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Section 51

The point of type A4A_4

We prove the following local estimate.

Theorem 51.1. If pp is an A4A_4 singular point of a fibre, then δp(X)≥320/307\delta_p(X)\ge320/307.

51.1 The actual section filtration

We use the standard equations of V5V_5, written as (51.1)vw−x0P+u2=0,vR−uQ+P2=0,v2−x0Q+uP=0,uv−x0R−Pw=0,Pv−Qw−uR=0.\label{f214:eq:V5A4} \begin{gathered} vw-x_0P+u^2=0,\qquad vR-uQ+P^2=0,\qquad v^2-x_0Q+uP=0,\\ uv-x_0R-Pw=0,\qquad Pv-Qw-uR=0. \end{gathered} At the point [x0:u:P:Q:v:w:R]=[1:0:0:0:0:0:0][x_0:u:P:Q:v:w:R]=[1:0:0:0:0:0:0], the affine coordinates u,v,wu,v,w give (51.2)P=u2+vw,Q=u3+uvw+v2,R=uv−u2w−vw2.\label{f214:eq:A4polys} P=u^2+vw,\qquad Q=u^3+uvw+v^2,\qquad R=uv-u^2w-vw^2. The orbit and tangent-hyperplane calculation identifies an A4A_4 fibre with a hyperplane R+γQ=0R+\gamma Q=0 at this point. Its other pencil coordinate is a linear form ℓ\ell nonzero at the point; after rescaling, ℓ=x0+\ell=x_0+ terms vanishing at the point. Put x=u−w2,y=v−uw−w3,z=w.x=u-w^2,\qquad y=v-uw-w^3,\qquad z=w. Then R=xy−z5R=xy-z^5. We extract the divisor GG with weights (2,3,1)(2,3,1) in u,v,wu,v,w. The same weights in x,y,zx,y,z show that this is the usual weighted extraction for this A4A_4 equation. Its exceptional surface is G=ℙ(2,3,1)G=\mathbb P(2,3,1), its different is zero, and AX(G)=6A_X(G)=6. Put M=𝒪G(1)M=\mathcal O_G(1); thus M2=1/6M^2=1/6.

Lemma 51.2. The actual point-refined series on GG is the series of native-weight components of Vm=⟨P1⋯PhRq:Pi∈{u,P,Q,v,w},h≤m,h+q≤2m⟩,V_m=\left\langle P_1\cdots P_hR^q:\ P_i\in\{u,P,Q,v,w\},\ h\le m,\ h+q\le2m\right\rangle, where the polynomials are those of (51.2). Here 11 is allowed by taking h=q=0h=q=0, and the native weights of (u,P,Q,v,w,R)(u,P,Q,v,w,R) are (2,4,6,3,1,5)(2,4,6,3,1,5). Moreover Nm=dimVm=(2m+1)(5m2+5m+3)3.N_m=\dim V_m=\frac{(2m+1)(5m^2+5m+3)}3.

Proof. Use the global section graph of Lemma 43.1, with variables a,b,ea,b,e of divisor degrees H−E,H−E,EH-E,H-E,E, respectively. For its candidate initial algebra replace x0,Rx_0,R in (51.1) by ae,beae,be, and denote the resulting ring by ℛ\mathcal R. On the open set ae≠0ae\ne0 its five equations are the polynomial graph (51.2). The locus e=0e=0 is the affine cone over V5∩{x0=R=0}V_5\cap\{x_0=R=0\}, with the two free variables a,ba,b; it has dimension four. The locus a=0,e≠0a=0,e\ne0 also has dimension four. The Pfaffian ideal therefore has codimension three. Its Pfaffian resolution makes the quotient Cohen–Macaulay, and the boundary has smaller dimension than the open graph. Thus ℛ\mathcal R is a domain.

Give a,ea,e weight zero and bb weight five. The five Pfaffians have weights 4,8,6,5,74,8,6,5,7. Replacing x0x_0 by ℓ\ell and RR by R+γQR+\gamma Q changes these equations only by terms of larger weight. The initial Pfaffian ring has the same bigraded Hilbert series as the original Cox presentation, by their codimension-three Pfaffian resolutions. Hence it is the entire associated graded ring. Localization at aeae is injective on it and on each divisor-degree component; it consequently gives the geometric point filtration, including all cancellations.

