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Section 56

Completion for Family 2.16

Proposition 56.1 (Every point of a double fibre). If p∈Λp\in\Lambda and g−1(g(p))=2Λg^{-1}(g(p))=2\Lambda, then δp(X)≥88/85\delta_p(X)\ge88/85.

Proof. Apply Abban–Zhuang to the plt curve extraction of Lemma 54.2. The refined threshold over any point of Λ\Lambda is bounded below by the global surface threshold. Lemmas 55.1 and 55.4 give δp(X)≥min{357/22,8885}=8885.\delta_p(X)\ge \min\left\{\frac{3}{57/22},\frac{88}{85}\right\} =\frac{88}{85}. To recall the local argument, choose a threefold basis compatible with FF and a given prime divisor over XX, and write its pull-back as Sm(F)F+ΓmS_m(F)F+\Gamma_m. The finite-level bounds in the proof of Lemma 55.4 make (F,D/2+λΓm|F)(F,D/2+\lambda\Gamma_m|_F) log canonical for every fixed λ<88/85\lambda<88/85 and large mm. Inversion of adjunction gives log canonicity of (X♯,F+λΓm)(X^\sharp,F+\lambda\Gamma_m) near FF. The pull-back boundary for the original basis divisor has coefficient 1−AX(F)+λSm(F)≤11-A_X(F)+\lambda S_m(F)\le1 on FF, so it too is log canonical there. By properness, the centre on X♯X^\sharp of any divisor whose centre on XX contains pp meets ω−1(p)\omega^{-1}(p). This proves the required inequality for all such divisors. Passing to the limit gives the stated bound. Bounded support, the ample-series condition, and the different were verified above. The estimate includes p=q=Λ∩Ep=q=\Lambda\cap E. ◻

Proof of Theorem 53.1 and the Family 2.16 assertion of Theorem 1.1. Every plane conic fibre is smooth, reduced with two components, or a double line. Proposition 53.3 and Proposition 56.1 therefore give δp(X)≥min{176/171,88/85}=176/171\delta_p(X)\ge\min\{176/171,88/85\}=176/171 for every point pp. For any prime divisor VV over XX, choose a point of its centre. The definition of δp\delta_p gives AX(V)/SX(V)≥176/171A_X(V)/S_X(V)\ge176/171. Taking the infimum proves the global bound, and hence K-stability. ◻

Example 56.2 (A smooth member with a double fibre). In coordinates [s:x:z:t0:t1:t2][s:x:z:t_0:t_1:t_2] on ℙ5\mathbb P^5, take Q1=zt0−st1−xt2,Q2=x2+sz+t0t2+t12+t22,V=(Q1=Q2=0).Q_1=z t_0-s t_1-x t_2, \qquad Q_2=x^2+s z+t_0t_2+t_1^2+t_2^2, \qquad V=(Q_1=Q_2=0). The determinant of the Hessian matrix of Q1+λQ2Q_1+\lambda Q_2 is 4λ6+4λ2−14\lambda^6+4\lambda^2-1. It has six distinct roots and its leading coefficient is nonzero. Simultaneous diagonalization therefore gives six distinct pencil eigenvalues, which proves that the intersection of the quadrics is smooth. The plane t0=t1=t2=0t_0=t_1=t_2=0 cuts out the smooth conic x2+sz=0x^2+s z=0. Blow it up. Over [y0:u:v]=[1:0:0][y_0:u:v]=[1:0:0], the strict transform equations are z=0z=0 and x2=0x^2=0, giving a double line. For its leading model, R=su,T=tv,q=s2u+t2v,P=([1:0],[0:1]).R=su,\qquad T=tv,\qquad q=s^2u+t^2v, \qquad P=([1:0],[0:1]). Here PP is a ramification point of D→ℙ[u:v]1D\to\mathbb P^1_{[u:v]}. Thus the limiting monomial calculation already occurs on the actual exceptional surface. The branch valuation has expected order 85/4485/44 and discrepancy two for (F,D/2)(F,D/2), so the refined surface threshold is exactly 88/8588/85 in this example. In particular, smoothness of XX does not rule out the fibres treated in this part.

Remark 56.3 (Avoiding a Zariski decomposition on the extracted threefold). We have not computed a Zariski decomposition of ω*L−tF\omega^*L-tF on the weighted threefold extraction. The volume integrals in Lemma 53.2 take place on XX itself. For the new extraction, the prime initial algebra in Lemma 54.3 identifies the actual section filtration, and Lemma 54.4 proves completeness of its point-ideal spaces. Their dimensions compute SX(F)S_X(F) exactly. The surface estimate then uses a degeneration preserving the different and explicit order sums. These statements provide the required vanishing information; no unproved decomposition on X♯X^\sharp is substituted for them.