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Section 49

Points of type A2A_2

Lemma 49.1. Let pp be an A2A_2 point of a fibre. There are regular parameters z,x,yz,x,y at pp, of extraction weights 2,3,32,3,3, such that the leading forms of a basis of H0(V,H)H^0(V,H) are 1,z,x,y,z2,zx,xy−z3,1,z,x,y,z^2,zx,xy-z^3, and the last form defines the fibre. These forms generate the full weighted initial section algebra. More precisely, with homogeneous variables h,z,x,y,P,Q,Rh,z,x,y,P,Q,R, it is given by (49.1)hP=z2,hQ=zx,hR=xy−zP,zQ=xP,yQ=zR+P2.\label{f214:eq:A2-ring} hP=z^2,\quad hQ=zx,\quad hR=xy-zP,\quad zQ=xP,\quad yQ=zR+P^2. The initial Cox algebra of XX is obtained by substituting h=aeh=ae and R=beR=be, where a,b,ea,b,e have degrees F,F,H−FF,F,H-F and weights 0,6,00,6,0.

Proof. The tangent conic of the fibre is reduced, with two components. Its vertex rr is not in the scheme ZZ of Lemma 43.3. Indeed, a point of ZZ is the tangent direction of a line on VV through pp. Every hyperplane section singular at pp contains that line, so its cubic part vanishes in this direction. At an A2A_2 point the cubic part is nonzero on the radical of the quadratic part, which gives a contradiction.

Thus ZZ is contained in the two components away from their intersection. Since ZZ is noncollinear, its lengths on these components are two and one. Let x=0x=0 be the component carrying length two, and let y=0y=0 be the other component. The quadrics containing ZZ and divisible by xx form a pencil. It contains xyxy and a quadric xℓx\ell, where ℓ(r)≠0\ell(r)\ne0: the residual linear forms are precisely the lines through the length-one point on y=0y=0. Complete x,yx,y by a linear coordinate zz nonzero at rr. The two remaining normal hyperplane coordinates can therefore be chosen to have weighted leading forms xzxz and z2z^2. For the second assertion use that some quadric of the net is nonzero at rr, since r∉Zr\notin Z.

The fibre has local equation xy+γz3xy+\gamma z^3 plus terms of weight greater than six, with γ≠0\gamma\ne0. Rescaling the coordinates gives xy−z3xy-z^3. Together with the three linear coordinates and the constant section, this proves the claimed list of leading forms.

We verify that no further leading generators have been missed. The relations in (49.1) are the five maximal Pfaffians of the skew-symmetric matrix (0hxz0−h0Pyz−x−P0RQ−z−y−R0P0−z−Q−P0),\begin{pmatrix} 0&h&x&z&0\\ -h&0&P&y&z\\ -x&-P&0&R&Q\\ -z&-y&-R&0&P\\ 0&-z&-Q&-P&0 \end{pmatrix}, with the following signs. Deleting rows and columns 1,…,51,\ldots,5 in order gives P2−yQ+zR,xP−zQ,hP−z2,hQ−xz,hR−xy+zP.P^2-yQ+zR,\quad xP-zQ,\quad hP-z^2,\quad hQ-xz, \quad hR-xy+zP. Thus its maximal Pfaffians generate precisely the displayed ideal. After inverting hh they give a polynomial algebra in h±1,z,x,yh^{\pm1},z,x,y. On h=0h=0 the reduced equations are z=0z=0, xy=xP=0xy=xP=0, and yQ=P2yQ=P^2; both components have dimension three. Thus the ideal has height three and its Pfaffian resolution is Cohen–Macaulay. No component is contained in h=0h=0, so the algebra is a domain. Its ordinary Hilbert series is (1+3t+t2)/(1−t)4(1+3t+t^2)/(1-t)^4, the Hilbert series of VV.

The algebra generated by the displayed leading forms embeds in the associated graded section algebra. Since both have the same ordinary Hilbert function, they are equal. This dimension argument checks all possible cancellations, not only quadratic relations.

For the Cox algebra, the same argument applies after h=ae,R=beh=ae,R=be. The boundary h=R=0h=R=0 in (49.1) has dimension two; therefore the boundary e=0e=0 after substitution has dimension four. The complementary open set has dimension five and is a domain. The height-three Pfaffian resolution proves Cohen–Macaulayness. The dimension-two common zero locus says exactly that h,Rh,R form a regular sequence. Lemma 43.1 now identifies the substituted algebra with the full initial global section algebra and proves its primeness. ◻

49.1 The weighted extraction at a point of type A2A_2

We use the local normal form established in the geometric lemma: after choosing parameters z,x,yz,x,y of weights 2,3,32,3,3, respectively, the initial forms of the seven hyperplane sections span ℋ=⟨1,z,x,y,z2,zx,B⟩,B=xy−z3.\mathcal H=\langle1,z,x,y,z^2,zx,B\rangle, \qquad B=xy-z^3. The initial form of the singular pencil member is BB. This normal form holds on both point orbits on which a normal hyperplane section can have an A2A_2 singularity; no assumption on the other pencil member is needed besides its being nonzero at the point.

Lemma 49.1 identifies the entire initial algebra. Its anticanonical degree-mm piece has dimension Nm=(2m+1)(5m2+5m+3)/3.N_m=(2m+1)(5m^2+5m+3)/3.

