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Section 72

Reduced singular conic fibres: exact surface estimates

The following computations record an obstruction to extending the preceding smooth-fibre flag argument without an additional threefold estimate. They do not establish instability. Write S=Blp1,p2,p3,p4ℙ2,A=l−e1−e2,D=l−e3−e4,Z=A+D,C=l.S=\operatorname{Bl}_{p_1,p_2,p_3,p_4}\mathbb P^2,\quad A=l-e_1-e_2,\quad D=l-e_3-e_4,\quad Z=A+D,\quad C=l. Assume that SS and CC are smooth and that CC avoids the four exceptional curves. Thus AA and DD meet transversally at one point p0p_0, while CC meets each of A,DA,D once, possibly at p0p_0. Put (b,k)={(2−u,1)0≤u≤1,(2−u,2−u)1≤u≤2.(b,k)=\begin{cases}(2-u,1)&0\leq u\leq1,\\ (2-u,2-u)&1\leq u\leq2. \end{cases} Then the positive part restricted from the threefold is Mu=(2b+k)l−b∑eiM_u=(2b+k)l-b\sum e_i. In both intervals k≤b≤2kk\leq b\leq2k.

Lemma 72.1. The pseudoeffective threshold of AA with respect to MuM_u is b+kb+k. The negative part of Mu−vAM_u-vA is vNu,v[0,k]0[k,b](v−k)D[b,b+k](v−k)D+(v−b)(e1+e2).\begin{array}{c|c} v&N_{u,v}\\ \hline {[0,k]}&0\\ {[k,b]}&(v-k)D\\ {[b,b+k]}&(v-k)D+(v-b)(e_1+e_2). \end{array} The corresponding positive parts have volumes 4bk+k2−2kv−v2,2k(2b+k−2v),2(b+k−v)2,4bk+k^2-2kv-v^2,\qquad 2k(2b+k-2v),\qquad 2(b+k-v)^2, and their intersections with AA are respectively k+vk+v, 2k2k, and 2(b+k−v)2(b+k-v). Consequently, S(WS;A)=109104.S(W^S;A)=\frac{109}{104}. For p∈Ap\in A, the point estimate obtained from this flag is S(WS,A;p)=79104+1552𝟏p=p0+552𝟏p∈e1∪e2+5104𝟏p∈C.S(W^{S,A};p)=\frac{79}{104} +\frac{15}{52}\boldsymbol1_{p=p_0} +\frac5{52}\boldsymbol1_{p\in e_1\cup e_2} +\frac5{104}\boldsymbol1_{p\in C}. In particular, at the node it is 109/104109/104 if p0∉Cp_0\notin C, and 57/5257/52 if p0∈Cp_0\in C.

Proof. The curves D,e1,e2D,e_1,e_2 are mutually disjoint (−1)(-1)-curves. Subtracting the displayed coefficients makes the positive part orthogonal to its negative part. Intersecting with the ten (−1)(-1)-curves proves nefness. In the last chamber the positive part is (b+k−v)(2l−e3−e4)(b+k-v)(2l-e_3-e_4). The nef divisor 2l−e3−e42l-e_3-e_4 has intersection 2(b+k−v)2(b+k-v) with Mu−vAM_u-vA, so v>b+kv>b+k is not pseudoeffective. Squaring and intersecting with AA give all the displayed expressions.

For the curve moment integrate the three volume expressions with factor 3/263/26. For the point moment integrate (Pu,v⋅A)2(P_{u,v}\cdot A)^2 with factor 3/263/26. This gives 79/10479/104. The negative component DD contributes 626∫02∫kb+k(Pu,v⋅A)(v−k)dvdu=1552.\frac6{26}\int_0^2\int_k^{b+k} (P_{u,v}\cdot A)(v-k)\,dv\,du=\frac{15}{52}. Each of e1,e2e_1,e_2 contributes 626∫02∫bb+k2(b+k−v)(v−b)dvdu=552.\frac6{26}\int_0^2\int_b^{b+k} 2(b+k-v)(v-b)\,dv\,du=\frac5{52}. Finally the fixed part (u−1)+C(u-1)_+C contributes 5/1045/104 at its intersection with AA. All intersections are transverse. The node, the two exceptional endpoints, and any other point of C∩AC\cap A are distinct; C∩AC\cap A can coincide only with the node. ◻

Lemma 72.2. Let σ:T→S\sigma:T\to S blow up p0p_0, with exceptional curve JJ. Then S(WS;J)=10952+5104𝟏p0∈C.S(W^S;J)=\frac{109}{52}+\frac5{104}\boldsymbol1_{p_0\in C}. The point moments on JJ are bounded by 47104+3152𝟏q∈A′∪D′+5104𝟏p0∈C,q∈C′.\frac{47}{104} +\frac{31}{52}\boldsymbol1_{q\in A'\cup D'} +\frac5{104}\boldsymbol1_{p_0\in C,\ q\in C'}. Here the three directions A′,D′,C′A',D',C' are pairwise distinct whenever C′C' meets JJ. Thus the maximum is 109/104109/104, attained at either branch direction.

