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Section 95

The exceptional surface at an index-four point

Let pp be the A3A_3 point of a fibre whose ramification index is four. We extract pp with weights (1,2,2)(1,2,2). Its exceptional pair is (G,Δ)=(ℙ2,Λ/2)(G,\Delta)=(\mathbb P^2,\Lambda/2), where Λ\Lambda is a line. Write W=WGW=W^G for the actual refined series. The different is essential: the two points where the initial fibre conic meets Λ\Lambda have log discrepancy 1/21/2 after adjunction to that conic.

Theorem 95.1. For the weight-(1,2,2)(1,2,2) extraction at an index-four point, δ(G,Λ/2;W)≥8077,δp(X)=400389>1.\delta(G,\Lambda/2;W)\ge\frac{80}{77},\qquad \delta_p(X)=\frac{400}{389}>1.

Lemma 95.2 (The conic flag and its complete quotients). Choose native coordinates x,z,wx,z,w of weights (1,2,2)(1,2,2), and put c=x2+z,t=zw−c2.c=x^2+z,\qquad t=zw-c^2. On the coarse exceptional plane use coordinates U=z,V=x2,W0=w−z−2x2.U=z,\qquad V=x^2,\qquad W_0=w-z-2x^2. Then the initial fibre is the smooth conic B=(UW0−V2=0),Λ=(V=0).B=(UW_0-V^2=0),\qquad \Lambda=(V=0). Parametrize BB by [U:V:W0]=[p2:pq:q2][U:V:W_0]=[p^2:pq:q^2], and write P=(p=0),Q=(q=0),R=(p+q=0).P=(p=0),\qquad Q=(q=0),\qquad R=(p+q=0). Thus Δ|B=(P+Q)/2\Delta|_B=(P+Q)/2.

Fix m≥1m\ge1. In the primary weight-jj piece Wm,jW_{m,j}, let kk be the order along BB. Put n=j−4kn=j-4k and ε≡n(mod2)\varepsilon\equiv n\pmod2, 0≤ε≤10\le\varepsilon\le1. Set qk={m,0≤k≤m,2m−k,m≤k≤2m,q_k=\begin{cases}m,&0\le k\le m,\\2m-k,&m\le k\le2m,\end{cases} and a=max(⌊n/2⌋−qk,0),b=max(⌊n/2⌋−m,0),c0=max(n−m,0),d=n−ε−a−b−c0.a=\max(\lfloor n/2\rfloor-q_k,0),\quad b=\max(\lfloor n/2\rfloor-m,0),\quad c_0=\max(n-m,0),\quad d=n-\varepsilon-a-b-c_0. For 0≤k≤2m0\le k\le2m and n≥0n\ge0, the nonzero quotient is precisely (35.7)ξεpaqb(p+q)c0H0(ℙ1,𝒪(d)),\xi^{\varepsilon}p^a q^b(p+q)^{c_0} H^0(\mathbb P^1,\mathcal O(d)), \tag{35.7} provided d≥0d\ge0. Here ξ2=pq\xi^2=pq: this notation records the fractional fixed divisor ε(P+Q)/2\varepsilon(P+Q)/2, using the index covers. It does not assert that pqpq has a square root in the function field of BB. Each such quotient has dimension d+1d+1; all other quotients are zero.

Proof. Use the homogeneous central model in Lemma 93.2, with centre y(ux4+vy4)=0y(ux^4+vy^4)=0. Its affine blow-up chart has equation t=zw−(x2+z)2t=zw-(x^2+z)^2. The change of coordinates in the statement gives t=UW0−V2t=UW_0-V^2. The primary weight spaces on this model are the actual associated graded spaces of the original point filtration, as proved in that lemma. The defining section tt has weight four. Consequently the filtration by its order preserves the weight decomposition, and taking weight spaces commutes with taking the successive tt-quotients. No interchange of two arbitrary filtrations is being assumed.

