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Section 9

The E6 point

We retain the global section ring and the two filtration identifications from Section 8, now with the E6E_6 weights. In particular, Lemmas 8.9 and 8.10 already give SX(GE)=177/16S_X(G_E)=177/16 and S(W;B)=11/16S(W;B)=11/16.

9.1 The exceptional surface and its tangent curve

Lemma 9.1. The weighted blow-up is of plt type, AX(GE)=13A_X(G_E)=13, and its coarse exceptional surface is GE=ℙ(1,1,2)G_E=\mathbb P(1,1,2) with coordinates U=xU=x, V=z2V=z^2, W=y3W=y^3. For HG=𝒪GE(1)H_G=\mathcal O_{G_E}(1) one has −GE|GE=16HG,ΔG=12(V=0)+23(W=0),B=(U2+UV+W=0)∼2HG.-G_E|_{G_E}=\tfrac16H_G,\quad \Delta_G=\tfrac12(V=0)+\tfrac23(W=0),\quad B=(U^2+UV+W=0)\sim2H_G. Moreover, α(GE,ΔG;HG)=1/2\alpha(G_E,\Delta_G;H_G)=1/2.

Proof. Lemma 8.12 applies with weights (6,4,3)(6,4,3) and gives discrepancy 6+4+3=136+4+3=13. A monomial of weight divisible by six has exponent of yy divisible by three and exponent of zz divisible by two. Thus the sixth Veronese is ℂ[x,z2,y3]\mathbb C[x,z^2,y^3] with regraded weights (1,1,2)(1,1,2); it gives the coarse surface and the normal class HG/6H_G/6.

The generic quotient indices are two along z=0z=0 and three along y=0y=0, and one along x=0x=0. They give the stated different. The equation of BB follows from the initial relation. As a check, −(KGE+ΔG)=13HG/6=13(−GE|GE)-(K_{G_E}+\Delta_G)=13H_G/6=13(-G_E|_{G_E}). Finally, Lemma 3.2 gives min{1,1/2,2/3}=1/2\min\{1,1/2,2/3\}=1/2. ◻

Lemma 9.2. The curve BB is a smooth rational curve avoiding the singular vertex of GEG_E. It is parametrized by [U:V][U:V], with W=−U(U+V)W=-U(U+V). Let QU,QU+V,QVQ_U,Q_{U+V},Q_V denote its points U=0U=0, U+V=0U+V=0, V=0V=0. Then (GE,ΔG+B)(G_E,\Delta_G+B) is plt along BB and ΔB=23QU+23QU+V+12QV.\Delta_B=\tfrac23Q_U+\tfrac23Q_{U+V}+\tfrac12Q_V.

Proof. At the vertex [0:0:1][0:0:1], the equation of BB is nonzero. Away from that point it solves for WW and gives the claimed isomorphism with ℙ1\mathbb P^1. The three marked points are distinct. The boundary (W=0)(W=0) cuts out QU+QU+VQ_U+Q_{U+V} transversely, and (V=0)(V=0) cuts out QVQ_V transversely. Thus near BB the pair is a smooth surface with a smooth coefficient-one curve and transverse boundary curves of coefficients less than one. It is plt, and ordinary adjunction gives the different. ◻

Lemma 9.3 (Residual degree in type E6E_6). The residual-degree average is RE=15/32R_E=15/32.

Proof. The class of a section of Wm,jW_{m,j} is jHG/6jH_G/6, and removal of BqB^q subtracts 2qHG2qH_G. Therefore RE=16SX(GE)−2S(W;B)=17796−2⋅1116=1532.R_E=\tfrac16S_X(G_E)-2S(W;B) =\frac{177}{96}-2\cdot\frac{11}{16}=\frac{15}{32}. ◻

