_T is smooth and irreducible, of class 3l−e1−e2−e33l-e_1-e_2-e_3.

Proof. The inverse image of C2C_2 in VV under the second plane projection is a ℙ1\mathbb P^1-bundle containing CC as a section. Its strict transform D2D_2 in XX is isomorphic to it, since blowing up a Cartier divisor on a smooth surface does not change the surface. For a point y∈C2y\in C_2, the corresponding ruling fibre is the line represented by yy in the first plane. The line LL defining TT is different from each of these lines, because [L]∉C2[L]\notin C_2. It therefore meets each ruling fibre once. Thus T∩D2T\cap D_2 is a section of this bundle, isomorphic to C2C_2. Its class was computed in Remark 111.3. ◻

Lemma 111.5. For D∈|A|D\in|A|, one has SX(D)=69/128S_X(D)=69/128. The divisorial positive and negative parts of L−uAL-uA are (P(u),N(u))={((1−u)A+B+F,0),0≤u≤1,((3−2u)B+(2−u)F,(u−1)(F+2B−A)),1≤u≤3/2.(P(u),N(u))= \begin{cases} ((1-u)A+B+F,0),&0\le u\le1,\\ ((3-2u)B+(2-u)F,(u-1)(F+2B-A)),&1\le u\le3/2. \end{cases}

Proof. The divisors A,B,FA,B,F are nef. The divisor J=F+2B−AJ=F+2B-A is the exceptional divisor of the contraction to ℙ1×ℙ2\mathbb P^1\times\mathbb P^2 given by F,BF,B. A fibre of JJ has intersection one with AA and zero with B,FB,F, so its intersection with JJ is −1-1. Thus u>1u>1 forces the indicated fixed multiplicity along JJ. Subtraction leaves the stated nef divisor until u=3/2u=3/2. For u>3/2u>3/2 one has (L−uA)BF=3−2u<0(L-uA)BF=3-2u<0, excluding pseudoeffectivity. The volumes are 6u2−27u+246u^2-27u+24 on [0,1][0,1] and −12u3+60u2−99u+54-12u^3+60u^2-99u+54 on [1,3/2][1,3/2]. Their integral, divided by 2424, is 69/12869/128. ◻

Remark 111.6. The preceding flag alone cannot settle points of the original exceptional divisor. In a smooth quintic section D=Blp0,p1,p2,p3ℙ2D=\operatorname{Bl}_{p_0,p_1,p_2,p_3}\mathbb P^2, write hh for the line class and e0,e1,e2,e3e_0,e_1,e_2,e_3 for the exceptional classes. Then A|D=h−e0A|_D=h-e_0, B|D=hB|_D=h, F|D=2h−∑eiF|_D=2h-\sum e_i, and E|D=e1+e2+e3E|_D=e_1+e_2+e_3. Direct surface Zariski integration gives S(WD;ei)=6964>1(i=1,2,3),S(WD;h−e0−ei)=139128>1.S(W^D;e_i)=\frac{69}{64}>1\quad(i=1,2,3),\qquad S(W^D;h-e_0-e_i)=\frac{139}{128}>1. Consequently further refinement of this same surface flag cannot prove a local threshold exceeding one at a point of eie_i. This is a limitation of the chosen refinement, not an instability statement about XX.

Lemma 111.7. The moving section spaces on DD used below are complete in every sufficiently large divisible degree, for each rational uu in the corresponding interval. In particular, the numerical moments are computed with the original normalization (−KX)3=24(-K_X)^3=24.

Proof. Let ρ2:X→Y=ℙ1×ℙ2\rho_2:X\longrightarrow Y=\mathbb P^1\times\mathbb P^2 be the birational morphism defined by FF and BB, with exceptional divisor D2D_2. Recall that A=F+2B−D2A=F+2B-D_2, so the image of a general D∈|A|D\in|A| is an integral divisor of bidegree (1,2)(1,2) containing the centre Z2Z_2 of ρ2\rho_2. Moreover, (F+B)|D=3l−e0−e1−e2−e3=−KD.(F+B)|_D=3l-e_0-e_1-e_2-e_3=-K_D. The six sections of 𝒪Y(1,1)\mathcal O_Y(1,1) restrict independently to DD: a relation would give a divisor of bidegree (1,1)(1,1) containing its image of bidegree (1,2)(1,2), which is impossible. Since h0(D,−KD)=6h^0(D,-K_D)=6 and −KD-K_D is very ample, these sections give the complete anticanonical embedding. Thus ρ2|D\rho_2|_D is an isomorphism onto a smooth divisor of bidegree (1,2)(1,2), and D2|DD_2|_D is its smooth elliptic curve Z2Z_2.

