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Section 94

The exceptional surface at an index-three point

We now prove the exceptional-surface inequality that was missing for ramification index three. This argument applies whether the fibre has one A2A_2 singularity or has an A2A_2 and an A1A_1 singularity. Throughout this section pp is its A2A_2 point, GG is the exceptional divisor of the weight-(1,2,1)(1,2,1) blow-up of pp, and W=WGW=W^G is the actual refined series. Thus G=ℙ(1,2,1)G=\mathbb P(1,2,1) has zero different. We retain the normalization Nm=h0(X,mL)=10m3+15m2+11m+33.N_m=h^0(X,mL)=\frac{10m^3+15m^2+11m+3}{3}. A basis divisor of WW is the sum of the zero divisors of bases of all Wm,jW_{m,j}, divided by mNmmN_m. The denominator is not the dimension of any one homogeneous piece.

Theorem 94.1. At an index-three ramification point one has δ(G;W)≥160151,δp(X)≥160151>1.\delta(G;W)\ge\frac{160}{151},\qquad \delta_p(X)\ge\frac{160}{151}>1.

We give the algebra of the refinement, its expected orders, and the log-canonical calculation as separate lemmas. In particular, finite computations of products of sections are not used to assert generation of the section ring.

Lemma 94.2 (Comparison with the actual filtered section ring). Let LL be a line bundle on a smooth projective integral variety XX, let p∈Xp\in X, and let vv be the monomial valuation in regular parameters at pp with positive integral weights. Trivialize LL near pp, and put Rm=H0(X,mL)R_m=H^0(X,mL). Let BB be either grvR\mathop{\mathrm{gr}}_vR or a further associated graded algebra obtained by a weight filtration that preserves the primary vv-grading. Suppose that a graded algebra 𝒜⊂B\mathcal A\subset B is generated by initial forms of actual sections, and that dim𝒜m=dimRm(m≥0).\dim\mathcal A_m=\dim R_m\qquad(m\ge0). Then 𝒜=B\mathcal A=B. A primary-homogeneous basis of 𝒜m\mathcal A_m computes the complete multiset of vv-orders of an adapted basis of RmR_m, including all cancellations between sections.

Proof. Restriction of global sections to the completed local ring at pp is injective. The weighted initial form of a product of two nonzero local functions is the product of their weighted initial forms, because the weighted polynomial ring in the regular parameters is a domain. Thus initial forms of actual sections, and their products, give the asserted algebra inclusion. Each RmR_m has a finite, exhaustive and separated filtration. Taking its associated graded preserves its dimension; applying a second such filtration does so again, separately in each primary degree. Consequently dimBm=dimRm\dim B_m=\dim R_m. The inclusion and the assumed equality of dimensions give 𝒜m=Bm\mathcal A_m=B_m for every mm. Since the inclusion preserves primary degrees, it is an equality in each primary degree. Those dimensions are precisely the multiplicities of the jumping numbers of the original valuation filtration. This proves the last assertion. No generation or flat base-change assertion for the anticanonical ring is required. ◻

Lemma 94.3 (Thirteen sections and a second degeneration). In coordinates on GG of weights (1,2,1)(1,2,1), put t=zw−x3,c=x2+z,a=w+x.t=zw-x^3,\qquad c=x^2+z,\qquad a=w+x. The series WW contains the degree-one sections ti{1,x,c}(0≤i≤2),a,xa,ta,txa.t^i\{1,x,c\}\ (0\le i\le2),\qquad a,\ xa,\ ta,\ txa. Here degree one means anticanonical degree m=1m=1; the second grading is the weighted degree in x,z,wx,z,w. Degenerate these spaces by the one-parameter subgroup with weights (1,0,3)(1,0,3) on (x,z,w)(x,z,w), taking least weights. The resulting algebra contains the algebra 𝒜\mathcal A generated in degree one by {1,x,z,w,x2},t{1,x,z,w,x2},t2{1,x,z}.\{1,x,z,w,x^2\},\quad t\{1,x,z,w,x^2\},\quad t^2\{1,x,z\}. The relation is zw=x3+tzw=x^3+t.

