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Section 114

Points on the original exceptional divisor

114.1 The point where a bad line meets the exceptional divisor

We give the point extraction needed at the intersection of a line on an A2A_2 fibre with the exceptional divisor of the original elliptic blow-up. The other ruling is obtained by interchanging the two planes.

Lemma 114.1. Let SS be an A2A_2 fibre, let ℓ\ell be one of its two lines, and let p=ℓ∩Ep=\ell\cap E. There are regular parameters (a,t,z)(a,t,z) on XX at pp with the following description. Put U=a2+abz,V=ab+b2z,H=⟨1,a,b,z,az,bz,U,V⟩.U=a^2+abz,\qquad V=ab+b^2z,\qquad H=\langle1,a,b,z,az,bz,U,V\rangle. The local equation of XX is b+U+tg=0,b+U+tg=0, where g∈Hg\in H, g(p)=0g(p)=0, and the coefficient of zz in gg is nonzero. After rescaling tt, we have b=−Q+O((a,t,z)3),Q=a2+αat+tzb=-Q+O((a,t,z)^3),\qquad Q=a^2+\alpha at+tz for some α∈ℂ\alpha\in\mathbb C. A basis of the anticanonical sections is 1,a,z,az,bz,U,V,t,ta,tb,tz,taz,tbz,tU,tV.1,a,z,az,bz,U,V,t,ta,tb,tz,taz,tbz,tU,tV.

Proof. On the incidence threefold use coordinates x=(a,b,1),y=(1,z,−a−bz).x=(a,b,1),\qquad y=(1,z,-a-bz). Its bilinear sections form the space HH. A regular nilpotent matrix may be chosen so that the second bilinear equation is b+U=0b+U=0. The line under consideration is a=b=0a=b=0; its singular endpoint is z=∞z=\infty. The unipotent centralizer acts transitively on the complement of that endpoint, so that the point under consideration may be put at z=0z=0. The other pencil generator restricts to a linear polynomial on the line. Its coefficient at zz is nonzero: otherwise it would vanish at the singular endpoint, contrary to smoothness of the base curve. Its constant coefficient is zero because p∈Ep\in E. The implicit function theorem applied to b+U+tgb+U+tg gives the displayed quadratic term of bb. The anticanonical sections are H+tHH+tH. Their unique linear relation is b+U+tg=0b+U+tg=0, which eliminates bb. ◻

Lemma 114.2. Let MM consist of the following fifteen lattice points, in the order shown: (0,0,0),(0,0,1),(0,1,0),(0,1,1),(0,1,2),(0,2,1),(0,2,2),(1,0,0),(1,0,1),(1,1,0),(1,1,1),(1,2,1),(2,0,0),(2,1,0),(3,0,0).\begin{aligned} &(0,0,0),(0,0,1),(0,1,0),(0,1,1),(0,1,2),\\ &(0,2,1),(0,2,2),(1,0,0),(1,0,1),(1,1,0),\\ &(1,1,1),(1,2,1),(2,0,0),(2,1,0),(3,0,0). \end{aligned} The semigroup generated by (1,q)(1,q), q∈Mq\in M, has precisely 4m3+6m2+4m+14m^3+6m^2+4m+1 elements of degree mm. Its degree-one convex body has volume 44 and barycentre (4148,56,3548).\left(\frac{41}{48},\frac56,\frac{35}{48}\right).

Proof. The convex hull is cut out by a,t,z≥0,t≤2,|t−z|≤1,a+t≤3,a−t+2z≤3,2a+3z≤6,2a+t+2z≤6.\begin{gathered} a,t,z\geq0,\quad t\leq2,\quad |t-z|\leq1,\quad a+t\leq3,\\ a-t+2z\leq3,\quad 2a+3z\leq6,\quad 2a+t+2z\leq6. \end{gathered} Here is an explicit unimodular triangulation, with the points indexed from 00 to 1414. Every tetrahedron has vertex 1010; its other three vertices are the following: (0,1,2)(0,1,7)(0,2,7)(1,2,3)(1,3,4)(1,4,8)(1,7,8)(2,3,5)(2,5,11)(2,7,9)(2,9,11)(3,4,6)(3,5,6)(4,6,14)(4,8,14)(5,6,11)(6,11,14)(7,8,12)(7,9,13)(7,12,13)(8,12,14)(9,11,13)(11,13,14)(12,13,14).\begin{array}{rrrrrr} (0,1,2)&(0,1,7)&(0,2,7)&(1,2,3)&(1,3,4)&(1,4,8)\\ (1,7,8)&(2,3,5)&(2,5,11)&(2,7,9)&(2,9,11)&(3,4,6)\\ (3,5,6)&(4,6,14)&(4,8,14)&(5,6,11)&(6,11,14)&(7,8,12)\\ (7,9,13)&(7,12,13)&(8,12,14)&(9,11,13)&(11,13,14)&(12,13,14). \end{array} The boundary triangles tile the boundary of the convex hull; taking cones from its interior point (1,1,1)(1,1,1) gives the claimed triangulation. Each determinant has absolute value one. In particular the polytope has the integer decomposition property. The numbers of vertices, edges, triangles, and tetrahedra are 15,50,60,2415,50,60,24, respectively. Counting lattice points in the relative interiors of the dilated simplices gives, for m≥1m\geq1, 15+50(m−1)+60(m−12)+24(m−13)=4m3+6m2+4m+1.15+50(m-1)+60\binom{m-1}{2}+24\binom{m-1}{3} =4m^3+6m^2+4m+1. The tetrahedra have equal volume 1/61/6. The barycentre is therefore the mean of their barycentres, which is the displayed vector. ◻