Lemma 49.2. Let GG be the exceptional divisor of the weighted blowup with weights (2,3,3)(2,3,3) at an A2A_2 point. Then AX(G)=8,SX(G)=538,δ(G,ΔG;W)≥1615.A_X(G)=8,\qquad S_X(G)=\frac{53}{8},\qquad \delta(G,\Delta_G;W)\ge\frac{16}{15}.

Proof. The exceptional divisor is ℙ(2,3,3)\mathbb P(2,3,3). Its coarse space is ℙ(1,1,2)\mathbb P(1,1,2) with coordinates x,y,t=z3x,y,t=z^3, and ΔG=23{t=0}\Delta_G=\frac23\{t=0\}. The discrepancy is the sum 2+3+3=82+3+3=8.

In each native-degree piece take the lowest zz-power, refining it by any fixed monomial order. The leading term of BB is xyxy. The thirteen distinct degree-one leading monomials are 1,z,x,y,z2,zx,xy,zxy,x2y,xy2,z2xy,zx2y,x2y2.1,z,x,y,z^2,zx,xy,zxy,x^2y,xy^2,z^2xy,zx^2y,x^2y^2. They form a basis of the degree-one space. Their exponent vectors, with coordinates ordered as (z,x,y)(z,x,y), generate the full degree-prefixed lattice: the monomials 1,z,x,y1,z,x,y already suffice. Their convex hull has vertices (0,0,0),(0,0,1),(0,1,0),(0,1,2),(0,2,1),(0,2,2),(1,1,0),(1,2,1),(2,0,0),(2,1,1).\begin{gathered} (0,0,0),(0,0,1),(0,1,0),(0,1,2),(0,2,1),(0,2,2),\ (1,1,0),(1,2,1),(2,0,0),(2,1,1). \end{gathered} Its volume and first moment are, respectively, 103,(5524,258,6524).\frac{10}{3},\qquad \left(\frac{55}{24},\frac{25}{8},\frac{65}{24}\right). For an explicit description, this polytope is cut out by α,β,γ≥0\alpha,\beta,\gamma\ge0 and β−γ≤1,β≤2,α−2β+2γ≤2,α+2γ≤4,α+β−γ≤2,α+β+γ≤4.\begin{gathered} \beta-\gamma\le1,\quad\beta\le2,\quad \alpha-2\beta+2\gamma\le2,\quad\alpha+2\gamma\le4,\ \alpha+\beta-\gamma\le2,\qquad \alpha+\beta+\gamma\le4. \end{gathered} Triangulating its boundary and using the determinant formula gives the stated volume and moment. Since the volume is the leading coefficient of NmN_m, the semigroup-volume lemma shows that the actual asymptotic pivot means for the full refined spaces are μz=1116,μx=1516,μy=1316.\mu_z=\frac{11}{16},\qquad \mu_x=\frac{15}{16},\qquad \mu_y=\frac{13}{16}. The native weighted degree is 2α+3β+3γ2\alpha+3\beta+3\gamma. Thus this also computes the expected vanishing of the primary extraction directly: SX(G)=2μz+3μx+3μy=53/8S_X(G)=2\mu_z+3\mu_x+3\mu_y=53/8.

We spell out the log-canonicity step because the exceptional weighted projective space is not well formed. In a fixed finite degree, choose a one-parameter subgroup which realizes the chosen monomial order on all monomials occurring in that degree. In every native-degree piece choose a basis simultaneously adapted to this weight filtration and an arbitrary divisorial valuation over GG. Its limit basis consists of the pivot monomials. On the coarse surface the limiting basis divisor therefore has asymptotic coefficients 1148{t=0}+1516{x=0}+1316{y=0}.\frac{11}{48}\{t=0\} +\frac{15}{16}\{x=0\} +\frac{13}{16}\{y=0\}. Together with the different 23{t=0}\frac23\{t=0\}, this toric boundary is log canonical after multiplication of the basis divisor by any c<16/15c<16/15: the three coefficient conditions are 23+c1148≤1\frac23+c\frac{11}{48}\le1, c1516≤1c\frac{15}{16}\le1 and c1316≤1c\frac{13}{16}\le1. They can also be checked on the index-two cover at the vertex of ℙ(1,1,2)\mathbb P(1,1,2); elsewhere the toric boundary has simple normal crossings. Log-canonical-threshold semicontinuity and the simultaneous basis construction give the same bound for the original valuation. Passing to the asymptotic threshold and then letting cc increase to 16/1516/15 proves the assertion. ◻

Corollary 49.3. At every singular point of a fibre of type A2A_2 one has δp(X)≥16/15>1\delta_p(X)\ge16/15>1.

Proof. Abban–Zhuang gives δp(X)≥min{8/(53/8),16/15}=16/15\delta_p(X)\ge\min\{8/(53/8),16/15\}=16/15. ◻

Example 49.4. The binomial B=xy−z3B=xy-z^3 has native weight six, although it is a single hyperplane section before passing to initial forms. The section BzxBzx has native weight eleven, and its leading monomial is zx2yzx^2y. Both lie in anticanonical degree one. These examples explain why the native weight and the anticanonical degree must be kept separate in the preceding computation. The full-volume check is what certifies that products of the displayed sections account for the leading asymptotic dimension, including all possible cancellations.