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Section 110

Fibre refinements and the remaining centres

Write A=π*𝒪V(1,0)A=\pi^*\mathcal O_V(1,0), B=π*𝒪V(0,1)B=\pi^*\mathcal O_V(0,1), H=A+BH=A+B, F=H−EF=H-E and L=−KX=H+FL=-K_X=H+F. A fibre is denoted by SS, and CS=E|SC_S=E|_S. Thus CSC_S is the original smooth elliptic curve CC, viewed as an anticanonical curve in the smooth locus of SS.

Lemma 110.1. One has L3=24,SX(F)=1116,SX(E)=38.L^3=24,\qquad S_X(F)=\frac{11}{16},\qquad S_X(E)=\frac38. For every divisorial valuation vv of a fibre SS, the exact refinement satisfies S(WS;v)=1516SS(v)+116v(CS).S(W^S;v)=\frac{15}{16}S_S(v)+\frac1{16}v(C_S).

Proof. The identities H3=H2F=6H^3=H^2F=6 and F2=0F^2=0 give L3=24L^3=24. The positive and fixed parts of L−uFL-uF are (P(u),N(u))={(H+(1−u)F,0),0≤u≤1,((2−u)H,(u−1)E),1≤u≤2.(P(u),N(u))= \begin{cases} (H+(1-u)F,0),&0\le u\le1,\\ ((2-u)H,(u-1)E),&1\le u\le2. \end{cases} Indeed, HH and FF are nef. For u>1u>1, the fibres of E→CE\to C force the fixed multiplicity u−1u-1. Subtracting this multiple of EE leaves the nef divisor (2−u)H(2-u)H. The intersection with HFHF shows that u>2u>2 is not pseudoeffective. Therefore SX(F)=124(∫01(24−18u)du+∫126(2−u)3du)=1116.S_X(F)=\frac1{24}\left(\int_0^1(24-18u)\,du+ \int_1^2 6(2-u)^3\,du\right)=\frac{11}{16}. Similarly L−uE=(1−u)H+(1+u)FL-uE=(1-u)H+(1+u)F is nef for 0≤u≤10\le u\le1, and its intersection with HFHF is negative for u>1u>1. Consequently SX(E)=124∫01(24−36u+12u3)du=38.S_X(E)=\frac1{24}\int_0^1(24-36u+12u^3)\,du=\frac38. The restrictions of the positive parts to SS are −KS-K_S for u≤1u\le1 and (2−u)(−KS)(2-u)(-K_S) for u≥1u\ge1. The fixed part restricts to (u−1)CS(u-1)C_S in the latter interval. The complete moving systems occur in the restriction calculation: for 0<u<10<u<1 this follows from vanishing, and for 1<u<21<u<2 it follows after removing the fixed part from restriction of multiples of HH to its member SS on VV. For this last assertion one may use the restriction sequence and Kodaira vanishing on the smooth index-two Fano threefold VV. The endpoints do not affect the integrals. The coefficients are 3⋅624(1+∫12(2−u)3du)=1516,3⋅624∫12(2−u)2(u−1)du=116.\frac{3\cdot6}{24}\left(1+\int_1^2(2-u)^3\,du\right)=\frac{15}{16}, \qquad \frac{3\cdot6}{24}\int_1^2(2-u)^2(u-1)\,du=\frac1{16}. This proves the asserted equality for the actual restricted series. All decompositions in this lemma take place on XX itself. ◻

Lemma 110.2. If δp(S)≥1\delta_p(S)\ge1, every prime divisor QQ over XX whose centre contains pp and is contained in SS satisfies βX(Q)≥516ordQ(S)>0.\beta_X(Q)\ge\frac5{16}\operatorname{ord}_Q(S)>0. If p∉Ep\notin E, one has the stronger local estimate δp(X)≥16/15\delta_p(X)\ge16/15.

Proof. The pair (S,CS)(S,C_S) is log canonical, so v(CS)≤AS(v)v(C_S)\le A_S(v). Lemma 110.1 gives S(WS;v)≤AS(v)S(W^S;v)\le A_S(v). The basis-divisor proof of Abban–Zhuang adjunction, retaining the coefficient of SS, gives βX(Q)≥(1−SX(S))ordQ(S)\beta_X(Q)\ge(1-S_X(S))\operatorname{ord}_Q(S). For clarity, choose a basis simultaneously adapted to QQ and SS, write its basis divisor as amS+D′ma_mS+D'_m, and restrict D′mD'_m to SS. The refined threshold bound gives numbers cm→1c_m\to1 for which (S,cmD′m|S)(S,c_mD'_m|_S) is log canonical near pp. Inversion of adjunction then gives AX(Q)≥cmSm(Q)+(1−cmam)ordQ(S).A_X(Q)\ge c_m S_m(Q)+(1-c_ma_m)\operatorname{ord}_Q(S). Pass to the limit. If p∉Ep\notin E, all relevant valuations of SS have zero order on CSC_S, and the refined threshold is at least 16/1516/15. The other Abban–Zhuang term is 16/1116/11. ◻