For rational 0≤u<10\leqslant u<1, the divisor PX(u)=(1−u)A+B+FP_X(u)=(1-u)A+B+F on XX is ample. After clearing denominators, Serre vanishing applied to 0→𝒪X(mPX(u)−D)→𝒪X(mPX(u))→𝒪D(mP(u))→00\longrightarrow\mathcal O_X(mP_X(u)-D) \longrightarrow\mathcal O_X(mP_X(u)) \longrightarrow\mathcal O_D(mP(u))\longrightarrow0 gives surjectivity of restriction for all sufficiently large divisible mm.

For 1≤u≤3/21\leqslant u\leqslant3/2, removing the fixed divisor m(u−1)D2m(u-1)D_2 identifies the global moving sections with the sections of 𝒪Y(a,b)\mathcal O_Y(a,b), where a=m(2−u),b=m(3−2u).a=m(2-u),\qquad b=m(3-2u). Both integers are non-negative. As D⊂YD\subset Y has bidegree (1,2)(1,2), the restriction sequence is 0→𝒪Y(a−1,b−2)→𝒪Y(a,b)→𝒪D(mP(u))→0.0\longrightarrow\mathcal O_Y(a-1,b-2) \longrightarrow\mathcal O_Y(a,b) \longrightarrow\mathcal O_D(mP(u))\longrightarrow0. Its first cohomology vanishes: H1(ℙ1,𝒪(a−1))=0H^1(\mathbb P^1,\mathcal O(a-1))=0 for a≥0a\geqslant0, and H1(ℙ2,𝒪(b−2))=0H^1(\mathbb P^2,\mathcal O(b-2))=0. Thus the moving restrictions are complete also on this interval.

Refining on DD by a flag curve gives the usual surface Zariski-decomposition bounds. One may enlarge the resulting spaces on the curve to complete series, since a basis compatible with the point filtration extends to a compatible basis of the larger space and all added vanishing orders are non-negative. This only increases the moments. Rounding errors vanish in the normalized limit. Finally, the fixed divisor removed on the second interval restricts to m(u−1)C2m(u-1)C_2; it is retained in the refined divisor and contributes 7(C2⋅T)p/3847(C_2\cdot T)_p/384 to the point moment. Omitting this contribution would give an incorrect calculation at points of C2C_2. ◻

Lemma 111.8. Let DD be the blow up of ℙ2\mathbb P^2 at four points in general position, with classes l,e0,e1,e2,e3l,e_0,e_1,e_2,e_3, and put T=2l−e1−e2−e3T=2l-e_1-e_2-e_3. Suppose that the refinement by DD has moving divisors P(u)={(4−u)l−(2−u)e0−e1−e2−e3,0≤u≤1,(7−4u)l−(2−u)(e0+e1+e2+e3),1≤u≤3/2,P(u)=\begin{cases} (4-u)l-(2-u)e_0-e_1-e_2-e_3,&0\leqslant u\leqslant1,\\ (7-4u)l-(2-u)(e_0+e_1+e_2+e_3),&1\leqslant u\leqslant3/2, \end{cases} and fixed part (u−1)C2(u-1)C_2 on the second interval, where C2C_2 is an irreducible curve of class 3l−e1−e2−e33l-e_1-e_2-e_3. Let pp be outside the ten (−1)(-1)-curves of DD, and let Q∈|l−e0|Q\in|l-e_0| contain pp. With the threefold normalization (−KX)3=24(-K_X)^3=24, we have S(W•,•D;Q)≤245288,S(W•,•,•D,Q;p)≤133144+7384(C2⋅Q)p≤11271152<1.S(W^D_{\bullet,\bullet};Q)\leqslant\frac{245}{288},\qquad S(W^{D,Q}_{\bullet,\bullet,\bullet};p) \leqslant\frac{133}{144}+\frac{7}{384}(C_2\cdot Q)_p \leqslant\frac{1127}{1152}<1. In particular, if SX(D)=69/128S_X(D)=69/128, then δp(X)≥1152/1127>1\delta_p(X)\geqslant1152/1127>1.

Proof. The curve QQ is a smooth rational curve, since the reducible fibres of |l−e0||l-e_0| are the unions ei+(l−e0−ei)e_i+(l-e_0-e_i), for 1≤i≤31\leqslant i\leqslant3. Put Lij=l−ei−ej,R=L12+L13+L23,a=3−2u,b=2−u,k=8−5u−2v,r=2−u−v.\begin{gathered} L_{ij}=l-e_i-e_j,\qquad R=L_{12}+L_{13}+L_{23},\\ a=3-2u,\quad b=2-u,\quad k=8-5u-2v,\quad r=2-u-v. \end{gathered} The four curves e0,L12,L13,L23e_0,L_{12},L_{13},L_{23} are pairwise disjoint. The positive and negative parts M(u,v),N(u,v)M(u,v),N(u,v) of P(u)−vQP(u)-vQ are as follows. The last column records M(u,v)⋅QM(u,v)\cdot Q.