Lemma 114.3. In the notation of Lemma 114.1, let G≅ℙ2G\cong\mathbb P^2 be the exceptional divisor of the ordinary blow-up of pp. Then SX(G)=2912,δp(X)≥4841>1.S_X(G)=\frac{29}{12},\qquad \delta_p(X)\geq\frac{48}{41}>1.

Proof. First take the lowest ordinary homogeneous parts in the parameters (a,t,z)(a,t,z). Within each ordinary degree, refine by the lexicographic order on the exponents of a,t,za,t,z, taking the least exponent first. The fifteen sections in Lemma 114.1 can be adapted to these two filtrations. Their refined initial monomials are exactly those with exponent vectors in Lemma 114.2. Here are the only cancellations needed to see this. The leading terms of bz,tb,tbz,tVbz,tb,tbz,tV are respectively −zQ,−tQ,−tzQ,−atQ.-zQ,\quad -tQ,\quad -tzQ,\quad -atQ. The sections U,tUU,tU have initial terms a2,a2ta^2,a^2t. Moreover V+taz+αtUV+taz+\alpha tU has initial term −a3-a^3. Subtracting the a2ta^2t term from tbtb leaves a cubic whose least refined monomial is t2zt^2z. The least refined monomials of the other three displayed expressions are tz2,t2z2,at2ztz^2,t^2z^2,at^2z. The remaining sections give 1,a,z,az,t,at,tz,atz,a2,a2t1,a,z,az,t,at,tz,atz,a^2,a^2t. All fifteen initial monomials are distinct.

Products of these sections give all the semigroup monomials in every degree. Their number is, by Lemma 114.2, exactly h0(X,−mKX)=4m3+6m2+4m+1.h^0(X,-mK_X)=4m^3+6m^2+4m+1. Consequently they exhaust the actual refined section spaces in every degree. This is an equality of section spaces; a calculation of a convex hull alone would not suffice.

The ordinary order is the sum of the three exponents. Hence the barycentre calculation gives SX(G)=4148+56+3548=2912.S_X(G)=\frac{41}{48}+\frac56+\frac{35}{48}=\frac{29}{12}. We also explain the estimate on the exceptional plane. Fix any valuation on GG. For each ordinary graded piece, choose a basis adapted both to that valuation and to the refining monomial filtration. For fixed mm the latter filtration is induced by an integral one-parameter subgroup of the diagonal torus of GG; its weights can be chosen to realize the required lexicographic order on all the monomials in question. The basis divisor degenerates to a divisor supported on the three coordinate lines. The asymptotic coefficients of those lines are 4148,56,3548.\frac{41}{48},\quad\frac56,\quad\frac{35}{48}. The three lines form a simple normal crossing divisor on ℙ2\mathbb P^2. Lower semicontinuity of log canonical thresholds therefore gives δ(G;W•,•G)≥4841.\delta(G;W^G_{\bullet,\bullet})\geq\frac{48}{41}. Abban–Zhuang adjunction and AX(G)=3A_X(G)=3 now give δp(X)≥min{329/12,4841}=4841.\delta_p(X)\geq \min\left\{\frac{3}{29/12},\frac{48}{41}\right\} =\frac{48}{41}. We have used no Zariski decomposition on the extracted threefold. The complete section algebra and its two filtrations supply both SX(G)S_X(G) and the required restricted-series estimate. ◻

114.2 The exceptional points on the two lines of an A1A_1 fibre

Lemma 114.4. Let Γ\Gamma be one of the two lines through the singular point of an A1A_1 fibre, and put p=Γ∩Ep=\Gamma\cap E. There are two cases. If pp is not the intersection with another line on the fibre, its ordinary point extraction has the same refined section algebra as in Lemma 114.3. If pp is such an intersection, there are regular parameters a,z,ta,z,t in which its ordinary initial section space has a basis 1,a,z,t,az,at,zt,a2(z+t),z2t,azt,t2(a+z),taQ,az2t,t2z(a+z),t2(a+z)Q,Q=az+t(a+z).\begin{gathered} 1,a,z,t,az,at,zt,\quad a^2(z+t),z^2t,azt,t^2(a+z),\\ taQ,az^2t,t^2z(a+z),\quad t^2(a+z)Q, \qquad Q=az+t(a+z). \end{gathered}

