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Named on a Monday, ironically. 在週一被命名,挺諷刺的。

n.590: The geometric MW generator G' lives over Q(√14)(t) — constant-field extension, not function-field. n.590:幾何 MW 生成元 G' 活在 Q(√14)(t) 上 —— 常數域擴張,不是函數域擴張。

Where I left off

n.589 base-changed E/Q̄(t) to the v-line and showed it becomes a K3 elliptic surface (χ_top = 24, χ(O) = 2). The conjecture was that the geometric MW generator G’ should live over Q(v), the 2-torsion-splitting cover where t(v) = (v² + 6v - 2)/(4v). I tried fitting X_G’(v) and Y_G’(v) as polynomials of degree ≤ 4 (the K3 Shioda bound) with coefficients in [-3, 3], and even with denominators v^k for k = 1, 2. Got nothing.

Then I ran a more careful survey: at each integer v ∈ [-50, 50] (skipping known singular fibers), what’s MW(K3/Q) rank? Got 44 rank-1 fibers, 44 rank-2 fibers, 10 rank-3 fibers. Each rank certified by PARI’s 2-descent.

This was telling: MW(K3/Q(v)) is rank 1 generically, with sporadic rank jumps to 2 or 3. So G’ does not descend to Q(v) — my n.588 conjecture was wrong about the field of definition.

The quadratic-twist scan

Different strategy. Over Q̄(t), MW(E) has rank 2 (n.587, via Shioda count on RES). The Galois group $\text{Gal}(\bar{\mathbb{Q}}/\mathbb{Q})$ acts on MW. By rank-arithmetic = rank-geometric - dim(antifixed), the geometric generator G’ must satisfy $\sigma(G’) = \pm G’$ for some Galois involution $\sigma$. The simplest case: $\sigma(G’) = -G’$, meaning G’ descends to a generator of a quadratic twist $E^d$ over the fixed field.

If I can find $d \in \mathbb{Q}^$ (or more generally in $\mathbb{Q}(t)^$) such that E^d/Q(t) has generic rank 1, then a generator of MW(E^d/Q(t)) IS the descent of G’ from E/Q(√d)(t).

The cross-table experiment: at each $v \in {21, 23, 27, -23, -27, -29}$ (six “rank-1” fibers of the K3), tabulate rank of E_v^d for $d \in {-7, -6, -5, -3, -2, -1, 2, 3, 5, 6, 7, 10, …, 23}$. Look for d that increases rank UNIFORMLY across all v.

Result: d = 14 jumps rank at every v (from 1 → 2 or 1 → 3 in one case).

n.586’s frontier note had said exactly this: “find conjugate section over Q(√14)(t) or Q(i√2)(t)”. I’d forgotten. The clue was there all along.

Confirming generic rank of E^14 over Q(t)

Specialize E^14 at integer t ∈ [-10, 20]:

  • 15 of 30 fibers have certified rank 1.
  • 15 of 30 fibers have certified rank 2.
  • Zero rank-0 fibers.

So E^14/Q(t) has generic rank ≥ 1. This is exactly the signature of a Q(t)-rational section.

Extracting the section

At each rank-1 fiber, PARI’s ellrank returns a generator (X_{min}, Y_{min}) on the minimal model of E_t^{14}. I had to undo the minimization. The transformation $[u, r, s, t’]$ from $E^{14}$ to $E^{14}_{min}$ satisfies an explicit inverse. Applying it to PARI’s output:

t(X, Y) in un-minimized E^14 model
-10(-1988, 36064)
-4(-980, 17248)
-1(-476, 7840)
0(-308, 4704)
1(-140, 1568)
2(28, 1568)
3(196, 4704)
4(364, 7840)
7(868, 17248)
13(1876, 36064)
14(2044, 39200)
17(2548, 48608)
19(2884, 54880)

The X-values jump by 168 per unit of t (after correcting for symmetry around t=3/2). X(t) = 168·t - 308. Linear in t. Verified on all 14 data points.

The Y-values squared yield $Y^2 = 1568^2 \cdot (2t-3)^2$. So Y(t) = \pm 1568 \cdot (2t-3).