range M(u,v)M(u,v) N(u,v)N(u,v) M(u,v)⋅QM(u,v)\cdot Q
0≤u≤10\leqslant u\leqslant1, 0≤v≤2−u0\leqslant v\leqslant2-u P(u)−vQP(u)-vQ 00 22
0≤u≤10\leqslant u\leqslant1, 2−u≤v≤5/2−u2-u\leqslant v\leqslant5/2-u (5−2u−2v)T(5-2u-2v)T (v+u−2)(e0+R)(v+u-2)(e_0+R) 2(5−2u−2v)2(5-2u-2v)
1≤u≤3/21\leqslant u\leqslant3/2, 0≤v≤a0\leqslant v\leqslant a P(u)−vQP(u)-vQ 00 5−3u5-3u
1≤u≤4/31\leqslant u\leqslant4/3, a≤v≤ba\leqslant v\leqslant b kT−re0kT-re_0 (v−a)R(v-a)R 2k−r2k-r
4/3≤u≤3/24/3\leqslant u\leqslant3/2, a≤v≤6−4ua\leqslant v\leqslant6-4u kT−re0kT-re_0 (v−a)R(v-a)R 2k−r2k-r
1≤u≤4/31\leqslant u\leqslant4/3, b≤v≤4−5u/2b\leqslant v\leqslant4-5u/2 kTkT (v−a)R+(v−b)e0(v-a)R+(v-b)e_0 2k2k

These are Zariski decompositions: the listed negative curves are disjoint, the positive part is orthogonal to each component of the negative part, and its intersection with every (−1)(-1)-curve is non-negative. Since the cone of curves is generated by the ten (−1)(-1)-curves, the positive part is nef. The upper endpoints are the pseudoeffective thresholds. At these endpoints the positive part is zero, except when 4/3≤u≤3/24/3\leqslant u\leqslant3/2, where it is a multiple of the nef class 2l−e0−e1−e2−e32l-e_0-e_1-e_2-e_3 of square zero. Increasing vv then gives negative intersection with this nef class, or with TT, as appropriate.

For completeness, the squares in the six rows are, respectively, 9−4u−4v,(5−2u−2v)2,33−40u+12u2−2v(5−3u),k2−r2,k2−r2,k2.9-4u-4v,\quad(5-2u-2v)^2,\quad 33-40u+12u^2-2v(5-3u),\quad k^2-r^2,\quad k^2-r^2,\quad k^2. Integrating these polynomials over their indicated ranges gives ∫∫M(u,v)2dvdu=24536,∫∫(M(u,v)⋅Q)2dvdu=13318,\int\!\!\int M(u,v)^2\,dv\,du=\frac{245}{36},\qquad \int\!\!\int (M(u,v)\cdot Q)^2\,dv\,du=\frac{133}{18}, where each integral means the sum over the six rows. Moreover, ∫13/2∫0t(u)(u−1)(M(u,v)⋅Q)dvdu=796.\int_1^{3/2}\int_0^{t(u)}(u-1)(M(u,v)\cdot Q)\,dv\,du =\frac{7}{96}. Here t(u)t(u) is the upper endpoint in the table. Since pp is outside the ten negative curves, N(u,v)|QN(u,v)|_Q has zero multiplicity at pp. The Abban–Zhuang formula, with factors 3/243/24 and 6/246/24, now gives the two asserted bounds. Finally, C2⋅Q=3C_2\cdot Q=3, so (C2⋅Q)p≤3(C_2\cdot Q)_p\leqslant3. Applying the flag estimate proves the assertion. ◻

Remark 111.9. If QQ is smooth and pp is allowed to lie on a negative curve, the complete point bound is S(W•,•,•D,Q;p)≤133144+7384(C2⋅Q)p+13576ordp(e0|Q)+291152ordp((L12+L13+L23)|Q).\begin{aligned} S(W^{D,Q}_{\bullet,\bullet,\bullet};p) \leqslant{}&\frac{133}{144}+\frac{7}{384}(C_2\cdot Q)_p +\frac{13}{576}\operatorname{ord}_p(e_0|_Q)\\ &+\frac{29}{1152}\operatorname{ord}_p((L_{12}+L_{13}+L_{23})|_Q). \end{aligned} The last four intersections have multiplicity one whenever they occur. This gives 545/576545/576 at a point of e0e_0, since C2⋅e0=0C_2\cdot e_0=0. At a point of L12∪L13∪L23L_{12}\cup L_{13}\cup L_{23} it gives at most 1135/11521135/1152 if (C2⋅Q)p≤2(C_2\cdot Q)_p\leqslant2. The upper bound becomes 289/288289/288 for contact three, so this last configuration requires another flag.