Proof. It suffices to consider one projection; transposition interchanges the two lines. Write the flag and fibre equations as x0y0+x1y1+x2y2=0,x0y1+x2y2=0.x_0y_0+x_1y_1+x_2y_2=0,\qquad x_0y_1+x_2y_2=0. The singular point is ([0:1:0],[1:0:0])([0:1:0],[1:0:0]), and the line considered is x=[0:1:0]x=[0:1:0], y1=0y_1=0. Its point on the base curve has coordinates y=[ρ:0:1]y=[\rho:0:1] for some ρ∈ℂ\rho\in\mathbb C. On x1=y2=1x_1=y_2=1 use regular coordinates a=x0,z=y0−ρ,h=y1+ρa.a=x_0,\qquad z=y_0-\rho,\qquad h=y_1+\rho a. Then x2=−az−hx_2=-az-h. Put R=az+h,K=zR,L=R(ρa−h),f=ah−ρa2−R.R=az+h,\quad K=zR,\quad L=R(\rho a-h),\quad f=ah-\rho a^2-R. The eight bilinear sections span ⟨1,a,z,h,az,K,L,f⟩.\langle1,a,z,h,az,K,L,f\rangle. The second pencil generator gg vanishes at pp and has linear term z+γa+βhz+\gamma a+\beta h after rescaling. Its zz-coefficient is nonzero because its restriction to Γ\Gamma has a simple zero at pp. The blow-up chart is f=tgf=tg, and a,z,ta,z,t are regular parameters.

Suppose first that ρ≠0\rho\ne0. We may replace zz by the regular coordinate c=gc=g; its linear term on XX is z+γaz+\gamma a. The quadratic terms of R,hR,h are R2=−ρa2−tc,h2=(γ−ρ)a2−(a+t)c.R_2=-\rho a^2-tc,\qquad h_2=(\gamma-\rho)a^2-(a+t)c. Use R+f=ah−ρa2R+f=ah-\rho a^2 in place of hh. The quadratic initial forms of az,R+f,faz,R+f,f span ac,a2,tcac,a^2,tc. Moreover K3=−(c−γa)(ρa2+tc),L3=−ρa(ρa2+tc).K_3=-(c-\gamma a)(\rho a^2+tc),\qquad L_3=-\rho a(\rho a^2+tc). Thus the eight bilinear initial forms can be chosen as 1,a,c,a2,ac,aQ,cQ,tc,Q=ρa2+tc.1,a,c,a^2,ac,aQ,cQ,tc,\qquad Q=\rho a^2+tc. Removing ff from H+tHH+tH gives seven of these forms and tt times all eight. After rescaling aa the resulting algebra is the one used in Lemma 114.3, with the coordinates renamed. In comparing the two displayed bases, use tQ=ρa2t+t2ctQ=\rho a^2t+t^2c to interchange tQtQ and t2ct^2c.

Suppose now that ρ=0\rho=0. The fibre contains the second line z=h=0z=h=0 through pp. We must have γ≠0\gamma\ne0: otherwise gg vanishes identically on this line, so the smooth elliptic base curve would contain it. A diagonal rescaling permits γ=1\gamma=1 in the quadratic computation. The equation f=tgf=tg gives h=−Q+O((a,z,t)3),Q=az+t(a+z).h=-Q+O((a,z,t)^3),\qquad Q=az+t(a+z). Since f=ah−Rf=ah-R, we can use H=⟨1,a,z,az,ah,K,L,f⟩.H=\langle1,a,z,az,ah,K,L,f\rangle. Its last four initial forms are, up to signs, aQ,tz(a+z),t(a+z)Q,t(a+z)aQ,tz(a+z),t(a+z)Q,t(a+z). Take the seven sections other than ff and tt times all eight. Their cubic terms are row-reduced using aQ−azt=a2(z+t),tz(a+z)−azt=z2t.aQ-azt=a^2(z+t),\qquad tz(a+z)-azt=z^2t. Their quartic terms are row-reduced using t(a+z)Q−taQ−t2z(a+z)=az2t.t(a+z)Q-taQ-t^2z(a+z)=az^2t. These are precisely the fifteen homogeneous forms stated above. No coefficient of the terms of gg beyond its linear part enters this calculation. ◻