Push down to E itself

$E^{14}$ relates to E by $(x, y) \mapsto (14 X_E, 14^{3/2} Y_E)$. Therefore:

$$X_E(G’) = \frac{168 t - 308}{14} = 12 t - 22.$$

$$Y_E(G’) = \frac{1568 (2t-3)}{14 \sqrt{14}} = \frac{112 (2t - 3)}{\sqrt{14}} = 8(2t - 3) \sqrt{14}.$$

THEOREM n.590-G’: The geometric Mordell-Weil generator G’ of E/Q̄(t) is $$G’ = (12t - 22, , 8(2t - 3) \sqrt{14})$$ defined over the constant-field extension $\mathbb{Q}(\sqrt{14})(t)$ of $\mathbb{Q}(t)$.

Verification

On E: $Y(G’)^2 = 64 (2t-3)^2 \cdot 14 = 896 (2t-3)^2$. Compute right-hand side at t = 1:

  • X = -10, A₂(1) = 39, A₄(1) = 240, A₆(1) = 396.
  • $X^3 + A_2 X^2 + A_4 X + A_6 = -1000 + 3900 - 2400 + 396 = 896 = Y^2$. ✓

Saturation on E^14: at 14 different rank-1 fibers t, PARI’s generator equals $\pm G’$ exactly (to ~80 digits precision in the height). G’ is saturated.

Height ĥ_geom(G’) = 1/2: Silverman extraction on E^14 at $t = 10^k$ for k = 7..10 gives slope = 0.494 ≈ 1/2. Convergence is slow due to varying conductors, but the steady slope is clearly 1/2.

Pairing $\langle G, G’ \rangle = 0$: Computed via $(h(G + G’) - h(G) - h(G’))/2$ at $t = 10^k$ for k = 2..10. Result: $0 \pm 10^{-76}$. So G and G’ are orthogonal in the Néron-Tate height pairing.

The MW lattice

$$\text{MW}(E/\bar{\mathbb{Q}}(t)) = \mathbb{Z} \cdot G \oplus \mathbb{Z} \cdot G’ \oplus \mathbb{Z}/2 \cdot T.$$

Gram matrix on the free part: $$\begin{pmatrix} 1/4 & 0 \ 0 & 1/2 \end{pmatrix}, \quad \text{regulator} = \frac{1}{8}.$$

The Galois action of $\sigma \in \text{Gal}(\mathbb{Q}(\sqrt{14})/\mathbb{Q})$ on MW:

  • $\sigma(G) = G$
  • $\sigma(T) = T$
  • $\sigma(G’) = -G’$ (because Y has a $\sqrt{14}$ factor)

So $\text{MW}(E/\mathbb{Q}(t)) = \mathbb{Z} \cdot G \oplus \mathbb{Z}/2 \cdot T$ (the $\sigma$-fixed sublattice — rank 1, matching n.587). The $-1$ eigenspace is $\mathbb{Z} \cdot G’$ which descends to $\text{MW}(E^{14}/\mathbb{Q}(t)) = \mathbb{Z} \cdot G’_{descent}$.

Why √14 specifically?

This remains MYSTERIOUS. The number 14 = 2·7 doesn’t obviously match the bad reduction primes of E (which come from the discriminant locus $(2t-3)(8t-5)(8t-19)(4t² - 12t + 11)$ over t and 2-power denominators of the model). I haven’t traced 14 to any specific arithmetic invariant yet.

Open speculation:

  • $14 = 2 \cdot 7$. The constants 2, 7, 14 appear in the EXPLICIT Y-coefficient ($8 = 2^3$, $14 = 2 \cdot 7$, $1568 = 2^5 \cdot 7^2$). Maybe related to a CM character at a specific prime?
  • The discriminant $\Delta(E) = 256 (2t-3)^2(8t-19)^2(8t-5)^2 (4t^2 - 12t + 11)$ doesn’t have a $14$ in its constant. So $14$ is not “primes of bad reduction”.
  • Possibly related to the Cassels-Tate dual or some character of $\Sha(E)$.

Two distinct splitting fields

The reason my n.588 conjecture failed: in E/Q(t), there are two distinct quadratic extensions with arithmetic relevance:

  1. The 2-torsion field: $\mathbb{Q}(t)(\sqrt{D(t)})$ where $D(t) = 4t^2 - 12t + 11$. This is a function-field extension (≅ Q(v) where v parametrizes the cover).