Proof. Use the central model from Lemma 93.2, whose centre has equation ux3y2+vy5=0ux^3y^2+vy^5=0. On the chart u=y2=1u=y^2=1 of MM, write the plane coordinates as xx and cc and the conic equation as z=c−x2z=c-x^2. One lift of the graph equation is t+xct+xc; a second lift, after multiplication by the other source coordinate, is x(t+xc)x(t+xc). On the blow-up chart put a=(t+xc)/za=(t+xc)/z and then w=a−xw=a-x. This gives t=zw−x3t=zw-x^3. The conic equation times the nine sections of 𝒪M(2,1)\mathcal O_M(2,1) gives ti{1,x,c}t^i\{1,x,c\} after division by the exceptional equation. The two lifted graph equations, multiplied by the two target coordinates, give a,xa,ta,txaa,xa,ta,txa. These are sections of L=2T+3H−EL=2T+3H-E. Their thirteen polynomials are independent, so they form the entire degree-one space.

These are also the primary initial sections on the original smooth threefold. Indeed its normalized quintics begin with x3y2x^3y^2 and y5y^5. Higher terms in the first lifted graph equation have primary weight greater than three; higher terms in the second have weight greater than four. Dividing by the exceptional equation, of weight two, therefore leaves the same initial forms aa and xaxa. The target coordinate has initial form zw−x3zw-x^3. Thus the claimed inclusion can be checked directly from the original sections, without assuming generation or base change for the entire ring. The secondary weights make t=zw−x3t=zw-x^3 homogeneous of weight three. Since both xx and aa occur, we may replace aa by a−x=wa-x=w; likewise we replace tata by twtw. The least-weight terms of cc and xaxa are zz and x2x^2, respectively. This gives the thirteen displayed initial sections. Products of these initial sections belong to the initial algebra of WW, proving the claimed inclusion. ◻

Lemma 94.4 (An exact normal basis). The degree-mm space of 𝒜\mathcal A has basis xazbwcts,x^a z^b w^c t^s, where a,b,c,sa,b,c,s are nonnegative integers satisfying (35.1)bc=0,a+2b+2c≤2m,s+c≤2m,s+a+b+2c≤3m.bc=0,\qquad a+2b+2c\le2m,\qquad s+c\le2m, \qquad s+a+b+2c\le3m. \tag{35.1} Its dimension is NmN_m. Consequently 𝒜\mathcal A is the entire secondary initial algebra of WW in every degree.

Proof. First straighten a product containing both zz and ww. Its factors include ztizt^i and wtjwt^j with 0≤i≤20\le i\le2, 0≤j≤10\le j\le1. Use (zti)(wtj)=(xti)(x2tj)+ti+j+1.(zt^i)(wt^j)=(xt^i)(x^2t^j)+t^{i+j+1}. The first term remains a product of two listed generators. The second is also a product of two such generators, since i+j+1≤4i+j+1\le4 and 1,t,t21,t,t^2 are generators. Repeating reduces the number of zwzw pairs, without increasing anticanonical degree. The resulting monomials have bc=0bc=0. These normal monomials are linearly independent in ℂ[x,z,w,t]/(zw−x3−t)\mathbb C[x,z,w,t]/(zw-x^3-t): the single defining relation has leading monomial zwzw for a suitable monomial order.

We next decide which normal monomials are products of at most mm generators. Use kk factors of type x2tix^2t^i and a−2ka-2k of type xtixt^i, together with bb factors of type ztizt^i and cc of type wtiwt^i. Fill the remaining places with 1,t,t21,t,t^2. This is possible exactly when max(0,a+b+c−m)≤k≤⌊a/2⌋,s≤2m−k−c.\max(0,a+b+c-m)\le k\le\lfloor a/2\rfloor, \qquad s\le2m-k-c. Indeed the last number is the total available tt-exponent; all integers between zero and this number can be distributed among the factors. Taking the smallest allowed kk gives precisely (35.1).