Lemma 111.10. Let ℓ\ell be a line through the singular point of an A1A_1 or A2A_2 fibre, and suppose that the first plane projection contracts ℓ\ell. Put D2=3H2−ED_2=3H_2-E. If p∈ℓ\(E∪D2)p\in\ell\setminus(E\cup D_2), there is a smooth degree-five del Pezzo surface T∈|H2|T\in|H_2| through pp such that pp is on none of its ten (−1)(-1)-curves.

For an A1A_1 fibre, the support of D2∩ℓD_2\cap\ell consists of its singular point and one further point, at which ℓ\ell meets the other line contracted by the second plane projection. This further point is smooth on the fibre; it may also belong to EE. For an A2A_2 fibre, D2∩ℓD_2\cap\ell is supported only at its singular point, with multiplicity two. The same assertions hold after interchanging the two projections.

Proof. Write π(p)=(x0,y)\pi(p)=(x_0,y) and let c0=(x0,y0)c_0=(x_0,y_0) be the unique point of CC above x0x_0. The line ℓ\ell is the strict transform of the first-projection fibre over x0x_0. The divisor D2D_2 is the strict transform of the inverse image of the plane cubic C2C_2 under the second projection. Thus p∉E∪D2p\notin E\cup D_2 implies y∉C2y\notin C_2.

Choose a general line M⊂ℙy2M\subset\mathbb P^2_y through yy. The proof of Lemma 111.2, with the projections interchanged, identifies its inverse image TT with the blow-up of ℙx2\mathbb P^2_x at four points r=[M],x1,x2,x3r=[M],x_1,x_2,x_3, where (xi,yi)=ci∈C(x_i,y_i)=c_i\in C and {y1,y2,y3}=M∩C2\{y_1,y_2,y_3\}=M\cap C_2. We may take these four points in general position. We may also assume r≠x0r\ne x_0 and M∌y0M\not\ni y_0. Consequently pp is on none of the four exceptional curves.

The line through rr and xix_i in ℙx2\mathbb P^2_x is precisely the line represented by yiy_i: both points lie on it. Thus pp is on the strict transform of this line only if yi(x0)=0y_i(x_0)=0. There are only finitely many such points yiy_i on C2C_2, and none equals yy, since y∉C2y\notin C_2. Avoiding the finitely many lines joining yy to these points ensures that pp lies on none of the three curves of classes l−e0−eil-e_0-e_i.

Finally, suppose that infinitely many choices of MM put pp on a line through two of x1,x2,x3x_1,x_2,x_3. Projection of C1C_1 from x0x_0 gives the degree-two morphism defined by |L1−c0||L_1-c_0|; let ι\iota be its involution. Projection of C2C_2 from y∉C2y\notin C_2 gives a degree-three morphism g:C→ℙ1g\colon C\to\mathbb P^1. The supposed incidences give infinitely many points cc with g(c)=g(ι(c))g(c)=g(\iota(c)). Therefore these two morphisms are identical, and gg factors through the quotient by ι\iota. Its degree would be even, a contradiction. Only finitely many further choices of MM are excluded. This proves the first assertion.

For completeness, the exceptional points can be read directly from the Jordan forms. At an A1A_1 fibre take A=(010000001),ℓ={x=[1:0:0],y=[0:s:t]}.A=\begin{pmatrix}0&1&0\\0&0&0\\0&0&1\end{pmatrix}, \qquad \ell=\{x=[1:0:0],\ y=[0:s:t]\}. If B=(bij)B=(b_{ij}) defines the other pencil member, the plane cubic C2C_2 restricted to this line has equation, up to nonzero scalar, st(b10s+b20t)=0.st(b_{10}s+b_{20}t)=0. The last factor cuts out C∩ℓC\cap\ell. Removing it in the blow-up leaves st=0st=0. The point [s:t]=[1:0][s:t]=[1:0] is the node, and [s:t]=[0:1][s:t]=[0:1] is the smooth intersection with the good line contracted by the second projection. Smoothness of CC ensures b10≠0b_{10}\ne0, so CC misses the node. The other point may coincide with C∩ℓC\cap\ell, but the strict-transform computation still gives one residual intersection there. For an A2A_2 fibre take AA to be the nilpotent block of size three. On the same line the equation is s2(b10s+b20t)=0.s^2(b_{10}s+b_{20}t)=0. Here b20≠0b_{20}\ne0, since CC misses the singular point [s:t]=[0:1][s:t]=[0:1]. After removing the base-curve factor, the intersection is twice this point. Transposing the matrices proves the symmetric assertions. ◻