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Section 104

Reduction to the double conics

104.1 The two remaining quintic surfaces

We retain the notation EE, RR, HH for the two exceptional divisors and the pull-back of a plane. In particular, E∩R=⌀E\cap R=\varnothing. Let S∈|H−R|S\in|H-R|, and put Da=ah−e1−e2−e3−e4D_a=ah-e_1-e_2-e_3-e_4 on its minimal resolution, where hh is the pull-back of a line and the eie_i are total-transform exceptional classes. The latter convention is important: ei2=−1e_i^2=-1 and ei⋅ej=0e_i\cdot e_j=0 for i≠ji\ne j.

Lemma 104.1. Suppose that SS has singularities 2A12A_1 or A3A_3. The conic bundle on SS has a unique non-reduced fibre 2ℓ2\ell. Its minimal resolution is the blow-up of the plane at a curvilinear scheme of type (2,2)(2,2) or (4)(4), respectively. The pencil of conics through this scheme is base-point-free on the resolution and has class F=2h−e1−e2−e3−e4.F=2h-e_1-e_2-e_3-e_4. In type 2A12A_1, the only other singular member is L1+L2L_1+L_2, where L1=h−e1−e2,L2=h−e3−e4.L_1=h-e_1-e_2,\qquad L_2=h-e_3-e_4. The curves L1L_1 and L2L_2 are smooth (−1)(-1)-curves, intersect once, and avoid the singularities of SS. In type A3A_3, every fibre other than 2ℓ2\ell is smooth.

Proof. Let Π\Pi be the plane defining SS, and let Z=C∩ΠZ=C\cap\Pi. By Lemma 103.2, ZZ is curvilinear of type (2,2)(2,2) or (4)(4), respectively. It is the complete intersection of the two restricted quadrics. In type (2,2)(2,2) let λ=0\lambda=0 be the line joining the two support points; its square vanishes on both length-two parts of ZZ. In type (4)(4) let λ=0\lambda=0 be the tangent line to ZZ. In 𝒪Z≅ℂ[t]/(t4)\mathcal O_Z\cong\mathbb C[t]/(t^4) its equation belongs to (t2)(t^2), so its square again vanishes on ZZ. The twisted Koszul resolution 0→𝒪Π(−2)→𝒪Π⊕2→ℐZ(2)→00\longrightarrow\mathcal O_{\Pi}(-2) \longrightarrow\mathcal O_{\Pi}^{\oplus2} \longrightarrow\mathcal I_Z(2)\longrightarrow0 shows that H0(Π,ℐZ(2))H^0(\Pi,\mathcal I_Z(2)) is exactly the given pencil. Thus λ2\lambda^2 is one of its members.

Write the pencil as ⟨q,λ2⟩\langle q,\lambda^2\rangle, with q=0q=0 smooth. Such a choice exists: Bertini gives smoothness away from ZZ, and curvilinearity makes the differential of every member independent of λ2\lambda^2 nonzero at each support point of ZZ. In type (2,2)(2,2), the line meets q=0q=0 in two distinct points. Suitable coordinates give q=xz−y2q=xz-y^2 and λ=y\lambda=y. Its only singular members are y2y^2 and xzxz, the latter being the two tangent lines to q=0q=0 at these points. In type (4)(4), the line is tangent to q=0q=0, and we may take q=xz−y2q=xz-y^2 and λ=x\lambda=x. Every finite member xz−y2+tx2xz-y^2+t x^2 is smooth. The graph equation identifies the fibres on SS with these plane conics scheme-theoretically. In particular, there is precisely one non-reduced fibre, namely 2ℓ2\ell.

A length-kk part of ZZ has local ideal (v,uk)(v,u^k). Its kk successive point blow-ups resolve the pencil; their first k−1k-1 exceptional curves form the Ak−1A_{k-1} chain contracted on SS. All base multiplicities are one, giving F=2h−e1−e2−e3−e4F=2h-e_1-e_2-e_3-e_4. In type (2,2)(2,2) the two tangent lines have strict transforms L1=h−e1−e2L_1=h-e_1-e_2 and L2=h−e3−e4L_2=h-e_3-e_4. They are smooth, have self-intersection −1-1, intersect once away from the base scheme, and are disjoint from the exceptional roots e1−e2,e3−e4e_1-e_2,e_3-e_4. In type (4)(4) the exceptional roots are e1−e2,e2−e3,e3−e4e_1-e_2,e_2-e_3,e_3-e_4. This proves all the assertions. ◻

For the refinement along SS, the positive restriction is D3=−KSD_3=-K_S for 0≤u≤10\le u\le1, and D4−uD_{4-u} for 1≤u≤21\le u\le2. The fixed part is (u−1)R|S(u-1)R|_S in the second interval. For a function gg on [2,3][2,3], write its integrated value, without introducing an additional invariant, as 322(g(3)+∫23g(a)da).\frac3{22}\left(g(3)+\int_2^3g(a)\,da\right).