For completeness, count the basis. If c=0c=0, put n=m−bn=m-b. There are 0≤a≤2n0\le a\le2n, and 0≤s≤min(2m,3m−a−b).0\le s\le\min(2m,3m-a-b). The contribution for this bb is (2n+1)(2m+1)−n(n+1)2.(2n+1)(2m+1)-\frac{n(n+1)}2. If b=0b=0 and c≥1c\ge1, put n=m−cn=m-c; the contribution is (2n+1)(m+n+1)−n(n+1)2.(2n+1)(m+n+1)-\frac{n(n+1)}2. Thus the total is ∑n=0m((2n+1)(2m+1)−n(n+1)2)+∑n=0m−1((2n+1)(m+n+1)−n(n+1)2)=(m+1)(11m2+16m+6)6+m2(3m+1)2=Nm.\begin{aligned} &\sum_{n=0}^m\left((2n+1)(2m+1)-\frac{n(n+1)}2\right) +\sum_{n=0}^{m-1}\left((2n+1)(m+n+1)-\frac{n(n+1)}2\right)\\ &\quad =\frac{(m+1)(11m^2+16m+6)}6 +\frac{m^2(3m+1)}2=N_m. \end{aligned} Lemma 94.2 now identifies this algebra with the entire secondary initial algebra of the actual refinement. In particular this proves generation in every degree.

The primary weights admit the following independent, all-degree check. For a row with 0≤s≤U0\le s\le U, use ∑s=0U(a+2b+c+3s)=(U+1)(a+2b+c)+32U(U+1).\sum_{s=0}^{U}(a+2b+c+3s) =(U+1)(a+2b+c)+\frac32U(U+1). On the first branch put b=m−nb=m-n, 0≤n≤m0\le n\le m, and 0≤a≤2n0\le a\le2n; then U=min(2m,2m+n−a)U=\min(2m,2m+n-a). On the second branch put c=m−nc=m-n, 0≤n<m0\le n<m, and 0≤a≤2n0\le a\le2n; then U=min(m+n,m+2n−a)U=\min(m+n,m+2n-a). Splitting both aa-sums at a=na=n gives, respectively, m(m+1)(45m2+61m+23)6,m2(59m2+6m−5)12.\frac{m(m+1)(45m^2+61m+23)}6,\qquad \frac{m^2(59m^2+6m-5)}{12}. Their sum is m(149m3+218m2+163m+46)12.\frac{m(149m^3+218m^2+163m+46)}{12}. These are polynomial summations for every m≥0m\ge0, rather than an extrapolation from finitely many Hilbert values. Dividing the last expression by mNmmN_m recovers SX(G)=149/40S_X(G)=149/40. ◻

Lemma 94.5 (Complete binary spaces with fixed factors). Fix mm, a primary degree jj and a secondary weight qq. Put b=max(j−q2,0),c=max(q−j2,0),k=q−3c.b=\max\left(\frac{j-q}{2},0\right),\qquad c=\max\left(\frac{q-j}{2},0\right),\qquad k=q-3c. If these numbers are nonnegative integers where required, set ℓ=max(0,⌈k+2b+2c−2m3⌉,⌈k+b+2c−3m2⌉),u=min(2m−c,⌊k3⌋).\ell=\max\left(0, \left\lceil\frac{k+2b+2c-2m}{3}\right\rceil, \left\lceil\frac{k+b+2c-3m}{2}\right\rceil\right),\qquad u=\min\left(2m-c,\left\lfloor\frac{k}{3}\right\rfloor\right). The component is zero unless u≥ℓu\ge\ell. Otherwise, with d=u−ℓd=u-\ell and A=k−3uA=k-3u, it is exactly (35.2)xAzbwctℓSymd(x3,zw).x^A z^b w^c t^\ell\operatorname{Sym}^d(x^3,zw). \tag{35.2} In particular its dimension is d+1d+1.

Proof. A normal monomial has primary degree a+2b+c+3sa+2b+c+3s and secondary weight a+3c+3sa+3c+3s. Their difference determines b−cb-c, and bc=0bc=0 determines b,cb,c. The remaining equation is a+3s=ka+3s=k. Substitution in (35.1) gives exactly ℓ≤s≤u\ell\le s\le u. The normal basis in this component is therefore xAzbwctℓ{x3(d−i)ti:0≤i≤d}.x^A z^b w^c t^\ell\{x^{3(d-i)}t^i:0\le i\le d\}. Since t=zw−x3t=zw-x^3, its span is (35.2). ◻

Example 94.6. For m=2m=2, j=q=3j=q=3, one has b=c=0b=c=0, k=3k=3, ℓ=0\ell=0, u=1u=1. The component is the two-dimensional space ⟨x3,t⟩=⟨x3,zw⟩.\langle x^3,t\rangle=\langle x^3,zw\rangle. The cancellation zw−t=x3zw-t=x^3 is thus built into the complete binary space. Its contribution to the maximal average vanishing at any prescribed point of the quotient pencil is 1/(2N2)1/(2N_2), since the two basis orders are zero and one. It would be incorrect to count the two polynomials as independent monomials in x,z,wx,z,w without this cancellation.

