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Section 27

The weighted extraction of a double fibre

Let f−1(y)=2Λf^{-1}(y)=2\Lambda. The construction of Lemma 18.1 applies to any smooth plane conic bundle and gives the normalized weighted extraction ω:X♯=Bl𝔪y𝒪XX→X.\omega:X^\sharp=\mathop{\mathrm{Bl}}_{\mathfrak m_y\mathcal O_X}X\longrightarrow X. Its exceptional divisor, denoted here by TT, is of plt type. We recall the geometric data to fix all conventions.

Lemma 27.1. The transverse weights are (1,2)(1,2), and T=Λ×ℙ1,AX(T)=3,ω*L|T=h,T|T=−fT/2,ΔT=D/2,T=\Lambda\times\mathbb P^1,\quad A_X(T)=3,\quad \omega^*L|_T=h,\quad T|_T=-f_T/2,\quad \Delta_T=D/2, where h=𝒪T(1,0)h=\mathcal O_T(1,0), fT=𝒪T(0,1)f_T=\mathcal O_T(0,1), and DD is a smooth (2,1)(2,1)-curve. The notation fTf_T denotes a divisor class, not the conic-bundle morphism. The curve DD is the graph of a degree-two map Λ→ℙ1\Lambda\to\mathbb P^1.

Proof. In a local trivialization of the plane bundle, the equation has the form x2+η1Q1(s0,s1)+η2Q2(s0,s1)+x^2+\eta_1Q_1(s_0,s_1)+\eta_2Q_2(s_0,s_1)+ higher weighted-order terms, with weights 1,2,21,2,2. The quadrics Q1,Q2Q_1,Q_2 have no common zero, by smoothness of XX. Locally the base ideal is (x2,η2)(x^2,\eta_2). Its blow-up has charts η2=x2r\eta_2=x^2r and x2=η2rx^2=\eta_2r; the latter has an A1A_1 singularity transverse to the singular-locus curve. Flat base change from Blyℙ2\mathop{\mathrm{Bl}}_y\mathbb P^2 shows that the reduced exceptional surface is the product, and that the pullback of the exceptional base curve is 2T2T. The singular-locus curve is D=(η1Q1+η2Q2=0)D=(\eta_1Q_1+\eta_2Q_2=0), giving the different D/2D/2. The Jacobian on the first chart gives discrepancy three. Finally LΛ=1L\Lambda=1, since LL has degree two on the conic fibre. This proves all the formulas, including the case Λ⊂E\Lambda\subset E. ◻

There are two different section filtrations: Λ⊄E\Lambda\not\subset E and Λ⊂E\Lambda\subset E. The second must not be omitted. An example appears below.

Lemma 27.2 (Identifying the two filtrations). Choose y=[1:0:0]y=[1:0:0]. If Λ⊄E\Lambda\not\subset E, coordinates in (23.1) can be chosen so that its initial equation for ordT\mathop{\mathrm{ord}}_T is G0=x0u2+x1Q1(v,ex0)+x2Q2(v,ex0),G_0=x_0u^2+x_1Q_1(v,ex_0)+x_2Q_2(v,ex_0), with weights 11 on uu, 22 on x1,x2x_1,x_2, and zero on v,e,x0v,e,x_0. If Λ⊂E\Lambda\subset E, its initial equation is G0=e2x03+x1Q1(u,v)+x2Q2(u,v),G_0=e^2x_0^3+x_1Q_1(u,v)+x_2Q_2(u,v), with weights 11 on ee, 22 on x1,x2x_1,x_2, and zero on u,v,x0u,v,x_0. In either case Q1,Q2Q_1,Q_2 are relatively prime binary quadrics. The actual associated graded anticanonical section spaces are the bidegree (m,m)(m,m) pieces of the polynomial ring modulo G0G_0, for m≥2m\ge2.

Proof. On the plane over yy, the rank-one quadratic is the square of a linear form in u,v,ex0u,v,ex_0. If its line is different from e=0e=0, a linear change in u,vu,v, followed by addition of a multiple of ex0ex_0, makes this form uu. If its line is e=0e=0, normalize its nonzero coefficient to one. Taking initial terms gives the two equations. The two binary quadrics are the first base derivatives on Λ\Lambda, so they have no common zero by smoothness of the total space.

For completeness, the section ring calculation is global. On the plane bundle Y→ℙ2Y\to\mathbb P^2, the pushforward of 𝒪Y(pH+qB)\mathcal O_Y(pH+qB) for p≥0p\ge0 is ⨁a=0p𝒪ℙ2(q+a)⊕(p−a+1).\bigoplus_{a=0}^p\mathcal O_{\mathbb P^2}(q+a)^{\oplus(p-a+1)}. Thus H1(Y,(m−2)H+(m−1)B)=0H^1(Y,(m-2)H+(m-1)B)=0. Restriction from YY to the hypersurface of class 2H+B2H+B identifies H0(X,mL)H^0(X,mL) with the bidegree (m,m)(m,m) quotient by GG.

