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Section 103

Geometry and the statement for Family 3.6

Family 3.6: double conics and weighted curve extractions

Let C⊂ℙ3C\subset\mathbb P^3 be a smooth elliptic quartic, let Λ⊂ℙ3\Lambda\subset\mathbb P^3 be a line disjoint from CC, and let π:X→ℙ3\pi:X\to\mathbb P^3 blow up C⊔ΛC\sqcup\Lambda. These are exactly the smooth members of Family 3.6. Write E,RE,R for the exceptional divisors over C,ΛC,\Lambda, respectively, and put H=π*𝒪ℙ3(1),A=H−R,B=2H−E.H=\pi^*\mathcal O_{\mathbb P^3}(1),\qquad A=H-R,\qquad B=2H-E. The two pencils define morphisms σ:X→ℙ1\sigma:X\to\mathbb P^1 and ϕ:X→ℙ1\phi:X\to\mathbb P^1. Their general fibres are del Pezzo surfaces of degrees five and six, respectively. The product η=(σ,ϕ)\eta=(\sigma,\phi) is a conic bundle over ℙ1×ℙ1\mathbb P^1\times\mathbb P^1. We prove the following assertion.

Theorem 103.1. Every smooth Fano threefold in Family 3.6 is K-stable.

Cheltsov proved this when every conic fibre is reduced [42, Theorem 1]. The omitted configurations are quintic fibres with two A1A_1 points or one A3A_3 point. We first reduce possible nonpositive-beta centres to their double conics. We then blow up the scheme-theoretic conic fibre. The resulting exceptional surface has a nonzero different, which is retained in every subsequent estimate.

Lemma 103.2. Write C=(q0=q1=0)C=(q_0=q_1=0) and Λ=(l0=l1=0)\Lambda=(l_0=l_1=0). The variety XX is the complete intersection u0q1−u1q0=0,v0l1−v1l0=0u_0q_1-u_1q_0=0,\qquad v_0l_1-v_1l_0=0 in ℙ3×ℙ1×ℙ1\mathbb P^3\times\mathbb P^1\times\mathbb P^1, of classes 2H+B2H+B and H+AH+A. In particular, −KX=H+A+B=4H−E−R,(−KX)3=22.-K_X=H+A+B=4H-E-R,\qquad (-K_X)^3=22. Every quintic fibre is normal and has only Du Val singularities. Its possible singularity types are A1,A2,2A1,A3A_1,A_2,2A_1,A_3.

Proof. Each equation is the graph of a pencil whose base ideal is a regular sequence. Since the two centres are disjoint, the product of the two graphs is their simultaneous blow-up. Adjunction gives the asserted anticanonical class. The nonzero intersection numbers needed below are H3=1,HE2=−4,E3=−16,HR2=−1,R3=−2;H^3=1,\quad HE^2=-4,\quad E^3=-16,\quad HR^2=-1,\quad R^3=-2; also H2E=H2R=ER=0H^2E=H^2R=ER=0. They give the degree 2222.

A plane through Λ\Lambda cuts out on the smooth curve CC a curvilinear scheme of length four. On that plane the fibre is the blow-up of the scheme. A length-kk part has local ideal (y,xk)(y,x^k); one chart of its blow-up has equation yt=xky t=x^k and gives an Ak−1A_{k-1} singularity. The partitions of four give the stated list. The pencil of restricted quadrics supplies a conic bundle on each such fibre. The partitions (2,2)(2,2) and (4)(4) give a double conic, as described explicitly below. ◻

Lemma 103.3 (The two fibre moments). For a fibre S∈|A|S\in|A| and a fibre T∈|B|T\in|B|, SX(S)=6788,SX(T)=109176.S_X(S)=\frac{67}{88},\qquad S_X(T)=\frac{109}{176}. More precisely, the positive and negative parts of −KX−uS-K_X-uS are uP(u)N(u)P(u)3[0,1](4−u)H−E+(u−1)R022−15u[1,2](4−u)H−E(u−1)R(4−u)3−12(4−u)+16,\begin{array}{c|c|c|c} u&P(u)&N(u)&P(u)^3\\ \hline {[0,1]}&(4-u)H-E+(u-1)R&0&22-15u\\ {[1,2]}&(4-u)H-E&(u-1)R&(4-u)^3-12(4-u)+16, \end{array} and those of −KX−uT-K_X-uT are uP(u)N(u)P(u)3[0,1](4−2u)H+(u−1)E−R022−18u[1,3/2](4−2u)H−R(u−1)E(4−2u)3−3(4−2u)+2.\begin{array}{c|c|c|c} u&P(u)&N(u)&P(u)^3\\ \hline {[0,1]}&(4-2u)H+(u-1)E-R&0&22-18u\\ {[1,3/2]}&(4-2u)H-R&(u-1)E&(4-2u)^3-3(4-2u)+2. \end{array} The pseudoeffective thresholds are 22 and 3/23/2, respectively.

Proof. The nef classes H,A,BH,A,B express the positive parts in the displayed intervals. For example, in the second interval of the first table, P(u)=(2−u)H+BP(u)=(2-u)H+B; in that of the second table, P(u)=(3−2u)H+AP(u)=(3-2u)H+A. Intersection with the fibres of R→ΛR\to\Lambda or E→CE\to C forces the indicated fixed part when u>1u>1. The effective cone is generated by E,R,A,BE,R,A,B [42, Section 2]; it gives the two thresholds. The intersection numbers in Lemma 103.2 give the cubics in the tables. Thus, explicitly, 22SX(S)=∫01(22−15u)du+∫12((4−u)3−12(4−u)+16)du=674,22SX(T)=∫01(22−18u)du+∫13/2((4−2u)3−3(4−2u)+2)du=1098.\begin{aligned} 22S_X(S)&=\int_0^1(22-15u)\,du+ \int_1^2\big((4-u)^3-12(4-u)+16\big)\,du=\frac{67}{4},\\ 22S_X(T)&=\int_0^1(22-18u)\,du+ \int_1^{3/2}\big((4-2u)^3-3(4-2u)+2\big)\,du=\frac{109}{8}. \end{aligned} ◻

Lemma 103.4 (Previously established local estimates). The following estimates hold for the actual fibre refinements.

  1. If S∈|A|S\in|A| is smooth, then δp(S;WS)>1\delta_p(S;W^S)>1 for every p∈Sp\in S.

  2. If S∈|A|S\in|A| has just one singularity, of type A1A_1 or A2A_2, then δp(S;WS)>1\delta_p(S;W^S)>1 away from the conic fibre through that singularity.

  3. If T∈|B|T\in|B| is smooth, then δp(T;WT)≥1\delta_p(T;W^T)\ge1. The inequality is strict unless p∈Ep\in E and pp lies on a (−1)(-1)-curve of TT.

Every prime divisor whose centre on XX is a surface has positive beta.

Proof. The three estimates are [42, Corollaries 2–4]; they are local statements about the indicated fibre and do not assume that other fibres of XX are reduced. The divisorial assertion is the divisorial-stability calculation recalled in [42, Section 2]. ◻