Lemma 94.7 (Separate expected-order computation on GG). Sum over the nonzero components in (35.2), and define αm=1mNm∑(A+3d2)(d+1),bm=1mNm∑b(d+1),cm=1mNm∑c(d+1),sm=1mNm∑ℓ(d+1),hm=12mNm∑d(d+1).\begin{aligned} \alpha_m&=\frac1{mN_m}\sum\left(A+\frac{3d}{2}\right)(d+1),& b_m&=\frac1{mN_m}\sum b(d+1),& c_m&=\frac1{mN_m}\sum c(d+1),\\ s_m&=\frac1{mN_m}\sum\ell(d+1),& h_m&=\frac1{2mN_m}\sum d(d+1). \end{aligned} Their limits are (35.3)α=58,b=316,c=1180,s=79120,h=49240.\alpha=\frac58,\qquad b=\frac3{16},\qquad c=\frac{11}{80}, \qquad s=\frac{79}{120},\qquad h=\frac{49}{240}. \tag{35.3} The two weighted-corner moments have limits (35.4)α+3(c+s+h)=298,α+3(b+s+h)=15140.\alpha+3(c+s+h)=\frac{29}{8},\qquad \alpha+3(b+s+h)=\frac{151}{40}. \tag{35.4}

Proof. Here is an explicit integration of the normal-basis count. The two branches are c=0c=0, called the zz-branch, and b=0b=0, called the ww-branch. Their common boundary contributes only lower-order terms. Write y=b/my=b/m on the first branch and y=c/my=c/m on the second, and write k/mk/m again as kk. The lower and upper limits for s/ms/m are LUzmax(0,(k+2y−2)/3,(k+y−3)/2)min(2,k/3)wmax(0,(k+2y−2)/3,(k+2y−3)/2)min(2−y,k/3).\begin{array}{c|c|c} &L&U\\ \hline z&\max(0,(k+2y-2)/3,(k+y-3)/2)&\min(2,k/3)\\ w&\max(0,(k+2y-2)/3,(k+2y-3)/2)&\min(2-y,k/3). \end{array} Set d=U−Ld=U-L in these integrals. The region is 0≤y≤10\le y\le1, L≤UL\le U. It has the following four strips on each branch; all integrals below are ordinary integrals ∫01∫dkdy\int_0^1\int dk\,dy. branchrange of kLUz[0,2−2y]0k/3z[2−2y,5+y](k+2y−2)/3k/3z[5+y,6](k+y−3)/2k/3z[6,7−y](k+y−3)/22w[0,2−2y]0k/3w[2−2y,5−2y](k+2y−2)/3k/3w[5−2y,6−3y](k+2y−3)/2k/3w[6−3y,7−4y](k+2y−3)/22−y.\begin{array}{c|c|c|c} \text{branch}&\text{range of }k&L&U\\ \hline z&[0,2-2y]&0&k/3\\ z&[2-2y,5+y]&(k+2y-2)/3&k/3\\ z&[5+y,6]&(k+y-3)/2&k/3\\ z&[6,7-y]&(k+y-3)/2&2\\ \hline w&[0,2-2y]&0&k/3\\ w&[2-2y,5-2y]&(k+2y-2)/3&k/3\\ w&[5-2y,6-3y]&(k+2y-3)/2&k/3\\ w&[6-3y,7-4y]&(k+2y-3)/2&2-y. \end{array} Integrating the indicated polynomials gives (35.5)∫d∫(k−3U+3d/2)d∫yd∫Ld∫d2/2z11/69/85/8193/14453/144w3/223/2411/2441/485/16.\begin{array}{c|ccccc} &\int d&\int(k-3U+3d/2)d&\int yd&\int Ld&\int d^2/2\\ \hline z&11/6&9/8&5/8&193/144&53/144\\ w&3/2&23/24&11/24&41/48&5/16. \end{array} \tag{35.5} For example, on the first strip of the zz-branch, d=k/3d=k/3, so its contributions to the first, second and last columns are ∫01∫02−2yk3dkdy=29,∫01∫02−2yk26dkdy=19,∫01∫02−2yk218dkdy=127.\int_0^1\int_0^{2-2y}\frac{k}{3}\,dk\,dy=\frac29,\quad \int_0^1\int_0^{2-2y}\frac{k^2}{6}\,dk\,dy=\frac19,\quad \int_0^1\int_0^{2-2y}\frac{k^2}{18}\,dk\,dy=\frac1{27}. The other entries follow by substituting the displayed affine L,UL,U in the same integrals. Floors, ceilings and boundary rows change the order sums by O(m3)O(m^3), whereas mNm=(10/3)m4+O(m3)mN_m=(10/3)m^4+O(m^3). Thus multiply the summed columns by 3/103/10. The third column contributes to bb on the first branch and to cc on the second. This proves (35.3); substitution gives (35.4).