The fibre t=0t=0 is the plane blown up in a length-four cluster along a smooth conic and one further point of that conic. On its minimal resolution use h,e1,…,e5h,e_1,\ldots,e_5, where e1,…,e4e_1,\ldots,e_4 are the total transforms for the successive cluster points and e5e_5 is the other point. The middle exceptional curve is F=e2−e3F=e_2-e_3. The restriction and vanishing argument used for Lemma 92.1 applies to the central model as well: it is a canonical Fano threefold, and the same nef divisors occur. After removing the fixed conic, which is disjoint from FF, the kkth fibre quotient is the complete space of plane forms of degree dkd_k, with multiplicity qkq_k at all five cluster points, where dk={3m,k≤m,5m−2k,k≥m.d_k=\begin{cases}3m,&k\le m,\\5m-2k,&k\ge m.\end{cases} dk−qk=3m−kd_k-q_k=3m-k when k≥mk\ge m, whereas it is 2m2m when k≤mk\le m; also dk−2qk=md_k-2q_k=m in both intervals.

Here is a direct calculation of the FF-initial spaces. Use affine plane coordinates x,cx,c, with conic z=c−x2=0z=c-x^2=0, and place the separate point at [0:0:1][0:0:1] in coordinates [1:x:c][1:x:c]. The length-four cluster ideal is (z,x4)(z,x^4); its qkq_kth power is complete. A plane monomial xicbx^i c^b must satisfy i+b≤dki+b\le d_k and b≤dk−qkb\le d_k-q_k. The first condition bounds its degree, and the second is exactly its multiplicity condition at [0:0:1][0:0:1]. The cluster ideal is homogeneous for weights (1,2)(1,2) on (x,c)(x,c), so these conditions split into homogeneous pieces.

The valuation of FF has weights (1,2)(1,2) on (x,z)(x,z). A form contributing order nn after division by the cluster exceptional factor therefore has weight N=n+2qkN=n+2q_k. Put l=⌊N/2⌋l=\lfloor N/2\rfloor. Write such a form as xε(x2)lf(c/x2)x^\varepsilon (x^2)^l f(c/x^2). The bounds just given say that the exponents of ff lie between b−=max(0,N−dk),b+=min(l,dk−qk).b_-=\max(0,N-d_k),\qquad b_+=\min(l,d_k-q_k). Membership in (z,x4)qk(z,x^4)^{q_k} additionally says that f(h)f(h) is divisible by (h−1)M(h-1)^M, where M=max(0,2qk−l).M=\max(0,2q_k-l). Indeed a term xN−2izix^{N-2i}z^i belongs to this ideal precisely when N+2i≥4qkN+2i\ge4q_k.

Since hh and h−1h-1 have distinct zeros, the resulting polynomial space is exactly hb−(h−1)Mℂ[h]≤b+−b−−M.h^{b_-}(h-1)^M\mathbb C[h]_{\le b_+-b_--M}. On BB one has z=p2z=p^2, x2=pqx^2=pq, c=p(p+q)c=p(p+q). Dividing by the cluster factor zqk=p2qkz^{q_k}=p^{2q_k} gives ξεpl−2qk+Mql−b+(p+q)b−H0(ℙ1,𝒪(b+−b−−M)).\xi^\varepsilon p^{l-2q_k+M}q^{l-b_+}(p+q)^{b_-} H^0(\mathbb P^1,\mathcal O(b_+-b_--M)). Substituting dk−2qk=md_k-2q_k=m reduces its exponents to (35.7). This proves completeness and the dimension statement in every degree. ◻

Example 95.3. Take m=2m=2, k=0k=0, n=4n=4. Then a=b=0a=b=0, c0=2c_0=2, d=2d=2, so the quotient is (p+q)2H0(ℙ1,𝒪(2))(p+q)^2H^0(\mathbb P^1,\mathcal O(2)). The maximal sums of basis orders at P,Q,RP,Q,R are respectively 3,3,93,3,9: the first two are 0+1+20+1+2, while the last is 2+3+42+3+4. For n=3n=3 the quotient has the additional fixed divisor (P+Q)/2(P+Q)/2. This is why the parity term appears in the finite-level formulas, even though its contribution tends to zero after dividing by mNmmN_m.