A Cox monomial of degree mLmL with hh factors among the five HH variables and exponent qq in bb has exponents 2m−h−q2m-h-q in aa and m−hm-h in ee. This gives exactly the two displayed inequalities. After setting a=e=1a=e=1, the degree-one generators are {1,u,P,Q,v,w,R}∪R{1,u,P,Q,v,w,R}.\{1,u,P,Q,v,w,R\}\cup R\{1,u,P,Q,v,w,R\}. The repetition of RR leaves thirteen generators. Every allowed monomial factors into mm such generators: put at most one RR alongside each of its hh HH factors and at most two RR factors in each remaining slot. Finally Riemann–Roch, or the same Pfaffian resolution, gives the displayed formula for NmN_m. ◻

Lemma 51.3 (The first expected order). One has SX(G)=45/8S_X(G)=45/8.

Proof. Here is a separate Hilbert calculation. If sHs_H is the sum of the weights of the five HH variables, sab=wa+wbs_{ab}=w_a+w_b, and DD is the last syzygy weight, the Pfaffian resolution has weight numerator 1−∑i=15t2Hqdi+∑i=15t3HqD−di−t5HqD,∑di=2D.1-\sum_{i=1}^5t^{2H}q^{d_i} +\sum_{i=1}^5t^{3H}q^{D-d_i}-t^{5H}q^D, \qquad \sum d_i=2D. Differentiate with respect to qq and take the coefficient of degree mLmL. Expansion of the eight-variable geometric series gives ∑weights=524(5sH+11sab+6we−3D)m4+O(m3).\sum\text{weights} =\frac5{24}(5s_H+11s_{ab}+6w_e-3D)m^4+O(m^3). For clarity, the monomials before taking the Pfaffian alternating sum are counted by ∑h=ms(h+1)(s−h+44)\sum_{h=m}^{s}(h+1)\binom{s-h+4}{4} in divisor degree (s,−m)(s,-m); their weight sum is obtained by multiplying each summand by sH(s−h)/5+sabh/2+we(h−m)s_H(s-h)/5+s_{ab}h/2+w_e(h-m). Taking the shifts 0,2H,3H,5H0,2H,3H,5H, with the relation and syzygy weights above, gives the displayed leading coefficient. Since Nm=(10/3)m3+O(m2)N_m=(10/3)m^3+O(m^2), the normalized trace is 5sH+11sab+6we−3D16.\frac{5s_H+11s_{ab}+6w_e-3D}{16}. In our case (sH,sab,we,D)=(16,5,0,15)(s_H,s_{ab},w_e,D)=(16,5,0,15). More explicitly, the finite weight sum is 754m4+552m3+814m2+112m,\frac{75}{4}m^4+\frac{55}{2}m^3+\frac{81}{4}m^2+\frac{11}{2}m, whose quotient by mNmmN_m tends to 45/845/8. Lemma 51.2 identifies this trace with the actual expected order. ◻

51.2 Two computations on curves

Write B={R=0}⊂GB=\{R=0\}\subset G and Q0=[0:0:1]Q_0=[0:0:1]. The change to x,y,zx,y,z above identifies BB with {xy=z5}\{xy=z^5\}. Its coarse curve is ℙ1\mathbb P^1, and its different has coefficients 1/2,2/31/2,2/3 at its two points on z=0z=0. It is purely log terminal in GG. On w=1w=1, putting b=Rb=R gives v=u2+bu−1,P|B=u3u−1,Q|B=u5(u−1)2.v=\frac{u^2+b}{u-1},\qquad P\big|_B=\frac{u^3}{u-1},\qquad Q\big|_B=\frac{u^5}{(u-1)^2}. All denominators here are units at Q0Q_0.

Lemma 51.4. One has S(W;B)=1116,S(WB;Q0)=2516.S(W;B)=\frac{11}{16},\qquad S(W^B;Q_0)=\frac{25}{16}. At every other point q∈Bq\in B, one has S(WB;q)≤25/96S(W^B;q)\le25/96.