Lemma 110.3. Let SS be one of the sextic del Pezzo fibres occurring here. If SS is smooth, then δp(S)≥1\delta_p(S)\ge1 for every p∈Sp\in S, and δp(S)≥6/5\delta_p(S)\ge6/5 off the six lines. If SS has an A1A_1 singularity, then δp(S)≥1\delta_p(S)\ge1 off the two lines through the singular point. If SS has an A2A_2 singularity, then δp(S)≥1\delta_p(S)\ge1 off its two lines.

Proof. We give the surface calculations to fix the values needed here. On the minimal resolution, write the anticanonical class as DD. At a smooth point off all lines, blow up the point, with exceptional curve GG. The pencil classes h−eih-e_i in the plane model give the following Zariski decomposition. For 0≤v≤20\le v\le2 its positive part is D−vGD-vG. For 2≤v≤32\le v\le3 its negative part is (v−2)Z(v-2)Z, where ZZ has one of the following forms: Z=B1+B2+B3,Z=2B1+C1+B2,Z=3B1+2C1+C2.Z=B_1+B_2+B_3,\qquad Z=2B_1+C_1+B_2,\qquad Z=3B_1+2C_1+C_2. Here the BiB_i are the proper transforms of the distinct moving pencil members through the point and have square −1-1; the CiC_i are the intervening (−2)(-2)-curves. The three cases correspond to three distinct plane points, one infinitely near pair, and a chain of three infinitely near points. The curves BiB_i meet GG in distinct points, and the CiC_i do not meet GG. In each case the proposed positive part is nef: its intersection with every negative curve is nonnegative, and the displayed divisor has zero intersection with the support of the negative part. These negative curves generate the effective cone of the resulting weak quintic del Pezzo surface. Equivalently, the same verification uses the plane classes h−eih-e_i and their residual exceptional chains. The squares and intersections are P(v)2={6−v2,0≤v≤2,2(3−v)2,2≤v≤3,P(v)G={v,0≤v≤2,2(3−v),2≤v≤3.P(v)^2=\begin{cases}6-v^2,&0\le v\le2,\\ 2(3-v)^2,&2\le v\le3, \end{cases} \qquad P(v)G=\begin{cases}v,&0\le v\le2,\\ 2(3-v),&2\le v\le3. \end{cases} They give SS(G)=5/3S_S(G)=5/3. At any point q∈Gq\in G, let kk be the coefficient of the component of ZZ meeting qq; put k=0k=0 when there is no such component. Then k≤3k\le3 and S(WSG;q)≤16(∫02v2dv+∫234(3−v)2dv)+k3∫232(3−v)(v−2)dv=23+k9≤1.S(W_S^G;q) \le\frac16\left(\int_0^2v^2\,dv+ \int_2^3 4(3-v)^2\,dv\right) +\frac{k}{3}\int_2^3 2(3-v)(v-2)\,dv =\frac23+\frac{k}{9}\le1. On a smooth sextic surface k≤1k\le1, so this bound is 7/97/9 and Abban–Zhuang gives δp(S)≥6/5\delta_p(S)\ge6/5.

On a smooth sextic surface, a line TT has adjacent lines U,VU,V. For 0≤v≤10\le v\le1, D−vTD-vT is nef. For 1≤v≤21\le v\le2, the negative part is (v−1)(U+V)(v-1)(U+V). Thus P(v)2={6−2v−v2,0≤v≤1,(2−v)(4−v),1≤v≤2,P(v)T={1+v,0≤v≤1,3−v,1≤v≤2.P(v)^2=\begin{cases}6-2v-v^2,&0\le v\le1,\\ (2-v)(4-v),&1\le v\le2, \end{cases} \qquad P(v)T=\begin{cases}1+v,&0\le v\le1,\\ 3-v,&1\le v\le2. \end{cases} Consequently SS(T)=1S_S(T)=1, and the secondary invariant is 7/97/9 away from T∩(U∪V)T\cap(U\cup V) and 11 at these two intersections. This proves the assertion on all smooth fibres.

