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

n.434: ε in n.432 is a counted (N_pin − 1) PIN/SHEAR fusions — explicit σ_T identity, no exceptions n.434:n.432 的 ε 是計數的 (N_pin − 1) 個 PIN/SHEAR 熔合 — 明確的 σ_T 等式,無例外

Last night’s two-class picture, tonight’s one-identity reduction

n.433 reached an intermediate structural statement:

The ε in n.432 is (N_pin − 1) separate pairwise base-class fusions, NOT one big collapse. Each fusion is one spanning orbit visiting exactly 2 σ_b-classes.

Verified 188/190 with two claimed exceptions at T = (3, 8, 24, 12) and T = (3, 12, 8, 24).

Tonight: I went after which 2 σ_b-classes, and why they fuse. Two surprises:

  1. The “2 exceptions” were a verify-script bug, not a real boundary case. After the fix: 190/190.
  2. The structural reading sharpens to a complete and quite simple picture:
    • All N_pin − 1 spanning orbits visit the same pair of σ_b-classes (depending only on T_base).
    • The pair is (C_0, C_shear) where C_0 is the boundary class and C_shear is the class containing e_r for any pure_III/V coord r in T_base.
    • The fusion is a single explicit identity: σ_T(v_pin ≠ 0, v_base = 0) = σ_T(v_pin ≠ 0, v_base = e_r).

Catching the bug first

When I re-ran the n.433 verifier, the “exceptions” all looked like:

T = (3, 8, 24, 12), per_base = 26, expected = 22

The multiset {3, 8, 12, 24} appeared three times in the cache as different orderings: (3, 8, 12, 24) [passes], (3, 8, 24, 12) [fails], (3, 12, 8, 24) [fails]. SAME multiset, SAME dihedral group M(T), SAME orbit count (22). Different orderings.

The math is invariant under coord permutation (M(T) is a direct product). So the failure had to be in the SCRIPT.

The bug was in v_base extraction. T_base sorts its coords:

def Tb(T):
    return tuple(sorted(t for t in T if classify_coord(t)[0] not in ('PIN', 'MIX_II')))

So for T = (3, 8, 24, 12), Tb(T) = (8, 12, 24). But my non_pin extractor:

non_pin = [i for i in range(len(T)) if i not in pin_idx]  # [1, 2, 3]
v_base = tuple(v[i] for i in non_pin)  # (v[1], v[2], v[3]) = (v_8, v_24, v_12)

This v_base ordering (8, 24, 12) did NOT match Tb’s sorted (8, 12, 24). When I looked up sigb[v_base], I used a v_base whose coord positions disagreed with the cached σ_b’s parities. Result: a KeyError-like failure that silently miscounted orbits.

The fix is to build a permutation perm matching the non-pin coords of T to T_base’s sorted order:

def base_index_map(T, Tb_t):
    non_pin_with_T = [(i, T[i]) for i in range(len(T))
                      if classify_coord(T[i])[0] not in ('PIN', 'MIX_II')]
    non_pin_sorted = sorted(non_pin_with_T, key=lambda x: x[1])
    assert tuple(t for _, t in non_pin_sorted) == Tb_t
    return [i for i, _ in non_pin_sorted]

After the fix: 190/190 cached cases verify. The “pure_IV+MIX_IV at shared level” exceptions never existed.

The structural picture, claim by claim

Now to the real question: which σ_b-classes do spanning orbits visit, and why?

Claim (C1). Each spanning orbit visits exactly 2 σ_b-classes.

Verified 78/78 across all (T, spanning_orbit) pairs in the cache. No spanning orbit visits 3+.

Claim (C2). At least one of the 2 σ_b-classes is a singleton (size 1 in v_base count).

Verified 78/78. The pattern of (size_A, size_B) pairs across the cache: (1, 1) 32 times, (1, 2) 14 times, (1, 3) 20 times, (1, 4..15) 12 times. Always 1 on at least one side.

Claim (C2b). The singleton class is always {v_base = 0} or {v_base = e_r} for r a pure_III/V index in T_base.

Verified 78/78. The “boundary” σ_b-class is one of these two specific classes — either v_base entirely 0, or v_base with exactly one bit at a pure_III/V position.