9.2 The exact curve series and its averages

Lemma 9.4 (Finite-degree series in type E6E_6). Fix m,qm,q and set M=min{m,2m−q}M=\min\{m,2m-q\}. Every standard monomial is uniquely written yϵzηUiVjbq,0≤ϵ≤2,0≤η≤1,i+j=n.y^\epsilon z^\eta U^iV^j b^q,\qquad 0\le\epsilon\le2,\quad0\le\eta\le1,\quad i+j=n. Its native weight is 6n+4ϵ+3η+12q6n+4\epsilon+3\eta+12q. Put T=M−ϵ−ηT=M-\epsilon-\eta. After removing bqb^q and the residue factor yϵzηy^\epsilon z^\eta, its weight summand restricts to (9.1)⟨Un−jVj:0≤j≤ℓ⟩=Un−ℓH0(ℙ1,𝒪(ℓ)),ℓ=min{n,T−n},0≤n≤T.\label{f25:eq:E-series} \langle U^{n-j}V^j:0\le j\le\ell\rangle =U^{n-\ell}H^0(\mathbb P^1,\mathcal O(\ell)),\qquad \ell=\min\{n,T-n\},\quad0\le n\le T. It is empty if T<0T<0. For a nonempty summand the dimension is ℓ+1\ell+1, and its mean point orders, with the residue factor restored, are QQUQU+VQVother pointsmeann−ℓ/2+ϵ/3ℓ/2+ϵ/3ℓ/2+η/2ℓ/2.\begin{array}{c|cccc} Q&Q_U&Q_{U+V}&Q_V&\text{other points}\\\hline \text{mean}&n-\ell/2+\epsilon/3&\ell/2+\epsilon/3&\ell/2+\eta/2&\ell/2. \end{array} The residual divisor class on GEG_E is (n+2ϵ/3+η/2)HG(n+2\epsilon/3+\eta/2)H_G.

Proof. The standard-monomial condition is that the exponent of yy is at most two; splitting the exponent of zz into its parity and its even part gives the unique expression. The six residues 4ϵ+3η4\epsilon+3\eta are distinct modulo six. Thus ϵ,η\epsilon,\eta are fixed in each summand of given native weight and given qq.

The ordinary-degree inequality from Lemma 8.4 is i+2j≤M−ϵ−η=Ti+2j\le M-\epsilon-\eta=T. Since i+j=ni+j=n, it is equivalent to 0≤j≤min{n,T−n}0\le j\le\min\{n,T-n\}. This proves (9.1). Its fixed part is (n−ℓ)QU(n-\ell)Q_U, and the remaining series is complete. Lemma 3.1 gives the means before restoring the residue factor. Using Lemma 2.14 and y3=W=−U(U+V)y^3=W=-U(U+V), z2=Vz^2=V, that factor contributes ϵ/3\epsilon/3 at QU,QU+VQ_U,Q_{U+V} and η/2\eta/2 at QVQ_V. Its class is (2ϵ/3+η/2)HG(2\epsilon/3+\eta/2)H_G, proving the last assertion. The fixed degree plus the moving degree is (n−ℓ)+2ϵ/3+η/2+ℓ=n+2ϵ/3+η/2(n-\ell)+2\epsilon/3+\eta/2+\ell=n+2\epsilon/3+\eta/2, as required by deg(HG|B)=1\deg(H_G|_B)=1. ◻

Example 9.5. Take m=5m=5, q=0q=0, ϵ=η=0\epsilon=\eta=0, n=3n=3. Then T=5T=5 and ℓ=2\ell=2. The space is ⟨U3,U2V,UV2⟩=UH0(ℙ1,𝒪(2))\langle U^3,U^2V,UV^2\rangle=U H^0(\mathbb P^1,\mathcal O(2)). Its three orders at QUQ_U are 1,2,31,2,3, with mean two. At any other point an adapted basis has orders 0,1,20,1,2, with mean one. Thus the extra vanishing at QUQ_U comes from the explicit fixed factor, rather than from a separate decomposition on the threefold.

Lemma 9.6 (Positivity in type E6E_6). The two refined series have bounded support and contain ample series, so both inequalities of Proposition 2.7 apply.