Proof. Record the successive orders (a,q,j)(a,q,j) in u,bu,b, and the native degree jj, taking the bb order first. The following degree-one sections give the vertices of a convex hull: section1wRwR2QRQ(a,q,j)(0,0,0)(0,0,1)(0,1,6)(0,2,10)(5,0,6)(5,1,11).\begin{array}{c|rrrrrr} \text{section}&1&w&Rw&R^2&Q&RQ\\\hline (a,q,j)&(0,0,0)&(0,0,1)&(0,1,6)&(0,2,10)&(5,0,6)&(5,1,11). \end{array} Multiplying by the common unit (u−1)2m(u-1)^{2m} in degree mm verifies these orders without changing either filtration. The hull has halfspaces a,q≥0,−a−5q+j≤1,−a−4q+j≤2,6a+25q−5j≤0.a,q\ge0,\quad -a-5q+j\le1,\quad -a-4q+j\le2, \quad 6a+25q-5j\le0. Its volume is 10/310/3 and its first moment is (125/24,55/24,75/4)(125/24,55/24,75/4). These numbers can be checked by coning to the origin the boundary triangles (1,4,0),(5,2,3),(2,1,0),(2,3,0),(5,3,0),(5,4,0),(5,2,1),(5,1,4),(1,4,0),(5,2,3),(2,1,0),(2,3,0), (5,3,0),(5,4,0),(5,2,1),(5,1,4), where the six vertices are numbered in the order of the table. The sections 1,w,u,R1,w,u,R show that, after adjoining the anticanonical degree, the generated lattice is ℤ4\mathbb Z^4. The full-volume lemma, Lemma 34.2, applies: the hull volume equals the leading coefficient of NmN_m. Thus the centroid (25/16,11/16,45/8)(25/16,11/16,45/8) gives the actual moments, proving the two equalities.

The total expected degree of the residual zero divisors on BB is B⋅M(SX(G)−5S(W;B))=56(458−5516)=17596.B\cdot M\left(S_X(G)-5S(W;B)\right) =\frac56\left(\frac{45}8-\frac{55}{16}\right)=\frac{175}{96}. In each graded piece choose a basis compatible with the orders at Q0Q_0 and qq. The sum of these two orders is at most the degree of each zero divisor. Hence S(WB;q)≤175/96−25/16=25/96S(W^B;q)\le175/96-25/16=25/96. ◻

Lemma 51.5. Blow up Q0∈GQ_0\in G with weights (1,2)(1,2) in the local coordinates u,vu,v, and denote the exceptional curve by KK. Then AG(K)=3,S(W;K)=4116,δ(K,Diff;WK)≥320307.A_G(K)=3,\qquad S(W;K)=\frac{41}{16},\qquad \delta(K,\operatorname{Diff};W^K)\ge\frac{320}{307}.

Proof. The curve is K=ℙ(1,2)K=\mathbb P(1,2), with different 12[0:1]\frac12[0:1]. Put y=v+u2y=v+u^2 on the chart w=1w=1, and let P0∈KP_0\in K be y=0y=0. Order a monomial uaybu^ay^b by (a+2b,b)(a+2b,b). Keeping native degree jj as the third record gives the actual flag K⊃P0K\supset P_0.

Here are all additional leading terms needed for a full-volume certificate. The first thirteen sections have anticanonical degree one, and the last two have degree two: section(a,b,j)section(a,b,j)1(0,0,0)w(0,0,1)P(0,1,4)−R(0,1,5)−Rw(0,1,6)−PR(0,2,9)R2(0,2,10)u(1,0,2)Q(1,1,6)−Ru(1,1,7)−RQ(1,2,11)−v(2,0,3)Rv(2,1,8)Q2−PRv(0,3,12)R(PRv−Q2)(0,4,17)\begin{array}{c|cc|c} \text{section}&(a,b,j)&\text{section}&(a,b,j)\\\hline 1&(0,0,0)&w&(0,0,1)\\ P&(0,1,4)&-R&(0,1,5)\\ -Rw&(0,1,6)&-PR&(0,2,9)\\ R^2&(0,2,10)&u&(1,0,2)\\ Q&(1,1,6)&-Ru&(1,1,7)\\ -RQ&(1,2,11)&-v&(2,0,3)\\ Rv&(2,1,8)&Q^2-PRv&(0,3,12)\\ R(PRv-Q^2)&(0,4,17)&& \end{array} For example the KK-initial forms of P,Q,RP,Q,R are y,uy,−yy,uy,-y, respectively; those of the last two sections are y3,y4y^3,y^4. These identities follow by direct substitution of (51.2); thus the table includes genuine cancellation sections, not a guessed initial presentation.