As an additional normalization check, the fixed xx-coefficient is α−3h=180.\alpha-3h=\frac1{80}. Since x,z,w,tx,z,w,t have weighted degrees 1,2,1,31,2,1,3, the average divisor class obtained from (35.2) has degree (α−3h)+2b+c+3s+6h=14940=SX(G),(\alpha-3h)+2b+c+3s+6h=\frac{149}{40}=S_X(G), in agreement with the independent threefold calculation. ◻

Lemma 94.8 (A log resolution of the pencil). On G=ℙ(1,2,1)G=\mathbb P(1,2,1) put X0=(x=0),Z0=(z=0),W0=(w=0),Tλ=(zw−λx3=0),X_0=(x=0),\quad Z_0=(z=0),\quad W_0=(w=0),\quad T_\lambda=(zw-\lambda x^3=0), where T0=Z0+W0T_0=Z_0+W_0 and T∞=3X0T_\infty=3X_0. Suppose an effective divisor has the form B=aX0+bZ0+cW0+sT1+∑λ∈ℙ1νλTλ,B=aX_0+bZ_0+cW_0+sT_1+\sum_{\lambda\in\mathbb P^1} \nu_\lambda T_\lambda, with nonnegative coefficients, finite support, ∑νλ=2h\sum\nu_\lambda=2h and νλ≤h\nu_\lambda\le h. Put α=a+3h\alpha=a+3h. The pair (G,B)(G,B) is log canonical if α,b+h,c+h,s+h,h≤1\alpha,\ b+h,\ c+h,\ s+h,\ h\le1 and (35.6)α+3(c+s+h)≤4,α+3(b+s+h)≤4.\alpha+3(c+s+h)\le4,\qquad \alpha+3(b+s+h)\le4. \tag{35.6}

Proof. Away from the three coordinate vertices, the curves of this pencil are disjoint and smooth, and the displayed component bounds suffice. At [1:0:0][1:0:0], only Z0Z_0 and W0W_0 occur; they cross transversely.

At [0:1:0][0:1:0], take the index-two cover of the chart z=1z=1. It is 𝔸x,w2\mathbb A^2_{x,w} modulo the involution (x,w)↦(−x,−w)(x,w)\mapsto(-x,-w); the cover is quasi-étale. The curves in question are x=0x=0 and w=λx3w=\lambda x^3. Write u=a+3ν∞,v=c+s+2h−ν∞.u=a+3\nu_\infty,\qquad v=c+s+2h-\nu_\infty. Three successive ordinary blow-ups separate the branches w=λx3w=\lambda x^3. Their exceptional valuations have weights (1,i)(1,i), i=1,2,3i=1,2,3, in (x,w)(x,w), log discrepancies 1+i1+i, and orders u+ivu+iv on BB. The component bound gives u≤1u\le1, and the first inequality of (35.6) gives u+3v=a+3c+3s+6h=α+3(c+s+h)≤4.u+3v=a+3c+3s+6h=\alpha+3(c+s+h)\le4. Linear interpolation gives u+iv≤1+iu+iv\le1+i for i=1,2i=1,2 as well. After the third blow-up all distinct branches meet the last exceptional curve at different points; the total transform has simple normal crossings and every coefficient is at most one. Log canonicity descends through the quasi-étale cover.