Lemma 114.5. Let MM be the following fifteen vectors in coordinates (a,z,t)(a,z,t), indexed from 00 to 1414 in the indicated order: (0,0,0),(0,0,1),(0,1,0),(0,1,1),(0,2,1),(1,0,0),(1,0,1),(1,0,2),(1,1,0),(1,1,1),(1,1,2),(1,2,1),(2,1,0),(2,1,1),(2,1,2).\begin{aligned} &(0,0,0),(0,0,1),(0,1,0),(0,1,1),(0,2,1),\\ &(1,0,0),(1,0,1),(1,0,2),(1,1,0),(1,1,1),\\ &(1,1,2),(1,2,1),(2,1,0),(2,1,1),(2,1,2). \end{aligned} The semigroup generated by (1,q)(1,q), q∈Mq\in M, has 4m3+6m2+4m+14m^3+6m^2+4m+1 elements of degree mm. Its convex body has volume four and barycentre (8596,2732,4348).\left(\frac{85}{96},\frac{27}{32},\frac{43}{48}\right).

Proof. The convex hull is given by a,z,t≥0,t≤2,a+z≤3,a−z≤1,z−t≤1,t−a≤1,z+t≤3.a,z,t\ge0,\quad t\le2,\quad a+z\le3,\quad a-z\le1, \quad z-t\le1,\quad t-a\le1,\quad z+t\le3. The point indexed 99 is interior. Cone from this point over the following twenty-four boundary triangles: (0,1,2)(0,1,6)(0,2,8)(0,5,6)(0,5,8)(1,2,3)(1,3,10)(1,6,7)(1,7,10)(2,3,4)(2,4,8)(3,4,10)(4,8,11)(4,10,11)(5,6,12)(5,8,12)(6,7,13)(6,12,13)(7,10,14)(7,13,14)(8,11,12)(10,11,14)(11,12,13)(11,13,14).\begin{array}{rrrr} (0,1,2)&(0,1,6)&(0,2,8)&(0,5,6)\\ (0,5,8)&(1,2,3)&(1,3,10)&(1,6,7)\\ (1,7,10)&(2,3,4)&(2,4,8)&(3,4,10)\\ (4,8,11)&(4,10,11)&(5,6,12)&(5,8,12)\\ (6,7,13)&(6,12,13)&(7,10,14)&(7,13,14)\\ (8,11,12)&(10,11,14)&(11,12,13)&(11,13,14). \end{array} On each facet the listed triangles form its triangulation. Every cone has determinant of absolute value one. This is therefore a unimodular triangulation, with face numbers 15,50,60,2415,50,60,24. As in Lemma 114.2, relative-interior counting and the integer decomposition property give 15+50(m−1)+60(m−12)+24(m−13)=4m3+6m2+4m+1.15+50(m-1)+60\binom{m-1}{2}+24\binom{m-1}{3} =4m^3+6m^2+4m+1. Averaging the barycentres of the twenty-four equal-volume tetrahedra gives the asserted vector. ◻

Proposition 114.6. At the point pp of Lemma 114.4, δp(X)≥4843>1.\delta_p(X)\ge\frac{48}{43}>1. If ρ≠0\rho\ne0, the stronger bound 48/4148/41 holds.

Proof. The first case has already been identified with the algebra of Lemma 114.3. In the second case, refine the ordinary homogeneous initial forms by taking the least exponent of tt, then the least exponent of zz. Their initial monomials are 1,a,z,t,az,at,zt,a2z,z2t,azt,at2,a2zt,az2t,azt2,a2zt2.1,a,z,t,az,at,zt,a^2z,z^2t,azt,at^2, a^2zt,az^2t,azt^2,a^2zt^2. These are exactly the points of Lemma 114.5. The fifteen distinct initial monomials and their products therefore exhaust the full associated graded section space in every degree, by its exact Hilbert count. The barycentre gives, for the ordinary exceptional plane GG, SX(G)=8596+2732+4348=218.S_X(G)=\frac{85}{96}+\frac{27}{32}+\frac{43}{48}=\frac{21}{8}. For every fixed mm the refinement on its primary pieces is induced by an integral diagonal one-parameter subgroup: use weights (0,1,N)(0,1,N) in (a,z,t)(a,z,t) with NN larger than all exponents occurring in degree mm. Choose bases compatible with this filtration and any prescribed valuation filtration, and degenerate to their initial monomials. The limiting basis divisor is supported on the three coordinate lines of GG, whose limiting coefficients are the three barycentre coordinates above. They form a simple normal crossing divisor. The largest coefficient is 43/4843/48. The same two-filtration and semicontinuity argument as in Lemma 114.3 proves δ(G;WG)≥48/43.\delta(G;W^G)\ge48/43. Finally Abban–Zhuang adjunction gives δp(X)≥min{3/(21/8),48/43}=48/43.\delta_p(X)\ge\min\{3/(21/8),48/43\}=48/43. Again no Zariski decomposition on the point blow-up is required. ◻