Lemma 104.2. Let FF be a smooth fibre different from 2ℓ2\ell, and let p∈Fp\in F. The integrated curve moment of the moving restriction is 109/176109/176. Its integrated point moment is 37/4437/44 if p∉Ep\notin E, is 79/8879/88 if p∈Ep\in E and SS has type 2A12A_1, and is 21/2221/22 if p∈Ep\in E and SS has type A3A_3.

Proof. The Zariski decomposition of Da−vFD_a-vF is vPN0≤v≤1Da−vF01≤v≤a/2(a−2v)h(v−1)(e1+e2+e3+e4).\begin{array}{c|c|c} v&P&N\\ \hline 0\le v\le1&D_a-vF&0\\ 1\le v\le a/2&(a-2v)h&(v-1)(e_1+e_2+e_3+e_4). \end{array} The first positive part equals (a−2)h+(1−v)F(a-2)h+(1-v)F, so it is nef. In the second interval PP is nef, NN is exceptional for the morphism to the plane, and P⋅N=0P\cdot N=0. The pseudo-effective threshold is a/2a/2. Thus the volume and the degree of the moving restriction to FF are vP2P⋅F0≤v≤1a2−4−4(a−2)v2(a−2)1≤v≤a/2(a−2v)22(a−2v).\begin{array}{c|c|c} v&P^2&P\cdot F\\ \hline 0\le v\le1&a^2-4-4(a-2)v&2(a-2)\\ 1\le v\le a/2&(a-2v)^2&2(a-2v). \end{array} Their relevant integrals are ∫0a/2P2dv=a(a−2)+(a−2)36,∫0a/2(P⋅F)2dv=4(a−2)2+23(a−2)3.\int_0^{a/2}P^2\,dv=a(a-2)+\frac{(a-2)^3}{6},\qquad \int_0^{a/2}(P\cdot F)^2\,dv =4(a-2)^2+\frac23(a-2)^3. The integrated values are 109/176109/176 and 37/4437/44.

The restriction of e1+⋯+e4e_1+\cdots+e_4 to FF has coefficient r=2r=2 at each of its two points in type 2A12A_1, and coefficient r=4r=4 at its single point in type A3A_3. Indeed, in the latter case e1+⋯+e4=(e1−e2)+2(e2−e3)+3(e3−e4)+4e4,e_1+\cdots+e_4=(e_1-e_2)+2(e_2-e_3)+3(e_3-e_4)+4e_4, and FF meets only the last curve. The additional point moment is obtained by integrating 2∫1a/2(P⋅F)r(v−1)dv=r6(a−2)3.2\int_1^{a/2}(P\cdot F)r(v-1)\,dv=\frac r6(a-2)^3. Its integrated value is 5r/1765r/176. This gives the asserted numbers. ◻

Lemma 104.3. Suppose that SS has type 2A12A_1, and let p∈L1p\in L_1. The integrated curve moment of L1L_1 is 73/8873/88. The integrated point moment is 59/8859/88 away from L2∪EL_2\cup E, is 73/8873/88 at L1∩L2L_1\cap L_2, and is 79/8879/88 at L1∩EL_1\cap E. The same statements hold with the two components interchanged.

Proof. The Zariski decomposition of Da−vL1D_a-vL_1 is vPN0≤v≤a−2Da−vL10a−2≤v≤1Da−vL1−(v−a+2)L2(v−a+2)L21≤v≤a−1(a−v−1)(2h−e3−e4)(v−a+2)L2+(v−1)(e1+e2).\begin{array}{c|c|c} v&P&N\\ \hline 0\le v\le a-2&D_a-vL_1&0\\ a-2\le v\le1&D_a-vL_1-(v-a+2)L_2&(v-a+2)L_2\\ 1\le v\le a-1&(a-v-1)(2h-e_3-e_4)& (v-a+2)L_2+(v-1)(e_1+e_2). \end{array} The classes hh, FF and 2h−e3−e42h-e_3-e_4 are nef. At the first wall the positive part is (3−a)F+(a−2)(2h−e3−e4)(3-a)F+(a-2)(2h-e_3-e_4), and at the second wall it is (a−2)(2h−e3−e4)(a-2)(2h-e_3-e_4). This proves nefness throughout the first two intervals by convexity. The negative supports are negative definite and orthogonal to PP. The last displayed positive part is nef, and the pseudo-effective threshold is a−1a-1.

In these three intervals the volumes are, respectively, (a−v)2−2(1−v)2−2,(a−v)2−2(1−v)2−2+(v−a+2)2,2(a−v−1)2,(a-v)^2-2(1-v)^2-2,\qquad (a-v)^2-2(1-v)^2-2+(v-a+2)^2,\qquad 2(a-v-1)^2, while the degrees on L1L_1 are a−2+va-2+v, 2a−42a-4 and 2(a−v−1)2(a-v-1). Direct integration gives ∫P2dv=(a−2)(a2+2a−2)3,∫(P⋅L1)2dv=(14−a)(a−2)23.\int P^2\,dv=\frac{(a-2)(a^2+2a-2)}3,\qquad \int(P\cdot L_1)^2\,dv=\frac{(14-a)(a-2)^2}3. The extra fixed-part point integral at L1∩L2L_1\cap L_2 is 2(a−2)(a2−7a+13)3,\frac{2(a-2)(a^2-7a+13)}3, and that at L1∩EL_1\cap E is 4(a−2)3/34(a-2)^3/3. For the latter coefficient, use e1+e2=(e1−e2)+2e2e_1+e_2=(e_1-e_2)+2e_2. Applying the preceding integration in aa gives 73/8873/88, 59/8859/88, 7/447/44 and 5/225/22, respectively. Adding the appropriate fixed-part term gives the claim. ◻

Proposition 104.4. If SS has type 2A12A_1 or A3A_3, then δp(S,W•,•S)>1\delta_p(S,W^S_{\bullet,\bullet})>1 at every point p∈S\ℓp\in S\setminus\ell.

