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Section 105

The weighted extraction and its actual section ring

Write a double conic as 2ℓ2\ell. We use the normalized blow-up of its fibre ideal, rather than the ordinary blow-up of its support. The latter has exceptional surface 𝔽3\mathbb F_3, since Nℓ/X=𝒪ℙ1(1)⊕𝒪ℙ1(−2)N_{\ell/X}=\mathcal O_{\mathbb P^1}(1)\oplus \mathcal O_{\mathbb P^1}(-2). Indeed, the derivative of the conic equation along its double line gives a surjection 𝒪(1)⊕𝒪⊕2→𝒪(2)\mathcal O(1)\oplus\mathcal O^{\oplus2}\to\mathcal O(2). It vanishes on 𝒪(1)\mathcal O(1), and the other two entries are relatively prime binary quadratics, so the kernel is as stated. In the weighted construction below the exceptional pair is a product of two projective lines with a smooth boundary. Put EC=EE_C=E and EΛ=RE_\Lambda=R in this section.

Lemma 105.1. Let XX be the blowup of ℙ3\mathbb P^3 along a smooth complete intersection C={q0=q1=0}C=\{q_0=q_1=0\} of two quadrics and a line Λ\Lambda disjoint from CC. Put A=H−EΛA=H-E_\Lambda and B=2H−ECB=2H-E_C. Suppose that a fibre of the conic bundle η=(|A|,|B|):X→ℙ1×ℙ1\eta=(|A|,|B|):X\to\mathbb P^1\times\mathbb P^1 is 2ℓ2\ell. There are homogeneous coordinates [r:s:z:w][r:s:z:w] on ℙ3\mathbb P^3 such that Λ={s=w=0},π(ℓ)={z=w=0},q0=z2+w(c0r+c1s+c2z+c3w),\Lambda=\{s=w=0\},\qquad \pi(\ell)=\{z=w=0\},\qquad q_0=z^2+w(c_0r+c_1s+c_2z+c_3w), where (c0,c1)≠(0,0)(c_0,c_1)\ne(0,0). If f(r,s)=s(c0r+c1s),g(r,s)=q1(r,s,0,0),f(r,s)=s(c_0r+c_1s),\qquad g(r,s)=q_1(r,s,0,0), then ff and gg have no common zero on ℙ1\mathbb P^1. In particular, g(1,0)≠0g(1,0)\ne0. On a neighbourhood of the whole curve ℓ\ell, the threefold is given in ℙ[r:s:z]2×𝔸a,b2\mathbb P^2_{[r:s:z]}\times\mathbb A^2_{a,b} by an equation whose terms of smallest weight, for wt(z)=1\operatorname{wt}(z)=1 and wt(a)=wt(b)=2\operatorname{wt}(a)=\operatorname{wt}(b)=2, are z2+af(r,s)+bg(r,s).z^2+af(r,s)+bg(r,s).

Proof. The plane corresponding to the first coordinate of η(ℓ)\eta(\ell) contains Λ\Lambda, and its intersection with the corresponding quadric is the double line 2π(ℓ)2\pi(\ell). The quadric cannot be smooth, since a tangent plane section of a smooth quadric is a pair of distinct lines. Every singular member of the pencil through a smooth elliptic quartic is a rank-three quadric. Choose the plane w=0w=0 and its double line z=w=0z=w=0; the displayed form follows. The rank-three condition is precisely (c0,c1)≠(0,0)(c_0,c_1)\ne(0,0). The zeroes of ff are the point Λ∩π(ℓ)=[1:0:0:0]\Lambda\cap\pi(\ell)=[1:0:0:0] and the vertex of q0=0q_0=0, counted with multiplicity. The first point does not belong to CC. The vertex does not belong to CC either, since otherwise the complete intersection {q0=q1=0}\{q_0=q_1=0\} would be singular. Thus ff and gg are relatively prime.

