Text size

Section 122

The point of a fibre with ramification index two

Let pp be the singular point of a fibre corresponding to a ramification point of index two. We use the ordinary blow-up of pp.

Theorem 122.1. One has δp(X)≥72/67\delta_p(X)\ge72/67.

Lemma 122.2 (The actual initial sections). The exceptional divisor of the ordinary blow-up of pp is G=ℙ2G=\mathbb P^2, and AX(G)=3A_X(G)=3. There are homogeneous coordinates x,z,wx,z,w on GG such that a diagonal degeneration of the actual refined anticanonical series contains the algebra generated in degree one by {1,x,z,w,wx,x2},t{1,x,z,w,wx,x2},t2{1,x,z},zw=x2+t.\{1,x,z,w,wx,x^2\},\qquad t\{1,x,z,w,wx,x^2\},\qquad t^2\{1,x,z\}, \qquad zw=x^2+t. The primary degrees of x,z,w,tx,z,w,t are 1,1,1,21,1,1,2, respectively.

Proof. Write the conic as YC−X2=0YC-X^2=0. On the chart Y=u=1Y=u=1, put x=X/Yx=X/Y, c=C/Yc=C/Y, z=c−x2z=c-x^2 and let t=v/ut=v/u be the target parameter. The centre is cut out by the conic and F=tg(x,c)+f(x,c)F=tg(x,c)+f(x,c). Adding a multiple of the conic equation to ff, and rescaling the target parameter, we may assume f=z+R(x,c),R(x,c)=Ax2+Bxc+Cc2,A≠0,g(0,0)=1.f=z+R(x,c),\qquad R(x,c)=A x^2+Bxc+C c^2,\qquad A\ne0,\qquad g(0,0)=1. The inequality A≠0A\ne0 expresses ramification index two. On the blow-up chart F=zaF=za, put w=a−1w=a-1. Then x,z,wx,z,w are regular parameters at pp, and tg(x,c)=zw−R(x,c),c=z+x2.t g(x,c)=zw-R(x,c),\qquad c=z+x^2. Thus the initial form of tt for the ordinary point valuation is Q=zw−R(x,z)Q=zw-R(x,z).

The complete-intersection ideal sequence gives the fifteen anticanonical sections ti{1,x,c}(0≤i≤2),tia{1,x,c}(0≤i≤1).t^i\{1,x,c\}\quad(0\le i\le2),\qquad t^ia\{1,x,c\}\quad(0\le i\le1). Subtracting the first group from the second gives their initial basis {1,x,z,w,wx,wz},Q{1,x,z,w,wx,wz},Q2{1,x,z}.\{1,x,z,w,wx,wz\},\qquad Q\{1,x,z,w,wx,wz\},\qquad Q^2\{1,x,z\}. These forms are independent; in particular, wzwz and QQ are independent because A≠0A\ne0.

Now give x,z,wx,z,w the secondary weights 1,2,01,2,0. The least secondary term of QQ is zw−Ax2zw-Ax^2. Replacing wzwz by wz−Q=R(x,z)wz-Q=R(x,z) gives Ax2Ax^2, and replacing QwzQwz by Qwz−Q2Qwz-Q^2 gives Ax2(zw−Ax2)Ax^2(zw-Ax^2). After rescaling xx, these are precisely the generators in the statement. Products give an inclusion in every degree. We do not assume generation of the anticanonical ring in degree one. ◻

Lemma 122.3 (The complete normal basis). In anticanonical degree mm, a basis of the algebra above consists of xazbwctsx^az^bw^ct^s, where a,b,c,sa,b,c,s are nonnegative integers, bc=0bc=0, and c=0a+2b≤2m,s≤min(2m,3m−a−b),b=0,c≥1c≤m,a+c≤2m,s≤min(2m−c,3m−a−c).\begin{array}{c|c} c=0 & a+2b\le2m,\quad s\le\min(2m,3m-a-b),\\ b=0,\ c\ge1 & c\le m,\quad a+c\le2m,\quad s\le\min(2m-c,3m-a-c). \end{array} Its dimension is (2m+1)(2m2+2m+1)(2m+1)(2m^2+2m+1). Consequently it is the whole secondary initial algebra of the actual refined series.

Proof. Straighten every factor zwzw by zw=x2+tzw=x^2+t. The only pairs of generators requiring this are z,wz,w and z,wxz,wx. Their products become x2+tx^2+t and x3+xtx^3+xt, respectively. The capacities for powers of tt show that each resulting term is a product of the same number of degree-one generators: zz has capacity two, whereas ww, wxwx and x2x^2 have capacity one. Each replacement reduces the number of zwzw pairs. The resulting monomials are independent, since zwzw is a leading monomial of the single relation.