Lemma 95.4 (The conic and point moments, computed separately). For refinement along BB one has S(W;B)=6980.S(W;B)=\frac{69}{80}. Writing WBW^B for the resulting series on BB, its point moments are (35.8)S(WB;P)=77160,S(WB;Q)=2764,S(WB;R)=910,S(WB;O)=2564(O∉{P,Q,R}).\begin{gathered} S(W^B;P)=\frac{77}{160},\qquad S(W^B;Q)=\frac{27}{64},\qquad S(W^B;R)=\frac9{10},\\ S(W^B;O)=\frac{25}{64}\quad(O\notin\{P,Q,R\}). \end{gathered} \tag{35.8} The average degree of the residual plane divisors after removing their BB-components is 113/160113/160.

Proof. Use the quotients (35.7). Their contributions to the order sums at B,P,Q,R,OB,P,Q,R,O are respectively k(d+1),(a+ε/2+d/2)(d+1),(b+ε/2+d/2)(d+1),(c0+d/2)(d+1),d(d+1)/2.k(d+1),\quad (a+\varepsilon/2+d/2)(d+1),\quad (b+\varepsilon/2+d/2)(d+1),\quad (c_0+d/2)(d+1),\quad d(d+1)/2. These are the maximal sums for complete binary spaces, with the fixed factors included. Sum them and divide by mNmmN_m.

We spell out the integrals. Put u=k/mu=k/m, v=n/mv=n/m and q(u)={1,0≤u≤1,2−u,1≤u≤2,q(u)=\begin{cases}1,&0\le u\le1,\\2-u,&1\le u\le2,\end{cases} A=(v/2−q(u))+,C=(v−1)+,B0=(v/2−1)+,D=v−A−B0−C,A=(v/2-q(u))_+,\quad C=(v-1)_+,\quad B_0=(v/2-1)_+,\quad D=v-A-B_0-C, where r+=max(r,0)r_+=\max(r,0). Integrate over D≥0D\ge0, v≥0v\ge0, 0≤u≤20\le u\le2. Floors and parity change the sums by O(m3)O(m^3). The following are the unnormalized integrals, with measure dvdudv\,du: (35.9)DuD(A+D/2)D(B0+D/2)D(C+D/2)DD2/2(4u+v)D0≤u≤12111/1211/1225/671≤u≤24/315/811/1647/96115/32221/24.\begin{array}{c|rrrrrrr} &D&uD&(A+D/2)D&(B_0+D/2)D&(C+D/2)D&D^2/2&(4u+v)D\\ \hline 0\le u\le1&2&1&11/12&11/12&2&5/6&7\\ 1\le u\le2&4/3&15/8&11/16&47/96&1&15/32&221/24. \end{array} \tag{35.9} For the first row, split the vv-interval at 1,2,31,2,3; the values of DD are v,1,3−vv,1,3-v. For the second row, use q=2−uq=2-u and the following five regions: qvD[0,1][0,min(1,2q)]v[1/2,1][1,2q]1[0,1/2][2q,1]v/2+q[0,1][max(1,2q),2]1+q−v/2[0,1][2,2+q]2+q−v.\begin{array}{c|c|c} q&v&D\\ \hline [0,1]&[0,\min(1,2q)]&v\\ {}[1/2,1]&[1,2q]&1\\ {}[0,1/2]&[2q,1]&v/2+q\\ {}[0,1]&[\max(1,2q),2]&1+q-v/2\\ {}[0,1]&[2,2+q]&2+q-v. \end{array} These regions give each entry by integrating a quadratic polynomial. For example the last column of (35.9) sums to 389/24389/24, while the first sums to 10/310/3. Multiplication by 3/103/10, the leading normalization of 1/(mNm)1/(mN_m), gives SX(G)=389/80S_X(G)=389/80 again. The second column gives 69/8069/80. Columns three through six give (35.8). Thus the computation also checks the normalization independently of the threefold character sum.