In the chart of the pencil of planes through Λ\Lambda with w=asw=as, the blowup of Λ\Lambda is a trivial ℙ2\mathbb P^2-bundle with fibre coordinates [r:s:z][r:s:z]. The second pencil has local equation q0+bq1=0q_0+bq_1=0. Substitution gives z2+as(c0r+c1s+c2z+c3as)+bq1(r,s,z,as)=0.z^2+as(c_0r+c_1s+c_2z+c_3as)+bq_1(r,s,z,as)=0. This equation contains the whole strict transform of π(ℓ)\pi(\ell) and has the stated initial form. The use of the blowup chart is essential at Λ∩π(ℓ)\Lambda\cap\pi(\ell): the coordinate aa remains regular there. ◻

Lemma 105.2. In the notation of Lemma 105.1, let σ:Y→X\sigma:Y\to X be the normalized blowup of the ideal (a,b)(a,b), and let GG be its reduced exceptional divisor. Then σ\sigma is the weighted blowup of ℓ\ell with transverse weights (1,2)(1,2), and AX(G)=3,G≅ℙ1×ℙ1,(KY+G)|G=KG+12D,A_X(G)=3,\qquad G\cong\mathbb P^1\times\mathbb P^1,\qquad (K_Y+G)|_G=K_G+\frac12D, where D={Uf(r,s)+Vg(r,s)=0}⊂ℙ[r:s]1×ℙ[U:V]1D=\{Uf(r,s)+Vg(r,s)=0\}\subset \mathbb P^1_{[r:s]}\times\mathbb P^1_{[U:V]} is a smooth curve of bidegree (2,1)(2,1). The pair (Y,G)(Y,G) is purely log terminal.

Proof. At every point of ℓ\ell at least one of ff and gg is nonzero. If g≠0g\ne0, the equation of XX allows us to eliminate bb, and (a,b)=(a,z2)(a,b)=(a,z^2) in the local ring. If f≠0f\ne0, the same argument, with aa eliminated, gives (a,b)=(b,z2)(a,b)=(b,z^2); this equality follows as well from the implicit function theorem, or from the completed local ring. The normalized blowup of (a,z2)(a,z^2) is the weighted blowup with ordG(z)=1\operatorname{ord}_G(z)=1 and ordG(a)=2\operatorname{ord}_G(a)=2. Its log discrepancy is 1+2=31+2=3.

The exceptional divisor is the relative weighted hypersurface Z2+Uf(r,s)+Vg(r,s)=0Z^2+Uf(r,s)+Vg(r,s)=0 with weights (1,2,2)(1,2,2) in [Z:U:V][Z:U:V]. The projection to [U:V][U:V] identifies its coarse space with ℙ[r:s]1×ℙ[U:V]1\mathbb P^1_{[r:s]}\times\mathbb P^1_{[U:V]}: indeed, the second Veronese replaces ZZ by T=Z2T=Z^2, and the equation eliminates TT. Here ZZ has degree one along the first factor, so that TT, UfUf and VgVg have the same degree. Along Z=0Z=0 the transverse weighted chart has stabilizer of order two. It follows either by adjunction on the index cover, or directly from the cyclic quotient chart of the (1,2)(1,2)-weighted blowup, that the different is D/2D/2. There is no other divisorial stabilizer. Since ff and gg are relatively prime, DD is the graph of the morphism [r:s]↦[−g(r,s):f(r,s)][r:s]\mapsto[-g(r,s):f(r,s)]; it is smooth and has bidegree (2,1)(2,1). The local weighted blowup of a smooth codimension-two centre with coprime transverse weights is purely log terminal. This also follows here from the quotient charts and the smoothness of DD. ◻

Remark 105.3. If c0=0c_0=0, the line Λ\Lambda passes through the vertex of the singular quadric. The quadric fibre of |B||B| is then nonnormal. For example, blowing up {y=z=0}\{y=z=0\} in the quadric x2−yz=0x^2-yz=0 gives, in the chart y=tzy=tz, the surface x2−tz2=0x^2-tz^2=0, singular along x=z=0x=z=0. Thus a proof using only sextic del Pezzo surfaces with Du Val singularities would omit these smooth threefolds. The weighted extraction above applies without alteration: in this case ff is a square, while ff and gg remain relatively prime and DD remains smooth.