If c=0c=0, use rr factors x2x^2, a−2ra-2r factors xx and bb factors zz. The smallest possible rr is max(0,a+b−m)\max(0,a+b-m). Such a distribution is possible exactly when a+2b≤2ma+2b\le2m, and its capacity for tt is 2m−r=min(2m,3m−a−b)2m-r=\min(2m,3m-a-b). If c≥1c\ge1, use as many factors wxwx as possible, namely min(a,c)\min(a,c). The smallest necessary number of factors x2x^2 is max(0,a−m)\max(0,a-m). This is possible exactly when c≤mc\le m and a+c≤2ma+c\le2m. The resulting capacity is min(2m−c,3m−a−c)\min(2m-c,3m-a-c). Every smaller nonnegative power of tt can be distributed among these factors.

The two rows contain, respectively, (m+1)(11m2+16m+6)6,m(13m2+9m+2)6\frac{(m+1)(11m^2+16m+6)}6,\qquad \frac{m(13m^2+9m+2)}6 monomials. Their sum is (2m+1)(2m2+2m+1)(2m+1)(2m^2+2m+1), which equals h0(X,−mKX)h^0(X,-mK_X) by Riemann–Roch and Kodaira vanishing. Thus the inclusion of Lemma 122.2 is an equality in every degree. ◻

Lemma 122.4 (The expected order). One has SX(G)=131/48S_X(G)=131/48.

Proof. The primary degree of xazbwctsx^az^bw^ct^s is a+b+c+2sa+b+c+2s. In the first row of Lemma 122.3, put b=m−nb=m-n. Then 0≤n≤m0\le n\le m, 0≤a≤2n0\le a\le2n and 0≤s≤U=min(2m,2m+n−a)0\le s\le U=\min(2m,2m+n-a). In the second row put c=m−nc=m-n. Then 0≤n<m0\le n<m, 0≤a≤m+n0\le a\le m+n and 0≤s≤U=min(m+n,2m+n−a)0\le s\le U=\min(m+n,2m+n-a). In either row the sum in ss is (U+1)(a+m−n)+U(U+1).(U+1)(a+m-n)+U(U+1). Split the first aa-sum at nn and the second at mm. The sums over the two rows are therefore m(m+1)(31m2+43m+16)6,m2(23m2+14m+3)4.\frac{m(m+1)(31m^2+43m+16)}6,\qquad \frac{m^2(23m^2+14m+3)}4. Their sum is m(131m3+190m2+127m+32)12.\frac{m(131m^3+190m^2+127m+32)}{12}. The calculation holds for every nonnegative integer mm. The all-degree equality in Lemma 122.3, or equivalently Lemma 94.2, identifies these primary degrees with the orders of the actual sections. Dividing by m(2m+1)(2m2+2m+1)m(2m+1)(2m^2+2m+1) and taking the limit proves the assertion. ◻

Lemma 122.5 (The binary spaces). The secondary initial series decomposes into complete binary spaces xAzbwctℓSymd(x2,zw).x^Az^bw^ct^\ell\operatorname{Sym}^d(x^2,zw). Their limiting fixed coefficients on (x=0)(x=0), (z=0)(z=0), (w=0)(w=0) and (t=0)(t=0) are, respectively, a0=364,b0=532,c0=732,s0=197384.a_0=\frac3{64},\qquad b_0=\frac5{32},\qquad c_0=\frac7{32},\qquad s_0=\frac{197}{384}. The total mass of the moving pencil is 2h02h_0, where h0=41/128h_0=41/128, and its coefficient at each pencil member is at most h0h_0.

Proof. Let jj and qq be the primary and secondary degrees. Then j=a+b+c+2sj=a+b+c+2s, q=a+2b+2sq=a+2b+2s, so b=max(q−j,0)b=\max(q-j,0) and c=max(j−q,0)c=\max(j-q,0). Put k=j−b−ck=j-b-c. On the first row of the normal basis one has ℓ=max(0,⌈k+2b−2m2⌉,k+b−3m),u=min(2m,⌊k/2⌋),\ell=\max\left(0,\left\lceil\frac{k+2b-2m}{2}\right\rceil, k+b-3m\right),\qquad u=\min(2m,\lfloor k/2\rfloor), and on the second row ℓ=max(0,⌈k+c−2m2⌉,k+c−3m),u=min(2m−c,⌊k/2⌋).\ell=\max\left(0,\left\lceil\frac{k+c-2m}{2}\right\rceil, k+c-3m\right),\qquad u=\min(2m-c,\lfloor k/2\rfloor). Set A=k−2uA=k-2u and d=u−ℓd=u-\ell. Whenever d≥0d\ge0, the corresponding component is precisely the binary space in the statement, since ⟨x2,t⟩=⟨x2,zw⟩\langle x^2,t\rangle=\langle x^2,zw\rangle.