For an A1A_1 fibre, let TT be one of the two lines not through the node. On the resolution, TT meets a (−1)(-1)-curve UU meeting the exceptional (−2)(-2)-curve RR. For 1≤v≤21\le v\le2 the negative part is (v−1)(2U+R)(v-1)(2U+R); for v≤1v\le1 it is zero. The same displayed formula for P(v)2P(v)^2 holds, because (2U+R)2=−2(2U+R)^2=-2. Thus SS(T)=1S_S(T)=1, and the secondary invariant is 7/97/9 away from T∩UT\cap U. The latter point lies on a line through the node and is excluded from the assertion. This finishes the proof. ◻

Remark 110.4. The restriction to the two lines through the singularity is necessary for this particular fibre argument. On an A1A_1 fibre, either such line TT has P(v)2={6−2v−v2/2,0≤v≤1,7−4v+v2/2,1≤v≤2,(3−v)2,2≤v≤3,SS(T)=119.P(v)^2=\begin{cases} 6-2v-v^2/2,&0\le v\le1,\\ 7-4v+v^2/2,&1\le v\le2,\\ (3-v)^2,&2\le v\le3, \end{cases} \qquad S_S(T)=\frac{11}{9}. On an A2A_2 fibre either line has P(v)2={6−2v−v2/3,0≤v≤3/2,(3−v)2,3/2≤v≤3,SS(T)=54.P(v)^2=\begin{cases} 6-2v-v^2/3,&0\le v\le3/2,\\ (3-v)^2,&3/2\le v\le3, \end{cases} \qquad S_S(T)=\frac54. These are obtained by solving the intersection equations against the (−2)(-2)-chain and then adjoining the adjacent (−1)(-1)-curves when their intersection becomes negative. They agree with the calculations in [12, Lemmas 4.5–4.6]. In particular the first refined moments are 55/4855/48 and 75/6475/64, respectively. They exceed one, so the fibre refinement alone does not prove the required result there.

Lemma 110.5. Every prime divisor over XX whose centre is a curve in EE dominating the pencil base has positive beta invariant.

Proof. First consider a point p∈CSp\in C_S on a smooth fibre. If pp is off the six lines, Lemmas 110.1 and 110.3 give δp(X)≥min{1611,16(6/5)15+6/5}=3227>1.\delta_p(X)\ge\min\left\{\frac{16}{11}, \frac{16(6/5)}{15+6/5}\right\}=\frac{32}{27}>1. If pp lies on just one line TT, refine once more by TT. The first invariant is 15/1615/16. Since CST=1C_ST=1, the intersection at pp is transverse; the secondary invariant is at most 1516⋅79+116=1924.\frac{15}{16}\cdot\frac79+\frac1{16}=\frac{19}{24}. Hence δp(X)≥16/15\delta_p(X)\ge16/15.

Only the corners of the hexagon of lines remain. There are finitely many pairs (S,p)(S,p) with SS smooth and p∈CSp\in C_S such a corner. To see this, view VV as the incidence variety of points and lines in ℙ2\mathbb P^2. The contact plane at (x,ℓ)(x,\ell) is the span of the tangent directions of the two projection fibres. At a corner, these are the two line directions in SS, so TpCT_pC lies in the contact plane. The induced morphism TC→𝒪V(1,1)|CT_C\longrightarrow\mathcal O_V(1,1)|_C is not identically zero. Otherwise the second projection would send every point of the smooth plane cubic given by the first projection to its tangent line. This tangent-line map has degree six with respect to 𝒪(ℙ2)*(1)\mathcal O_{(\mathbb P^2)^*}(1): the three quadratic partial derivatives of its smooth cubic equation have no common zero on the cubic. But the second projection of CC has degree three, a contradiction. The displayed morphism therefore has only finitely many zeros. For each zero there is at most one smooth pencil member whose tangent plane is the contact plane, since the two pencil sections have independent differentials along the smooth complete intersection CC.

A curve in EE dominating the pencil base meets a general fibre at points avoiding this finite set. At any such point the preceding strict local bound excludes the curve as a nonpositive-beta centre. ◻

Proposition 110.6. If QQ is a prime divisor over XX with βX(Q)≤0\beta_X(Q)\le0, its centre is contained in one of the two lines through the singular point of an A1A_1 or A2A_2 fibre.

Proof. A centre meeting a smooth fibre outside EE is excluded by Lemma 110.2. A horizontal curve in EE is excluded by Lemma 110.5. The divisor EE itself has SX(E)=3/8<1S_X(E)=3/8<1. These observations exclude all horizontal centres. A divisorial centre in a fibre is the fibre itself and has SX(F)=11/16<1S_X(F)=11/16<1. Any remaining centre lies in a fibre and has dimension at most one. At every point outside the stated lines, Lemma 110.3 and the strict inequality in Lemma 110.2 exclude it. The singular point of either singular fibre lies on the stated lines. ◻