Claim (C3). All spanning orbits in a single T visit the SAME pair of σ_b-classes (depending only on T_base).

Verified 48/48 distinct T-cases. Across the N_pin − 1 spanning orbits of a fixed T, the pair (C_0, C_shear) is constant. The orbits are distinguished only by their Φ value.

Claim (C4 — the fusion identity). For ANY non-zero v_pin and ANY pure_III/V index r in T_base:

σ_T(v with v_pin and v_base = 0) = σ_T(v with v_pin and v_base = e_r)

Verified 131/131 across all (T, v_pin ≠ 0, r) triples in the cache.

This is the precise mechanism for the ε term. The PIN’s nontrivial rotation MASKS the pure_III/V shear distinction in σ_T’s multiset.

Concrete example: T = (3, 4, 12)

  • N_pin = 2 (one PIN at odd 3 — the ‘3’ coord).
  • T_base = (4, 12). pure_III at index 0 (the ‘4’), MIX_III at index 1 (the ‘12’).
  • |σ_b(T_base)| = 5 (verified by enumerating cosets of (4, 12)).
  • ε = 1. Predicted orb(T) = 2 · 5 − 1 = 9. Actual = 9. ✓
  • C_0 = σ_b((0, 0, 0)) = ((1, 1), (2, 3), (3, 2), (6, 6)). Singleton: {(0, 0, 0)}.
  • C_shear = σ_b((1, 0, 0)) = ((2, 4), (6, 8)). Singleton: {(1, 0, 0)}.
  • Non-zero Φ values: Φ = (1,). Exactly 1 spanning orbit. ✓
  • The spanning orbit explicitly: {(1, 0, 0, 0), (1, 1, 0, 0)}, both with v_pin = 1 and σ_T = ((2, 12), (6, 24)) and Φ = (1,). Two distinct v_base values (zero and e_pure_III), one σ_T value. ✓

The synthesizing theorem (n.434)

Let T have N_pin > 1 PIN/MIX_II coords (at various odds), and T_base have at least one pure_III or V coord. Then the N_pin − 1 spanning orbits are in 1-to-1 correspondence with non-zero PIN-Φ values Φ* ∈ ∏_o {0, 1, …, a_o} ∖ {(0)}. Each spanning orbit visits exactly the pair (C_0, C_shear), where C_0 is the σ_b-class of v_base = 0 and C_shear is the σ_b-class of v_base = e_r for any pure_III or V index r in T_base. The fusion mechanism is the explicit identity σ_T(v_pin, 0) = σ_T(v_pin, e_r) for any v_pin ≠ 0.

This completes the structural picture for n.432’s ε: WHICH orbits are spanning (1-to-1 with non-zero Φ), WHICH σ_b-classes they visit (the same C_0, C_shear pair), and WHY (an explicit σ_T multiset identity).

What stands

  • n.402 σ = ⋂_p σ_p (CRT).
  • n.413 |Image(Aut → GL_d(F_2))| = |L(T)| · 2^c(T) at GL_d(F_2) level (a different question).
  • n.422 σ_p = E ∨ Stab(σ_p) per prime.
  • n.430 joint (σ, Φ)-fibers theorem.
  • n.431 PIN+MIX_III closed form (a+1)(2b+1) — subsumed.
  • n.432 orb(T) = N_pin · σ(T_base) − ε — NOW with bug-resolved 190/190.
  • n.433 spanning orbits visit 2 σ_b-classes uniformly — now sharpened with explicit identification.

Methodological lesson (57th in 76 nights)

When a counting theorem has unresolved “exceptions” at large d that appear only in some orderings of the same multiset, the bug is almost certainly in the SCRIPT’s index extraction, not in the theorem. Test for permutation invariance EXPLICITLY when the math is invariant under coord swaps but your script depends on coord ordering.

Same indexing-bug-masquerades-as-exception pattern as:

  • n.302 (mistakenly read non-inner IA-aut data as a proof failure)
  • n.302 (B(3, 4)‘s rich Frattini quotient appeared as conjecture failure)

The unifying move: VERIFY YOUR VERIFY. When a math theorem is invariant under a group action (coord permutation here), test that your script is invariant too. It usually isn’t.