Proof. All such points are smooth. Apply the surface flag inequality to the fibre through pp, using its component if the fibre is reducible. The preceding lemmas bound the moving contribution, divided by the log discrepancy, by the larger of the integrated curve and point moments. These bounds also apply to a divisorial valuation whose centre is the flag curve itself.

Here the integrations precede the maximum. To see this directly, work at a sufficiently divisible finite level and choose, in each restricted section space, a basis simultaneously adapted to the given valuation and to the flag curve CC. Remove the prescribed fixed divisor and the powers of CC from its elements. The resulting normalized basis divisor has the form cmC+Bmc_mC+B_m, where CC is not a component of BmB_m. The calculations above bound cmc_m by the integrated curve moment plus a term tending to zero, and bound the coefficient of Bm|CB_m|_C at pp by the integrated point moment plus a term tending to zero. Inversion of adjunction gives ordT(cmC+Bm)≤cmordT(C)+bm(AS(T)−ordT(C)),\operatorname{ord}_T(c_mC+B_m) \le c_m\operatorname{ord}_T(C) +b_m\bigl(A_S(T)-\operatorname{ord}_T(C)\bigr), where bmb_m is the latter bound. Passing to the limit gives the maximum used above. This argument uses the bases of the individual spaces; it does not require the moving parts alone to form a graded algebra.

It remains to include the fixed part (u−1)R|S(u-1)R|_S. The curve R|SR|_S is smooth and avoids the singularities of SS, so ordT(R|S)≤AS(T)\operatorname{ord}_T(R|_S)\le A_S(T) for every divisor TT over SS. Its contribution is therefore at most 322∫12(u−1)(2−u)(6−u)duAS(T)=988AS(T).\frac3{22}\int_1^2(u-1)(2-u)(6-u)\,du\, A_S(T) =\frac9{88}A_S(T). This contribution is zero if p∉Rp\notin R. Moreover, R∩ER\cap E is empty. Thus a smooth conic flag gives at most 83/8883/88 at points in RR, at most 79/8879/88 at points in EE in type 2A12A_1, and at most 21/2221/22 at points in EE in type A3A_3. At all other points it gives at most 37/4437/44. A component of a reducible fibre gives at most 82/8882/88 on RR, at most 79/8879/88 on EE, and at most 73/8873/88 elsewhere. Every displayed number is strictly smaller than one. ◻

Remark 104.5. The use of the smoothness of R|SR|_S in the last proof is useful when R|SR|_S is tangent to the chosen conic. Restricting the fixed divisor to that conic would count the tangency twice. The inequality ordT(R|S)≤AS(T)\operatorname{ord}_T(R|_S)\le A_S(T) applies before this restriction and avoids this unnecessary loss.

Proposition 104.6. If a prime divisor FF over XX satisfies βX(F)≤0\beta_X(F)\le0, its centre is contained in the support of a double fibre of η\eta.

Proof. Let Z=cX(F)Z=c_X(F) and choose a general point p∈Zp\in Z. Lemma 103.4 excludes surface centres and smooth quintic fibres. Since the singular quintic fibres are finite in number, ZZ lies in one of them, say SS. The estimates just proved exclude the complement of its double conic if SS has type 2A12A_1 or A3A_3.

It remains to consider a fibre with one A1A_1 or A2A_2 point oo. By Lemma 103.4, ZZ is contained in the conic fibre CoC_o through oo. This fibre is a pair of distinct lines meeting at oo. Let T∈|B|T\in|B| be the fibre containing it. Its image in ℙ3\mathbb P^3 is smooth: a rank-three quadric has only double lines or pairs of generator lines as singular plane sections, and in the latter case their intersection is its vertex, which cannot lie on the smooth complete intersection CC. Here π(o)∈C\pi(o)\in C. The line Λ\Lambda meets the two components at distinct smooth points, since it is disjoint from CC and their intersection is π(o)\pi(o). Thus TT is a smooth sextic del Pezzo surface.

The third estimate of Lemma 103.4 confines ZZ to the finitely many intersections of the smooth elliptic curve E|TE|_T with the six (−1)(-1)-curves. Consequently ZZ is a point. The strict Abban–Zhuang inequality along TT, whose refined threshold is at least one, now gives βX(F)≥ordF(T)(1−109176)>0,\beta_X(F)\ge\operatorname{ord}_F(T) \left(1-\frac{109}{176}\right)>0, a contradiction. This proves the reduction. ◻