Lemma 105.4. Let T=BlΛ(ℙ3)×ℙ1T=\operatorname{Bl}_\Lambda(\mathbb P^3)\times\mathbb P^1, so that X⊂TX\subset T has class 2H+B2H+B. Write the Cox coordinates of TT as r,z,s,a0,a1,b0,b1r,z,s,a_0,a_1,b_0,b_1, of respective divisor classes H,H,H−A,A,A,B,B.H,H,H-A,A,A,B,B. Assign these coordinates weights 0,1,0,0,2,0,20,1,0,0,2,0,2. Then the initial equation of XX is F0=b0z2+b0a1s(c0r+c1a0s)+b1g(r,a0s).F_0=b_0z^2+b_0a_1s(c_0r+c_1a_0s)+b_1g(r,a_0s). This equation is irreducible. The induced weight filtration on H0(X,−mKX)H^0(X,-mK_X) is the filtration defined by GG.

Proof. The initial equation follows from the normal form above, after homogenizing ss by a0a_0. Regard F0F_0 as a polynomial of degree one in a1a_1. Its coefficient is b0s(c0r+c1a0s)b_0s(c_0r+c_1a_0s), and its constant term is b0z2+b1g(r,a0s)b_0z^2+b_1g(r,a_0s). These polynomials are relatively prime: no factor of s(c0r+c1a0s)s(c_0r+c_1a_0s) divides the term b0z2b_0z^2, and b0b_0 does not divide b1gb_1g. In the case c0=0c_0=0 the extra factor a0a_0 also does not divide the constant term. Gauss’s lemma proves irreducibility.

For m≥1m\ge1 the restriction sequence for X⊂TX\subset T is exact on sections in degree m(H+A+B)m(H+A+B). Indeed, after subtracting 2H+B2H+B the relative degree is m−2m-2. For m=1m=1 the relative line bundle 𝒪ℙ2(−1)\mathcal O_{\mathbb P^2}(-1) is acyclic; for m≥2m\ge2 the pushforward is a direct sum of line bundles with nonnegative degrees on both base factors. Thus the relevant section spaces are the homogeneous pieces of the Cox ring modulo the equation of XX.

Taking the initial form of a principal ideal gives the ideal (F0)(F_0). As its quotient is a domain, localization in a coordinate chart meeting ℓ\ell is injective. In that chart the same filtration is the (1,2)(1,2)-weight filtration just computed on the transverse parameters. Consequently a nonzero initial section cannot disappear after restriction to the weighted normal cone. This identifies the global weight filtration with ordG\operatorname{ord}_G, including all possible cancellations between sections. ◻

Lemma 105.5 (The weighted curve moment). For the extraction of Lemma 105.2, the weights on the product-graph coordinates are (H0,H1,H2,H3)=(0,0,1,2),(U0,U1)=(V0,V1)=(0,2).(H_0,H_1,H_2,H_3)=(0,0,1,2),\qquad (U_0,U_1)=(V_0,V_1)=(0,2). Its two equations have degrees (2,1,0)(2,1,0) and (1,0,1)(1,0,1) and both have weight 22. One has SX(G)=24388.S_X(G)=\frac{243}{88}.

Proof. The initial product graph is the same variety as the initial Cox hypersurface in Lemma 105.4. Indeed, its plane-graph equation is homogeneous for these weights. Its two base centres are {z2+w(c0r+c1s)=g(r,s)=0},{s=w=0}.\{z^2+w(c_0r+c_1s)=g(r,s)=0\},\qquad \{s=w=0\}. They are disjoint because g(1,0)≠0g(1,0)\ne0, and the first is a complete intersection. Thus the initial product graph is their integral blow-up graph, with the displayed regular sequence of two equations. This also verifies directly the integrality needed in the Koszul calculation. Write hm=h0(X,−mKX)h_m=h^0(X,-mK_X) and let TmT_m be the sum of the weights. The Koszul resolution gives hm=(m+33)(m+1)2−((m+13)+(m+23))m(m+1)+(m3)m2=(2m+1)(11m2+11m+6)6.\begin{aligned} h_m&={m+3\choose3}(m+1)^2- \left({m+1\choose3}+{m+2\choose3}\right)m(m+1) +{m\choose3}m^2\\ &=\frac{(2m+1)(11m^2+11m+6)}6. \end{aligned} The average weight in H0(ℙ3×ℙ1×ℙ1,𝒪(a,b,c))H^0(\mathbb P^3\times\mathbb P^1\times\mathbb P^1, \mathcal O(a,b,c)) is 3a/4+b+c3a/4+b+c. Put Nf=(m+13)m(m+1),Ng=(m+23)m(m+1),Nfg=(m3)m2.N_f={m+1\choose3}m(m+1),\qquad N_g={m+2\choose3}m(m+1),\qquad N_{fg}={m\choose3}m^2. The shifts by the two equations therefore give Tm=11m4hm+12Nf−14Ng−14Nfg=m(81m3+118m2+83m+22)8.T_m=\frac{11m}{4}h_m+\frac12N_f-\frac14N_g-\frac14N_{fg} =\frac{m(81m^3+118m^2+83m+22)}8. Taking the limit of Tm/(mhm)T_m/(mh_m) proves the assertion. Integrality of the initial graph ensures that these are the actual valuation weights. ◻