For completeness, the following integrations give all the coefficients. Divide the indices by mm, write y=b/my=b/m or y=c/my=c/m, and let kk denote k/mk/m. In each row 0≤y≤10\le y\le1. The limiting lower and upper bounds for s/ms/m are range of kLUz[0,2−2y]0k/2z[2−2y,4](k+2y−2)/2k/2z[4,5−y]k+y−32w[0,2−y]0k/2w[2−y,4−2y](k+y−2)/2k/2w[4−2y,4−y](k+y−2)/22−yw[4−y,5−2y]k+y−32−y.\begin{array}{c|c|c|c} &\text{range of }k&L&U\\\hline z &[0,2-2y]&0&k/2\\ z &[2-2y,4]&(k+2y-2)/2&k/2\\ z &[4,5-y]&k+y-3&2\\\hline w &[0,2-y]&0&k/2\\ w &[2-y,4-2y]&(k+y-2)/2&k/2\\ w &[4-2y,4-y]&(k+y-2)/2&2-y\\ w &[4-y,5-2y]&k+y-3&2-y. \end{array} Put d=U−Ld=U-L. Integration with respect to dkdydk\,dy gives ∫d∫(k−2U+d)d∫yd∫Ld∫d2/2z11/69/85/87/613/24w13/613/87/885/9671/96.\begin{array}{c|ccccc} &\int d&\int(k-2U+d)d&\int yd&\int Ld&\int d^2/2\\\hline z&11/6&9/8&5/8&7/6&13/24\\ w&13/6&13/8&7/8&85/96&71/96. \end{array} Divide the summed columns by four, since mh0(X,−mKX)=4m4+O(m3)m h^0(X,-mK_X)=4m^4+O(m^3). This gives α=11/16\alpha=11/16, b0=5/32b_0=5/32, c0=7/32c_0=7/32, s0=197/384s_0=197/384 and h0=41/128h_0=41/128, where a0=α−2h0=3/64a_0=\alpha-2h_0=3/64. The rounding and boundary terms contribute O(m3)O(m^3) to the sums. As a check, a0+b0+c0+2s0+4h0=13148.a_0+b_0+c_0+2s_0+4h_0=\frac{131}{48}.

Finally, a basis of a complete binary space of degree dd has total zero multiplicity d(d+1)d(d+1) on the pencil parameter line. Its total order at any prescribed point is at most d(d+1)/2d(d+1)/2. This proves the last assertion, including the two reducible members of the pencil. ◻

Example 122.6. In degree one the primary degrees of the fifteen initial sections are 00, three copies of each of 1,2,3,41,2,3,4, and two copies of 55. Their sum is 4040, agreeing with Lemma 122.4. In anticanonical degree two, the component j=q=2j=q=2 is ⟨x2,t⟩=⟨x2,zw⟩\langle x^2,t\rangle=\langle x^2,zw\rangle. Thus the complete binary spaces include the cancellations along every member of the conic pencil.

Proof of Theorem 122.1. Consider the pencil Tλ=(zw−λx2=0)T_\lambda=(zw-\lambda x^2=0) on GG. Its special members are T0=(z=0)+(w=0)T_0=(z=0)+(w=0) and T∞=2(x=0)T_\infty=2(x=0). Lemma 122.5 bounds the coefficients of every basis divisor of the secondary initial series. The bounds on (x=0)(x=0), (z=0)(z=0), (w=0)(w=0), T1T_1 and all other irreducible members are 1116,61128,69128,56,41128.\frac{11}{16},\qquad\frac{61}{128},\qquad \frac{69}{128},\qquad\frac56,\qquad\frac{41}{128}.

The pencil has base points [0:0:1][0:0:1] and [0:1:0][0:1:0]. Blow up each twice, the second time at the common point of the strict transforms of the finite pencil members. The total boundary then has simple normal crossings. At the first base point the orders on the first and second exceptional curves are a0+b0+s0+2h0+ν∞,a0+2b0+2s0+4h0=83,a_0+b_0+s_0+2h_0+\nu_\infty,\qquad a_0+2b_0+2s_0+4h_0=\frac83, where 0≤ν∞≤h00\le\nu_\infty\le h_0 is the moving coefficient of T∞T_\infty. At the second base point the orders are obtained by replacing b0b_0 with c0c_0, and the second order is 67/2467/24. Their log discrepancies are two and three, respectively. The first order is half the sum of the second order and a0+2ν∞a_0+2\nu_\infty, the coefficient of (x=0)(x=0); hence its ratio is bounded by the larger of the second ratio and 11/1611/16. These blow-ups and the component bounds check all divisorial valuations. The largest ratio of order to discrepancy is 67/7267/72. It follows that for each τ<72/67\tau<72/67, every such basis divisor has log-canonical threshold at least τ\tau for all sufficiently large mm.

For any divisorial valuation over GG, choose in each primary piece a basis compatible with both that valuation and the secondary weight filtration. Two filtrations admit a common adapted basis. Diagonal degeneration gives a basis of the secondary initial series. Lower semicontinuity of log-canonical thresholds gives the same lower bound for the original basis divisor. Passing to the limit yields δ(G;WG)≥72/67\delta(G;W^G)\ge72/67. Abban–Zhuang adjunction and Lemma 122.4 give δp(X)≥min{144131,7267}=7267.\delta_p(X)\ge \min\left\{\frac{144}{131},\frac{72}{67}\right\} =\frac{72}{67}. We have not computed a Zariski decomposition on the blow-up of the threefold. The exact normal basis determines the actual refined series and its expected orders. All subsequent blow-ups occur on its exceptional plane, to resolve the conic pencil. ◻