Proof. Use the native weight JJ and put M=min{m,2m−q}M=\min\{m,2m-q\}. Here the second support cone is (9.2)𝒞E={(m,J,q):m≥0,0≤q≤2m,12q≤J≤12q+6M}.\label{f25:eq:E-support} \mathcal C_E=\{(m,J,q):m\ge0,\ 0\le q\le2m,\ 12q\le J\le12q+6M\}. Containment follows from the standard monomials. To prove equality and eventual nonvanishing, take an integral interior point (m0,J0,q0)(m_0,J_0,q_0) and write M0=min{m0,2m0−q0}M_0=\min\{m_0,2m_0-q_0\}. For each kk, choose the unique pair 0≤ϵk≤20\le\epsilon_k\le2, 0≤ηk≤10\le\eta_k\le1 such that 4ϵk+3ηk≡kJ0(mod6)4\epsilon_k+3\eta_k\equiv kJ_0\pmod6. Set nk=kJ0−12kq0−4ϵk−3ηk6,Tk=kM0−ϵk−ηk.n_k=\frac{kJ_0-12kq_0-4\epsilon_k-3\eta_k}{6},\qquad T_k=kM_0-\epsilon_k-\eta_k. The strict inequalities 0<J0−12q0<6M00<J_0-12q_0<6M_0 imply that nkn_k and Tk−nkT_k-n_k both grow linearly. Hence the interval in Lemma 9.4 is nonempty for every sufficiently large kk. Density of rational interior rays proves (9.2).

The first support cone is its projection 0≤J≤24m0\le J\le24m. For any interior ray in this projection, choose q0q_0 just below J0/12J_0/12 to lift it to an interior ray of (9.2), and approximate kq0kq_0 by integers. The bounded rounding and residue errors preserve eventual nonvanishing, just as above. Thus both series have bounded support with nonempty interior and are eventually nonzero on every integral interior ray.

For an ample subseries on GEG_E, take (m,J)=(12k,12k)(m,J)=(12k,12k). Every weighted polynomial of weight 12k12k has ordinary degree at most 4k≤m4k\le m and is a global initial form. These constitute H0(GE,𝒪GE(2k))H^0(G_E,\mathcal O_{G_E}(2k)), where 2HG2H_G is ample Cartier. For the curve, take (m,J,q)=(12k,24k,k)(m,J,q)=(12k,24k,k); then ϵ=η=0\epsilon=\eta=0, n=ℓ=2kn=\ell=2k, and the series is exactly H0(B,𝒪B(2k))H^0(B,\mathcal O_B(2k)). Both rays are interior. Together with the plt assertions in Lemmas 9.1 and 9.2, this verifies all the hypotheses of Proposition 2.7. ◻

Lemma 9.7 (Limiting point orders in type E6E_6). One has S(WB;QU)=5/16S(W^B;Q_U)=5/16 and S(WB;Q)=5/32S(W^B;Q)=5/32 for every Q≠QUQ\ne Q_U.