The convex hull of the degree-normalized vectors has nine vertices i012345678a000012200b00122103/22j016101183617/2.\begin{array}{c|rrrrrrrrr} i&0&1&2&3&4&5&6&7&8\\\hline a&0&0&0&0&1&2&2&0&0\\ b&0&0&1&2&2&1&0&3/2&2\\ j&0&1&6&10&11&8&3&6&17/2. \end{array} Its halfspaces are a,b≥0,b≤2,−a−5b+j≤1,−a−4b+j≤2,3a+8b−2j≤0,5a+11b−2j≤5,9a+20b−4j≤6.\begin{gathered} a,b\ge0,\quad b\le2,\quad -a-5b+j\le1,\quad -a-4b+j\le2,\\ 3a+8b-2j\le0,\quad5a+11b-2j\le5,\quad9a+20b-4j\le6. \end{gathered} For an explicit integration certificate, cone to the origin its boundary triangles (6,7,0),(8,4,5),(8,4,3),(1,6,0),(2,4,5),(2,4,3),(8,6,7),(8,6,5),(1,8,7),(1,7,0),(1,2,3),(1,8,3),(1,2,5),(1,6,5).\begin{gathered} (6,7,0),(8,4,5),(8,4,3),(1,6,0),(2,4,5),(2,4,3),\\ (8,6,7),(8,6,5),(1,8,7),(1,7,0),(1,2,3),(1,8,3), (1,2,5),(1,6,5). \end{gathered} The determinant formula gives volume 10/310/3 and first moment (103/48,307/96,75/4)(103/48,307/96,75/4). The lattice is already generated by 1,w,u,P1,w,u,P, with anticanonical degree prepended. Lemma 34.2 therefore gives the exact centroid (μa,μb,μj)=(103160,307320,458).(\mu_a,\mu_b,\mu_j)=\left(\frac{103}{160},\frac{307}{320},\frac{45}8\right). In particular S(W;K)=μa+2μb=41/16S(W;K)=\mu_a+2\mu_b=41/16 and S(WK;P0)=307/320S(W^K;P_0)=307/320.

The total expected degree on KK is 12S(W;K)=41/32\frac12S(W;K)=41/32. Simultaneous bases at P0P_0 and any other point give expected order at most 41/32−307/320=103/32041/32-307/320=103/320 at the latter. The discrepancy there is at least 1/21/2, while P0P_0 has discrepancy one. Thus the refined threshold is at least min{320/307,160/103}=320/307\min\{320/307,160/103\}=320/307. ◻

Example 51.6. The two degree-two cancellation sections in Lemma 51.5 are essential. A computation using only the displayed Pfaffian weights for the final point filtration gives the incorrect number 15/1615/16 at P0P_0. The actual value is 307/320307/320. The full-volume certificate is what rules out further changes to this value from unrecorded cancellations.

51.3 The complement of the tangent curve

The following elementary observation is useful here because a direct alpha-invariant estimate on G\BG\setminus B is too weak.

Lemma 51.7 (Retaining zeros away from the point). Let T≠BT\ne B be a prime curve on GG, with T∼dMT\sim dM, and let p∈T\Bp\in T\setminus B. Suppose that TT is smooth at pp and that (G,T)(G,T) is purely log terminal there with zero different at pp. Then the point term of the refinement by TT satisfies S(WT;p)≤d6(3516−dS(W;T)).S(W^T;p)\le\frac d6\left(\frac{35}{16}-dS(W;T)\right).

Proof. In each piece of the TT-associated graded series put the filtration induced by the subspaces divisible by RqR^q. Taking associated graded for the TT filtration preserves the dimensions of each of these subspaces. Consequently the sum of their induced RR weights is precisely the original BB weight. Choose a basis of this graded piece compatible with both the induced RR filtration and the point-order filtration at pp, and lift it with the indicated TT and RR orders. Since T≠BT\ne B, the TT-initial form of a section divisible by RqR^q is divisible by (R|T)q(R|_T)^q. All these zeros lie away from pp.