The chart w=1w=1 at [0:0:1][0:0:1] is smooth. Its curves are x=0x=0 and z=λx3z=\lambda x^3. The identical three-blow-up calculation, with bb in place of cc, uses the second inequality of (35.6). This verifies every point and every exceptional divisor on a log resolution, and therefore all divisorial valuations over GG. ◻

Lemma 94.9 (All basis divisors of the initial series). Let BmB_m be any basis divisor obtained by taking an arbitrary basis in each primary-degree and secondary-weight component of 𝒜\mathcal A. For every τ<160/151\tau<160/151, the pair (G,τBm)(G,\tau B_m) is log canonical for all sufficiently large mm, independently of the chosen bases.

Proof. In (35.2), remove the fixed factor. A basis of the remaining complete binary space has total degree d(d+1)d(d+1) on the quotient ℙ1\mathbb P^1. At any prescribed point the sum of its vanishing orders is at most 0+1+⋯+d=d(d+1)2.0+1+\cdots+d=\frac{d(d+1)}2. This follows immediately from the dimensions of the subspaces with vanishing order at least ii. Thus BmB_m has the form in Lemma 94.8, with a=αm−3hm,b=bm,c=cm,s=sm,h=hm.a=\alpha_m-3h_m,\quad b=b_m,\quad c=c_m,\quad s=s_m, \quad h=h_m. All these coefficients are nonnegative by their definitions. In the limit the component bounds in that lemma are 58,47120,41120,6980,49240.\frac58,\quad\frac{47}{120},\quad\frac{41}{120}, \quad\frac{69}{80},\quad\frac{49}{240}. The corner bounds, divided by their log discrepancy four, are 2932,151160.\frac{29}{32},\qquad\frac{151}{160}. The largest of these seven numbers is 151/160151/160. Multiplication by any fixed τ<160/151\tau<160/151 therefore makes all inequalities strict for sufficiently large mm. The log-resolution lemma applies. ◻

Proof of Theorem 94.1. Fix a divisorial valuation vv over GG. In each Wm,jW_{m,j} choose a basis compatible with both its vv-filtration and its secondary weight filtration. Such a basis exists for two filtrations; see Lemma 2.3. Its least-weight terms give a basis in each of the components of 𝒜\mathcal A. Degenerating the sum of its zero divisors under the same one-parameter subgroup gives exactly the basis divisor considered in Lemma 94.9. Lower semicontinuity of log-canonical thresholds in this family gives the same lower bound for the original basis divisor. Since the basis was vv-adapted, its order at vv is Sm(W;v)S_m(W;v). Hence, for each τ<160/151\tau<160/151 and all large mm, τSm(W;v)≤AG(v).\tau S_m(W;v)\le A_G(v). Taking the limit and then letting τ\tau increase to 160/151160/151 proves the first assertion. Only two filtrations were split on an already fixed primary piece; no basis compatible with three unrelated filtrations is assumed.

Weighted point blow-up is a plt extraction, with zero different here. Abban–Zhuang adjunction, in the form of [3, Corollary 1.102], now yields δp(X)≥min{AX(G)SX(G),δ(G;W)}≥min{160149,160151}=160151.\delta_p(X)\ge \min\left\{\frac{A_X(G)}{S_X(G)},\delta(G;W)\right\} \ge\min\left\{\frac{160}{149},\frac{160}{151}\right\} =\frac{160}{151}. We have not computed a Zariski decomposition on the weighted blow-up of the threefold. The normal basis (35.1), its exact Hilbert count and the complete binary spaces (35.2) identify the actual refinement. The only further blow-ups in this proof are the explicit surface blow-ups in Lemma 94.8. ◻

Example 94.10 (An A2+A1A_2+A_1 fibre). For the graph of [x:y]↦[x3y2:x5+y5],[x:y]\longmapsto[x^3y^2:x^5+y^5], the fibre over zero has an A2A_2 point and an A1A_1 point. The theorem gives δp(X)≥160/151\delta_p(X)\ge160/151 at the A2A_2 point. The proof retains the factor y2y^2 in the central graph and consequently does not require the other length-two cluster in the fibre to split into separate points. This local assertion alone does not settle all other centres on that fibre.