Proof. The strict transforms A′,D′A',D' are disjoint (−2)(-2)-curves. For 0≤v≤k0\leq v\leq k, the divisor σ*Mu−vJ\sigma^*M_u-vJ is nef. For k≤v≤2b+kk\leq v\leq2b+k, its negative part is (v−k)(A′+D′)/2(v-k)(A'+D')/2. The positive part has square {4bk+k2−v20≤v≤k,2k(2b+k−v)k≤v≤2b+k,\begin{cases} 4bk+k^2-v^2&0\leq v\leq k,\\ 2k(2b+k-v)&k\leq v\leq2b+k, \end{cases} and intersection with JJ equal to vv and kk, respectively. For nefness, one may write the positive part in the second interval as (b−(v−k)/2)σ*Z+k(σ*l−J),(b-(v-k)/2)\sigma^*Z+k(\sigma^*l-J), a nonnegative combination of the two nef pencils σ*Z\sigma^*Z and σ*l−J\sigma^*l-J. At the threshold it equals k(σ*l−J)k(\sigma^*l-J). The nef divisor σ*l−J\sigma^*l-J has intersection 2b+k−v2b+k-v with σ*Mu−vJ\sigma^*M_u-vJ, proving the threshold.

Integrating the two squares gives 109/52109/52. The fixed curve CC adds 326∫125(2−u)2(u−1)du=5104\frac3{26}\int_1^2 5(2-u)^2(u-1)\,du=\frac5{104} exactly when it passes through p0p_0. For the second refinement, integrating (Pu,v⋅J)2(P_{u,v}\cdot J)^2 gives 47/10447/104. The coefficient (v−k)/2(v-k)/2 of either branch contributes 31/5231/52 at its direction; the strict transform of the fixed curve contributes 5/1045/104 at its direction. These directions are distinct because C,A,DC,A,D are three distinct lines through the same point in the plane model. ◻

Remark 72.3. Neither lemma is a destabilizing calculation for the threefold. The first curve moment exceeds its surface log discrepancy 11, while the node moment exceeds its surface log discrepancy 22. This says precisely that these unmodified surface Abban–Zhuang estimates fail to prove the desired threefold assertion. A successful proof must exploit more information, for example the positive first-stage margin 41v(S)/10441v(S)/104 and a comparison with the conic-bundle coordinates, or a different extraction.

Lemma 72.4. Keep the preceding assumptions, and let vv be a divisorial valuation centred at p∈Ap\in A on XX. If p≠p0p\neq p_0 or p0∉Cp_0\notin C, then AX(v)−SX(v)≥46v(S)−5AX(v)104.A_X(v)-S_X(v)\geq\frac{46v(S)-5A_X(v)}{104}. If p=p0∈Cp=p_0\in C, then AX(v)−SX(v)≥51v(S)−10AX(v)104.A_X(v)-S_X(v)\geq\frac{51v(S)-10A_X(v)}{104}. In particular these inequalities are strict whenever AX(v)/v(S)<46/5A_X(v)/v(S)<46/5 in the first case, or AX(v)/v(S)<51/10A_X(v)/v(S)<51/10 in the second case.

Proof. Choose a basis adapted simultaneously to vv and the single lexicographic flag X⊃S⊃A⊃{p}X\supset S\supset A\supset\{p\}. Write its normalized basis divisor as Dm=amS+D′mD_m=a_mS+D'_m, and write D′m|S=bmA+RmD'_m|_S=b_mA+R_m, where RmR_m does not contain AA. Then am→63/104a_m\to63/104, bm→109/104b_m\to109/104, and (Rm⋅A)p(R_m\cdot A)_p tends to the point moment in Lemma 72.1. Away from the node this moment is at most 89/10489/104. At the node it is 109/104109/104 off CC and 114/104114/104 on CC. Consequently, one can choose positive coefficients cmc_m with cmbm≤1c_mb_m\leq1 and cm(Rm⋅A)p≤1c_m(R_m\cdot A)_p\leq1, tending to c=104/109c=104/109 in the first case and c=104/114c=104/114 in the second case.

Both AA and SS are smooth at pp. Applying inversion of adjunction first to (S,A+cmRm)(S,A+c_mR_m) and then to (X,S+cmD′m)(X,S+c_mD'_m) gives AX(v)−cmv(Dm)≥(1−cmam)v(S).A_X(v)-c_m v(D_m)\geq(1-c_ma_m)v(S). All boundaries used here are effective. The basis is adapted to vv, so v(Dm)→SX(v)v(D_m)\to S_X(v). Passing to the limit and dividing by cc yields AX(v)−SX(v)≥(1/c−63/104)v(S)−(1/c−1)AX(v),A_X(v)-S_X(v)\geq(1/c-63/104)v(S)-(1/c-1)A_X(v), which is exactly the assertion. ◻