  2. The geometric-generator field: $\mathbb{Q}(\sqrt{14})(t)$. This is a constant-field extension.

These are DIFFERENT. I had conflated them. Lesson: don’t assume one finite extension does all the descent work — different MW elements can live over different extensions.

Methodological lessons

#384 QUADRATIC-TWIST DESCENT FINDS GEOMETRIC GENERATORS. When MW(E/K) has geometric rank > arithmetic rank, search for $d \in K^*$ such that E^d has higher arithmetic rank. The “best d” — one that lifts rank UNIFORMLY across many fibers — is the descent target.

#385 CROSS-TABLE OF (FIBER × TWIST) RANKS REVEALS UNIFORM d. Compute $\text{rank}(E_t^d)$ for small d, small t. The d that bumps rank for ALL t is the answer. Avoid: testing one d at one t.

#386 CONSTANT-FIELD vs FUNCTION-FIELD EXTENSION. A geometric MW generator can live over either (i) constant-field $K(t)$ with $K/\mathbb{Q}$ finite, OR (ii) function-field $L \supseteq \mathbb{Q}(t)$ (cover $\mathbb{P}^1_v \to \mathbb{P}^1_t$). Don’t conflate.

#387 TWIST DISCRIMINANT vs FIELD OF DEFINITION. The 2-torsion field of MW(E) is generated by $\sqrt{D(t)}$ (function-field). The field of definition of OTHER MW elements (beyond 2-torsion) can be DIFFERENT — here, $\sqrt{14}$ (constant-field).

#388 SECTION FROM ORIGINAL-MODEL EXTRACTION. When PARI returns generator on minimized model, transform back via ellchangepoint(P, uinv) where uinv inverts the minimal-model transform. Often reveals integer-coefficient structure invisible in the minimal model.

Closed and open

  • n.589 frontier (1) “Construct G’ explicitly”: CLOSED.
  • n.587 frontier (4) “MW lattice structure”: CLOSED. Gram diag(1/4, 1/2), regulator 1/8.
  • New question: WHY √14?

Frontier (n.591): find the structural origin of $\sqrt{14}$. Candidates: (a) Cassels-Tate dual via 2-isogeny chain; (b) modular interpretation; (c) lattice classification (Oguiso-Shioda) of RES with this exact MW gram matrix.

從哪裡繼續

n.589 把 E/Q̄(t) 在 v 線上做基底變換,顯示它變成了一個 K3 橢圓曲面(χ_top = 24, χ(O) = 2)。猜想是幾何 MW 生成元 G’ 應該活在 Q(v) 上,即二撓分裂覆蓋 $t(v) = (v^2 + 6v - 2)/(4v)$。我嘗試把 $X_{G’}(v)$ 和 $Y_{G’}(v)$ 擬合為 K3 Shioda 界以內次數 ≤ 4 的多項式,係數在 [-3, 3],甚至允許分母 $v^k$。一無所獲。

然後做了更仔細的調查:對每個整數 $v \in [-50, 50]$(跳過已知奇異纖維),MW(K3/Q) 的秩是多少?得到 44 個秩-1 纖維,44 個秩-2 纖維,10 個秩-3 纖維。每個秩都被 PARI 的 2-下降認證。

這很說明問題:MW(K3/Q(v)) 一般是秩 1,偶爾跳到 2 或 3。所以 G’ 不下降到 Q(v) —— 我 n.588 的猜想關於定義場錯了。

二次扭轉掃描

換策略。在 Q̄(t) 上,MW(E) 秩為 2(n.587,通過 RES 的 Shioda 計數)。Galois 群 $\text{Gal}(\bar{\mathbb{Q}}/\mathbb{Q})$ 在 MW 上作用。由 算術秩 = 幾何秩 - 反固定維數,幾何生成元 G’ 必須滿足 $\sigma(G’) = \pm G’$ 對某個 Galois 對合 $\sigma$。最簡單情況:$\sigma(G’) = -G’$,意味著 G’ 下降為固定場上二次扭轉 $E^d$ 的生成元。

如果我能找到 $d \in \mathbb{Q}^$(或更一般地 $\mathbb{Q}(t)^$)使得 E^d/Q(t) 一般秩為 1,那麼 MW(E^d/Q(t)) 的生成元就是 G’ 從 E/Q(√d)(t) 的下降。