Definition 105.6. For the exceptional divisor GG, let Vm≥j={s∈H0(X,−mKX):ordG(s)≥j},Wm,j=Vm≥j/Vm≥j+1.V_m^{\ge j}=\{s\in H^0(X,-mK_X):\operatorname{ord}_G(s)\ge j\}, \qquad W_{m,j}=V_m^{\ge j}/V_m^{\ge j+1}. These are the actual refined spaces on GG. Put hm=h0(X,−mKX)h_m=h^0(X,-mK_X). Their level-mm basis boundaries are normalized by mhmmh_m, summing over all jj and a basis in each Wm,jW_{m,j}. The different is D/2D/2, so throughout the surface calculation δ(G,D/2;W)=infFAG,D/2(F)S(W;F).\delta(G,D/2;W)=\inf_F\frac{A_{G,D/2}(F)}{S(W;F)}. For an odd weight the factor zz denotes a rational section whose square cuts out DD; its contribution to a basis boundary is D/2D/2. This convention retains the different, which is an additional fixed boundary independent of mm. More precisely, if aG,bGa_G,b_G denote the two ruling classes, the weight-jj space has rational divisor class maG+(j/2)bGma_G+(j/2)b_G. Writing j=2n+εj=2n+\varepsilon, its polynomial part has class (m−ε)aG+nbG(m-\varepsilon)a_G+nb_G, and its fixed half-divisor is εD/2\varepsilon D/2.

Lemma 105.7. On the chart a0=b0=1a_0=b_0=1, the direct sum of the actual spaces at level mm is spanned, modulo z2+af+bg=0z^2+af+bg=0, by rizjskaαbβ,i+j+k=m,0≤α≤m+k,0≤β≤m.r^i z^j s^k a^\alpha b^\beta, \qquad i+j+k=m,\quad0\le\alpha\le m+k,\quad0\le\beta\le m. The primary weight is j+2α+2βj+2\alpha+2\beta. All primary weights between zero and 6m6m occur, and Wm,2mW_{m,2m} contains the complete ample series H0(G,𝒪G(m,m))H^0(G,\mathcal O_G(m,m)). Thus the bounded-support and ample-series hypotheses of Abban–Zhuang theory hold.

Proof. The Cox degrees in Lemma 105.4 give exactly these inequalities after setting a0=b0=1a_0=b_0=1. The same lemma proves that their span is the actual associated graded space. Its largest primary weight is 6m6m. Every intermediate integral weight occurs, by taking products of the degree-one generators of weights 0,1,2,3,4,5,60,1,2,3,4,5,6. Taking j=0j=0, i+k=mi+k=m, and α+β=m\alpha+\beta=m gives all monomials of bidegree (m,m)(m,m) on GG. The ray (m,2m)(m,2m) is interior to the support, and 𝒪G(1,1)\mathcal O_G(1,1) is ample. ◻

Example 105.8. For m=1m=1, the even pieces, after the square relation is used, have dimensions 2,4,3,12,4,3,1 in weights 0,2,4,60,2,4,6. The odd pieces have dimensions 1,2,11,2,1 in weights 1,3,51,3,5. Their total is 1414, and their weighted sum is 3838. Thus the first-level expected order is 19/719/7; its limit, computed above, is 243/88243/88.