The weighted hypersurface filtration has associated graded quotient by G0G_0. This is the one-equation case of Lemma 5.1. Each displayed G0G_0 is a primitive linear polynomial in x1,x2x_1,x_2 over the ring of the other variables and is irreducible; the coprimality of the binary quadrics ensures primitivity. Hence this quotient is a domain, and it injects into its localization at x0x_0 and a nonzero homogeneous coordinate on Λ\Lambda. On that chart the weighted normal equation is precisely the local equation in Lemma 27.1. Its associated graded ring is the geometric one. The two inverted weight-zero coordinates have bidegrees forming a lattice basis. In any fixed bidegree, their common Laurent factor is therefore uniquely determined, and removing it preserves injectivity. The injectivity criterion in Lemma 5.1 now proves equality of the global quotient and geometric filtrations. In particular, no unaccounted cancellation is used to assign a section its order. ◻

Lemma 27.3 (The two expected vanishing orders). One has SX(T)={169/72,Λ⊄E,91/36,Λ⊂E.S_X(T)= \begin{cases} 169/72,&\Lambda\not\subset E,\\ 91/36,&\Lambda\subset E. \end{cases} Thus AX(T)−SX(T)A_X(T)-S_X(T) is respectively 47/7247/72 and 17/3617/36.

Proof. We give a separate Hilbert calculation. For the polynomial Cox ring, let P(p,q)P(p,q) be the dimension of degree pH+qBpH+qB, with p,q≥0p,q\ge0. A monomial has ee-exponent aa, total u,vu,v-degree p−ap-a, and total xx-degree q+aq+a. Therefore P(p,q)=∑a=0p(p−a+1)(q+a+22).P(p,q)=\sum_{a=0}^p(p-a+1)\binom{q+a+2}{2}. For d=q+ad=q+a, the sum of the x1,x2x_1,x_2 weights over all degree-dd base monomials is 2d(d+1)(d+2)/32d(d+1)(d+2)/3. In the first case, the additional weight sum of the u,vu,v monomials is (p−a)(p−a+1)/2(p-a)(p-a+1)/2. In the second case, each has the additional weight aa. Consequently the polynomial weight sums are U(p,q)=∑a=0p[(p−a)(p−a+1)2(d+22)+(p−a+1)2d(d+1)(d+2)3],V(p,q)=∑a=0p(p−a+1)[a(d+22)+2d(d+1)(d+2)3].\begin{split} U(p,q)&=\sum_{a=0}^p\left[\frac{(p-a)(p-a+1)}2\binom{d+2}{2} +(p-a+1)\frac{2d(d+1)(d+2)}3\right],\\ V(p,q)&=\sum_{a=0}^p(p-a+1)\left[a\binom{d+2}{2} +\frac{2d(d+1)(d+2)}3\right]. \end{split} The relation has bidegree (2,1)(2,1) and weight two. Subtract its multiples, including their additional weight two. The quotient dimension is Nm=P(m,m)−P(m−2,m−1)=(2m+1)(3m2+3m+2)2.N_m=P(m,m)-P(m-2,m-1)=\frac{(2m+1)(3m^2+3m+2)}2. The two quotient weight sums are, respectively, U(m,m)−U(m−2,m−1)−2P(m−2,m−1)=m(169m3+230m2+191m+58)24,V(m,m)−V(m−2,m−1)−2P(m−2,m−1)=m(91m3+128m2+107m+34)12.\begin{split} U(m,m)-U(m-2,m-1)-2P(m-2,m-1) &=\frac{m(169m^3+230m^2+191m+58)}{24},\\ V(m,m)-V(m-2,m-1)-2P(m-2,m-1) &=\frac{m(91m^3+128m^2+107m+34)}{12}. \end{split} Divide by mNmmN_m and take the limit. Lemma 27.2 identifies these algebraic weights with the geometric valuation, so Lemma 2.1 applies. ◻

No Zariski decomposition on X♯X^\sharp is used in this calculation. The argument instead proves equality of the geometric filtration with a weighted hypersurface filtration, and then counts its sections. Computing only (ω*L−tT)3(\omega^*L-tT)^3 would not suffice: this divisor is visibly nef for 0≤t≤20\le t\le2, where its volume is 18−3t2/218-3t^2/2, but the contribution of that interval to SX(T)S_X(T) is only 16/916/9. Both values in Lemma 27.3 are larger.