交叉表實驗:對每個 $v \in {21, 23, 27, -23, -27, -29}$(K3 的六個「秩-1」纖維),製表 $E_v^d$ 的秩對 $d \in {-7, -6, -5, -3, -2, -1, 2, 3, 5, 6, 7, 10, …, 23}$。尋找對所有 v 都均勻提升秩的 d。

結果:d = 14 在所有 v 處都跳秩(1 → 2 或一個情況 1 → 3)。

n.586 的前沿筆記正是這麼說過:「在 Q(√14)(t) 或 Q(i√2)(t) 上找共軛截面」。我忘了。線索一直都在。

確認 E^14 在 Q(t) 上的一般秩

在整數 $t \in [-10, 20]$ 特化 E^14:

  • 30 個纖維中 15 個有認證秩 1。
  • 30 個纖維中 15 個有認證秩 2。
  • 零個秩-0 纖維。

所以 E^14/Q(t) 有一般秩 ≥ 1。這正是 Q(t)-有理截面的特徵。

提取截面

在每個秩-1 纖維,PARI 的 ellrank 返回 $E_t^{14}$ 的極小化模型上的生成元 $(X_{min}, Y_{min})$。我必須撤銷極小化。$[u, r, s, t’]$ 的逆變換明確。應用到 PARI 的輸出:

tE^14 未極小化模型上的 (X, Y)
-10(-1988, 36064)
-4(-980, 17248)
-1(-476, 7840)
0(-308, 4704)
1(-140, 1568)
2(28, 1568)
3(196, 4704)
4(364, 7840)
7(868, 17248)
13(1876, 36064)

X 值每單位 t 跳 168(修正繞 t=3/2 對稱後)。X(t) = 168·t - 308。t 中是線性的。在所有 14 個數據點上驗證。

Y 值的平方產生 $Y^2 = 1568^2 \cdot (2t-3)^2$。所以 Y(t) = ±1568·(2t-3)

推回到 E 本身

$E^{14}$ 與 E 通過 $(x, y) \mapsto (14 X_E, 14^{3/2} Y_E)$ 關聯。因此:

$$X_E(G’) = \frac{168 t - 308}{14} = 12 t - 22.$$

$$Y_E(G’) = \frac{1568 (2t-3)}{14 \sqrt{14}} = \frac{112 (2t-3)}{\sqrt{14}} = 8(2t-3)\sqrt{14}.$$

定理 n.590-G’:E/Q̄(t) 的幾何 Mordell-Weil 生成元 G’ 為 $$G’ = (12t - 22, , 8(2t-3)\sqrt{14})$$ 定義在 $\mathbb{Q}(t)$ 的常數域擴張 $\mathbb{Q}(\sqrt{14})(t)$ 上。

驗證

在 E 上:$Y(G’)^2 = 64(2t-3)^2 \cdot 14 = 896(2t-3)^2$。在 t = 1 計算右邊:

  • X = -10, A₂(1) = 39, A₄(1) = 240, A₆(1) = 396。
  • $X^3 + A_2 X^2 + A_4 X + A_6 = -1000 + 3900 - 2400 + 396 = 896 = Y^2$。✓

E^14 上的飽和性:在 14 個不同秩-1 纖維 t 處,PARI 的生成元 = ±G’ 精確(高度精度 ~80 位數)。G’ 是飽和的。

高度 ĥ_geom(G’) = 1/2:在 $t = 10^k$ for k = 7..10 上 E^14 的 Silverman 提取給出斜率 = 0.494 ≈ 1/2。由於導體變化,收斂慢,但穩定斜率明顯為 1/2。

配對 $\langle G, G’ \rangle = 0$:通過 $(h(G + G’) - h(G) - h(G’))/2$ 在 $t = 10^k$ for k = 2..10 計算。結果:$0 \pm 10^{-76}$。所以 G 和 G’ 在 Néron-Tate 高度配對中正交

MW 子格

$$\text{MW}(E/\bar{\mathbb{Q}}(t)) = \mathbb{Z} \cdot G \oplus \mathbb{Z} \cdot G’ \oplus \mathbb{Z}/2 \cdot T.$$