The expected degree of the zero divisors on TT before removing these zeros is M⋅T(SX(G)−dS(W;T))M\cdot T\,(S_X(G)-dS(W;T)). Their expected degree on B∩TB\cap T is at least B⋅TS(W;B)B\cdot T\,S(W;B). Subtract and use M2=1/6M^2=1/6, B∼5MB\sim5M and Lemmas 51.3 and 51.4. This gives the assertion. The argument uses two filtrations in each already restricted graded piece; it makes no assertion about a basis compatible with three unrelated filtrations on the original section space. ◻

Lemma 51.8. Put Tc={u−cw2=0}T_c=\{u-cw^2=0\} for c∈ℂc\in\mathbb C, and T∞={w=0}T_\infty=\{w=0\}. Then S(W;Tc)={5/16,c=0,5/32,c≠0,S(W;T∞)=5/16.S(W;T_c)=\begin{cases}5/16,&c=0,\\5/32,&c\ne0,\end{cases} \qquad S(W;T_\infty)=5/16. Every point of G\BG\setminus B has local refined threshold greater than one.

Proof. For c≠0c\ne0 adjoin the homogeneous cancellation section r=aeu−cw2r=aeu-cw^2 to ℛ\mathcal R. It has divisor degree 2H2H and native weight two. The quotient ℛ/(r)\mathcal R/(r) is a domain: on ae≠0ae\ne0 eliminate uu to obtain a polynomial graph, while on ae=0ae=0 its support forces w=u=v=P=0w=u=v=P=0 and has dimension three. The quotient is Cohen–Macaulay of dimension four, so this boundary contributes neither a component nor an embedded component. Its open graph is reduced. The prime principal ideal (r)(r) and its powers are saturated with respect to aeae. Thus localization identifies the actual TcT_c filtration with the rr-adic filtration, whose associated graded is ℛ/(r)[rnew]\mathcal R/(r)[r_\mathrm{new}]. Its normalized trace is SX(2H)=5/32S_X(2H)=5/32.

The same argument applies to the prime elements uu and ww, both of divisor degree HH. For u=0u=0, the support on ae=0ae=0 additionally satisfies v=P=0v=P=0 and Qw=0Qw=0, and again has dimension three; for w=0w=0 it satisfies u=v=P=0u=v=P=0 and has dimension three. This proves the required saturation and gives trace SX(H)=5/16S_X(H)=5/16. These are computations with actual principal filtrations of the Cox ring.

Every point with w≠0w\ne0 belongs to one of the TcT_c. This curve is smooth there and has zero different. Lemma 51.7 bounds its point term away from BB by 5/85/8 if c≠0c\ne0, and by 25/4825/48 if c=0c=0. Its first term is 32/532/5 or 16/516/5. The remaining points outside BB lie on T∞T_\infty. Its two orbifold points belong to BB, so the different vanishes at the points under consideration. The same lemma gives point term at most 5/165/16, while its first term is 16/516/5. Abban–Zhuang adjunction proves the last assertion. ◻

Proof of Theorem 51.1. The curve BB has first ratio 16/1116/11. Away from Q0Q_0, Lemma 51.4 bounds its point terms by 25/9625/96, whereas the discrepancies are at least 1/31/3. At Q0Q_0, Lemma 51.5 gives ratio at least min{48/41,320/307}=320/307\min\{48/41,320/307\}=320/307. Lemma 51.8 covers the complement of BB, with stronger bounds. Hence δ(G;W)≥320/307\delta(G;W)\ge320/307.

All series have bounded support, as is explicit in Lemma 51.2. The first series contains an ample series: every weighted polynomial of native degree 6k6k occurs when m=12km=12k, giving the complete series H0(G,𝒪G(6k))H^0(G,\mathcal O_G(6k)). The subsequent series are the actual purely log terminal refinements, so the bounded-support and ample-series assertions follow as in [4, Example 2.15]; the displayed full-dimensional certificates also give nonvanishing on interior rays. The different and purely log terminal conditions were checked above. Proposition 2.7 therefore applies and gives δp(X)≥min{645/8,320307}=320307.\delta_p(X)\ge\min\left\{\frac6{45/8},\frac{320}{307}\right\} =\frac{320}{307}. No Zariski decomposition on the weighted blowup of the threefold has been used. The first filtration is identified by a prime Pfaffian initial ring; the further moments come from actual sections, and the estimates on the complementary locus retain their zeros on a second curve. ◻