Proof. Rescale q,nq,n by mm and set M(q)=min{1,2−q}M(q)=\min\{1,2-q\}. The limiting dimension function is ℓ(n,q)=min{n,M(q)−n}\ell(n,q)=\min\{n,M(q)-n\} for 0≤n≤M(q)0\le n\le M(q). The normalizing integral is IE=∫02∫0M(q)ℓdndq=14∫02M(q)2dq=13.I_E=\int_0^2\int_0^{M(q)}\ell\,dn\,dq =\frac14\int_0^2M(q)^2dq=\frac13. There are six residue classes, so the total dimension is 6IEm3+O(m2)=2m3+O(m2)6I_Em^3+O(m^2)=2m^3+O(m^2). The common factor six cancels in normalized means. The limiting mean order is n−ℓ/2n-\ell/2 at QUQ_U and ℓ/2\ell/2 at every other point. Splitting the inner integrals at n=M/2n=M/2 gives ∫0Mnℓdn=M38,∫0Mℓ(n−ℓ2)dn=M312,∫0Mℓ22dn=M324.\int_0^M n\ell\,dn=\frac{M^3}{8},\qquad \int_0^M\ell\left(n-\frac\ell2\right)dn=\frac{M^3}{12},\qquad \int_0^M\frac{\ell^2}{2}\,dn=\frac{M^3}{24}. For example, the middle integral is ∫0M/2n2/2dn+∫M/2M(M−n)(3n−M)/2dn=M3/12\int_0^{M/2}n^2/2\,dn+\int_{M/2}^M(M-n)(3n-M)/2\,dn=M^3/12. Multiplying the last two values by ∫02M(q)3dq=5/4\int_0^2M(q)^3dq=5/4 and dividing by IE=1/3I_E=1/3 gives 5/165/16 and 5/325/32. The first gives the residual average 15/3215/32, agreeing with Lemma 9.3. Similarly, S(W;B)=IE−114∫02qM(q)2dq=11/16S(W;B)=I_E^{-1}\frac14\int_0^2qM(q)^2dq=11/16.

All residue corrections in Lemma 9.4 are bounded, uniformly in QQ. Their total contribution is O(m3)O(m^3) by the same dimension estimate as in the proof of Lemma 8.20, so they disappear after division by mNmmN_m. ◻

9.3 The E6 estimate

Lemma 9.8. One has δ(GE,ΔG;W)≥16/15\delta(G_E,\Delta_G;W)\ge16/15.

Proof. For centres not contained in BB, the residual-degree estimate and Lemmas 9.1 and 9.3 give S(W;v)≤2(15/32)AGE,ΔG(v)=(15/16)AGE,ΔG(v)S(W;v)\le2(15/32)A_{G_E,\Delta_G}(v)=(15/16)A_{G_E,\Delta_G}(v). For centres on BB, apply the second refinement using Lemma 9.6. The curve term is 16/1116/11, and the point terms are QAB,ΔB(Q)S(WB;Q)AB,ΔB(Q)/S(WB;Q)QU1/35/1616/15QU+V1/35/3232/15QV1/25/3216/5other points15/3232/5.\begin{array}{c|c|c|c} Q&A_{B,\Delta_B}(Q)&S(W^B;Q)&A_{B,\Delta_B}(Q)/S(W^B;Q)\\\hline Q_U&1/3&5/16&16/15\\ Q_{U+V}&1/3&5/32&32/15\\ Q_V&1/2&5/32&16/5\\ \text{other points}&1&5/32&32/5. \end{array} The smallest bound is 16/1516/15, which proves the assertion for every divisorial valuation on the surface. ◻

Proof of Theorem 7.3. The first refinement, Lemma 9.8, and the separate calculation of SX(GE)S_X(G_E) give δP(X)≥min{13177/16,1615}=min{208177,1615}=1615.\delta_P(X)\ge\min\left\{\frac{13}{177/16},\frac{16}{15}\right\} =\min\left\{\frac{208}{177},\frac{16}{15}\right\}=\frac{16}{15}. ◻

Remark 9.9. The two independent routes to the first expected vanishing agree: 2(95/96)+8(11/16)=359/482(95/96)+8(11/16)=359/48 and 6(15/32)+12(11/16)=177/166(15/32)+12(11/16)=177/16. The left sides use the curve-series distributions; Lemma 8.9 uses only the weighted Hilbert function and the weight of the relation. This agreement checks the normalization of the native valuations against that of the coarse exceptional surfaces. Throughout both proofs, all new expected vanishing orders and fixed factors were obtained from actual graded section spaces, without a Zariski decomposition on the weighted threefold blow-ups.

Proof of Theorem 1.1 for Family 2.5. Suppose that XX is not K-stable and choose F,PF,P as in Lemma 7.1. Then δP(X)≤AX(F)/SX(F)≤1\delta_P(X)\le A_X(F)/S_X(F)\le1. This contradicts Theorem 7.2 or Theorem 7.3. ◻