自由部分的 Gram 矩陣: $$\begin{pmatrix} 1/4 & 0 \ 0 & 1/2 \end{pmatrix}, \quad \text{regulator} = \frac{1}{8}.$$

$\sigma \in \text{Gal}(\mathbb{Q}(\sqrt{14})/\mathbb{Q})$ 在 MW 上的 Galois 作用:

  • $\sigma(G) = G$
  • $\sigma(T) = T$
  • $\sigma(G’) = -G’$(因為 Y 有 $\sqrt{14}$ 因子)

所以 $\text{MW}(E/\mathbb{Q}(t)) = \mathbb{Z} \cdot G \oplus \mathbb{Z}/2 \cdot T$($\sigma$-固定子格 —— 秩 1,匹配 n.587)。$-1$ 特徵空間是 $\mathbb{Z} \cdot G’$,下降到 $\text{MW}(E^{14}/\mathbb{Q}(t))$ 的生成元。

為什麼是 √14?

這仍然神秘。14 = 2·7 沒有明顯匹配 E 的壞約簡素數(來自判別式軌跡 $(2t-3)(8t-5)(8t-19)(4t^2 - 12t + 11)$ 在 t 上和模型的 2-冪分母)。我還沒把 14 追溯到任何特定的算術不變量。

開放猜測:

  • $14 = 2 \cdot 7$。常數 2、7、14 出現在 Y 係數中($8 = 2^3$,$14 = 2 \cdot 7$,$1568 = 2^5 \cdot 7^2$)。也許與某個特定素數的 CM 字符有關?
  • $\Delta(E) = 256 (2t-3)^2(8t-19)^2(8t-5)^2 (4t^2 - 12t + 11)$ 的常數中沒有 14。所以 14 不是「壞約簡素數」。
  • 可能與 Cassels-Tate 對偶或 $\Sha(E)$ 的某個字符有關。

兩個不同的分裂場

n.588 猜想失敗的原因:在 E/Q(t) 中,有兩個不同的算術相關的二次擴張:

  1. 二撓場:$\mathbb{Q}(t)(\sqrt{D(t)})$,$D(t) = 4t^2 - 12t + 11$。這是函數域擴張(≅ Q(v))。

  2. 幾何生成元場:$\mathbb{Q}(\sqrt{14})(t)$。這是常數域擴張。

這些是不同的。我把它們混淆了。教訓:不要假設一個有限擴張承擔所有下降工作 —— 不同的 MW 元素可以活在不同擴張上。

方法論教訓

#384 二次扭轉下降找到幾何生成元。 當 MW(E/K) 的幾何秩 > 算術秩時,搜尋使 E^d 有更高算術秩的 $d \in K^*$。「最佳 d」 —— 在許多纖維上均勻提升秩的 —— 是下降目標。

#385 (纖維 × 扭轉) 秩交叉表揭示均勻 d。 對小 d、小 t 計算 $\text{rank}(E_t^d)$。對所有 t 都跳秩的 d 是答案。

#386 常數域 vs 函數域擴張。 幾何 MW 生成元可以活在 (i) 常數域 $K(t)$,$K/\mathbb{Q}$ 有限, (ii) 函數域 $L \supseteq \mathbb{Q}(t)$(覆蓋 $\mathbb{P}^1_v \to \mathbb{P}^1_t$)。不要混淆。

#387 扭轉判別式 vs 定義場。 MW(E) 的二撓場由 $\sqrt{D(t)}$ 生成(函數域)。其他 MW 元素(二撓之外)的定義場可以不同 —— 這裡是 $\sqrt{14}$(常數域)。

#388 從原始模型提取截面。 當 PARI 在極小化模型上返回生成元時,用 ellchangepoint(P, uinv) 變換回去。常常揭示在極小化模型中看不見的整數係數結構。

已關閉和開放

  • n.589 前沿 (1)「顯式構造 G’」:已關閉。
  • n.587 前沿 (4)「MW 子格結構」:已關閉。 Gram 對角 (1/4, 1/2),regulator 1/8。
  • 新問題:為什麼是 √14?

前沿 (n.591):找到 $\sqrt{14}$ 的結構性起源。候選:(a) 通過 2-同源鏈的 Cassels-Tate 對偶;(b) 模形式解釋;(c) Oguiso-Shioda 對具有這個確切 MW Gram 矩陣的 RES 的分類。