On the coarse plane a primary-degree-jj section has divisor degree j/2j/2. Consequently, after removing the conic components, the average degree is 12SX(G)−2S(W;B)=389160−13880=113160.\frac12 S_X(G)-2S(W;B)=\frac{389}{160}-\frac{138}{80} =\frac{113}{160}. ◻

Lemma 95.5 (Controlling points off the conic). Let Dm=emB+RmD_m=e_mB+R_m be a basis divisor of WW compatible with order along BB. Thus Rm≥0R_m\ge0 and B⊄Supp(Rm)B\not\subset\operatorname{Supp}(R_m). Then em→69/80,degRm→113/160,coeffΛ(Rm)≤27/64+o(1),e_m\longrightarrow69/80,\qquad \deg R_m\longrightarrow113/160, \qquad\operatorname{coeff}_{\Lambda}(R_m)\le27/64+o(1), where the error bound is independent of the chosen compatible basis. For every τ<80/77\tau<80/77, the pair (G,Λ/2+τDm)(G,\Lambda/2+\tau D_m) is log canonical off BB for all large mm.

Proof. The first two assertions follow from the preceding lemma. Restriction of the residual sections to BB gives bases of the quotients (35.7). Since Λ\Lambda and BB meet transversely at QQ, coeffΛ(Rm)≤multQ(Rm|B)≤Sm(WB;Q).\operatorname{coeff}_{\Lambda}(R_m) \le\operatorname{mult}_{Q}(R_m|_B) \le S_m(W^B;Q). This proves the uniform third assertion; it does not require a basis compatible with a third filtration.

Write Rm=bmΛ+R′mR_m=b_m\Lambda+R'_m, where R′mR'_m has no Λ\Lambda-component. For all large mm, 12+τbm<1,τdegRm<1.\frac12+\tau b_m<1,\qquad \tau\deg R_m<1. Off B∪ΛB\cup\Lambda the boundary is τR′m\tau R'_m. Its degree is less than one, so it is log canonical: at any point its multiplicity is at most its degree, and the standard multiplicity bound gives lctq(G;R′m)≥1/multq(R′m)\operatorname{lct}_q(G;R'_m)\ge1/\operatorname{mult}_q(R'_m). Along Λ\B\Lambda\setminus B, the divisor τR′m|Λ\tau R'_m|_\Lambda has degree less than one and hence all coefficients less than one. Inversion of adjunction gives log canonicity of (G,Λ+τR′m)(G,\Lambda+\tau R'_m) there. Decreasing the Λ\Lambda-coefficient to 1/2+τbm1/2+\tau b_m proves the assertion. ◻

Proof of Theorem 95.1. Fix τ<80/77\tau<80/77. For every basis divisor Dm=emB+RmD_m=e_mB+R_m compatible with BB, the coefficients of (Λ/2)|B+τRm|B(\Lambda/2)|_B+\tau R_m|_B are at most one for all large mm, by (35.8). The bounds at P,Q,RP,Q,R and the other points are uniform over the choice of basis. The restrictive inequality is the one at PP: 12+τ77160<1.\frac12+\tau\frac{77}{160}<1. Also τem<1\tau e_m<1. Inversion of adjunction along the smooth conic therefore gives log canonicity of (G,Λ/2+τDm)(G,\Lambda/2+\tau D_m) near BB. Lemma 95.5 proves it on the complement.

For any divisorial valuation over GG, choose in each primary piece a basis compatible with its filtration and the BB-filtration. The resulting order is the maximal basis order for that valuation. The preceding global log-canonicity statement, followed by m→∞m\to\infty and τ→80/77\tau\to80/77, proves δ(G,Λ/2;W)≥80/77\delta(G,\Lambda/2;W)\ge80/77. Abban–Zhuang adjunction for the point extraction gives δp(X)≥min{5389/80,8077}=400389.\delta_p(X)\ge\min\left\{\frac{5}{389/80},\frac{80}{77}\right\} =\frac{400}{389}. The exceptional divisor GG itself gives the opposite inequality, so equality holds.

No Zariski decomposition on the weight-(1,2,2)(1,2,2) blow-up of XX has been used. The commuting homogeneous fibre filtration and the plane ideal (c−x2,x4)qk(c-x^2,x^4)^{q_k} give the exact section spaces. Their complete binary quotients control the conic; the residual plane degree controls its complement. Keeping the different Λ/2\Lambda/2 is necessary at both stages. ◻