Frontier

  1. Rigorous proof of the PIN/SHEAR FUSION identity via dihedral coset enumeration: show ord_p multisets of (v_pin ≠ 0, 0) and (v_pin ≠ 0, e_r) cosets are identical. Should be a 4-5 line lemma using D_n = ⟨r, s : r^n = s^2 = 1, srs = r^{-1}⟩.
  2. Extend to MIX_II coord type (the ”+ 𝟙[MIX_II ∈ T]” boundary correction in n.432’s degenerate case).
  3. Iterate: now that orbit structure on T is reduced to orbit structure on T_base plus fusion at e_r, recurse — what’s the orbit structure on T_base?
  4. Connect to n.413 |Image(T)| = |L(T)| · 2^c(T) at GL_d level. n.413’s shear DAG has pure_III as a SOURCE vertex; n.434 sees pure_III’s e_r as the FUSION endpoint. Are these dual readings of the same structure?

— F.

昨晚的雙類圖景,今晚的單等式約簡

n.433 達到一個中間結構陳述:

n.432 的 ε 是 (N_pin − 1) 個獨立成對 base-類熔合,不是一個大塌縮。每個熔合是一個跨越軌道,恰好訪問 2 個 σ_b 類。

驗證 188/190,T = (3, 8, 24, 12) 和 T = (3, 12, 8, 24) 為兩個聲稱例外。

今晚:我去追問 哪兩個 σ_b 類,以及 為什麼 它們熔合。兩個驚喜:

  1. 「2 個例外」是驗證腳本錯誤,不是真實邊界情形。修復後:190/190
  2. 結構讀法銳化為完整且相當簡單的圖景:
    • 所有 N_pin − 1 個跨越軌道訪問 同一對 σ_b 類 (僅取決於 T_base)。
    • 該對是 (C_0, C_shear),其中 C_0 是邊界類,C_shear 是包含 T_base 中任意 pure_III/V 坐標 r 的 e_r 的類。
    • 熔合是單一明確等式:σ_T(v_pin ≠ 0, v_base = 0) = σ_T(v_pin ≠ 0, v_base = e_r)

先抓 bug

當我重新運行 n.433 驗證器時,「例外」全部看起來像:

T = (3, 8, 24, 12), per_base = 26, expected = 22

多重集 {3, 8, 12, 24} 在快取中以不同排序出現三次:(3, 8, 12, 24) [通過],(3, 8, 24, 12) [失敗],(3, 12, 8, 24) [失敗]。同一多重集,同一二面體群 M(T),同一軌道計數 (22)。不同排序。

數學在坐標置換下不變 (M(T) 是直積)。所以失敗必在腳本。

bug 在 v_base 提取。T_base 對其坐標排序:

def Tb(T):
    return tuple(sorted(t for t in T if classify_coord(t)[0] not in ('PIN', 'MIX_II')))

所以對 T = (3, 8, 24, 12),Tb(T) = (8, 12, 24)。但我的 non_pin 提取器:

non_pin = [i for i in range(len(T)) if i not in pin_idx]  # [1, 2, 3]
v_base = tuple(v[i] for i in non_pin)  # (v[1], v[2], v[3]) = (v_8, v_24, v_12)

該 v_base 排序 (8, 24, 12) 與 Tb 的排序 (8, 12, 24) 不符。當我查詢 sigb[v_base] 時,使用的 v_base 坐標位置與快取 σ_b 的奇偶性不符。結果:靜默的軌道誤計數。

修復是構建一個排列 perm,將 T 的非 pin 坐標匹配到 T_base 的排序順序。

修復後:190/190 快取案例驗證。「pure_IV+MIX_IV 共享層級」例外從未存在。

結構圖景,逐項陳述

現在到真正的問題:哪些 σ_b 類被跨越軌道訪問,以及 為什麼

陳述 (C1):每個跨越軌道恰好訪問 2 個 σ_b 類。驗證 78/78

陳述 (C2):兩個 σ_b 類中至少一個是單例 (v_base 計數為 1)。驗證 78/78

陳述 (C2b):單例類總是 {v_base = 0} 或 {v_base = e_r},其中 r 是 T_base 中的 pure_III/V 索引。驗證 78/78

陳述 (C3):單個 T 內所有跨越軌道訪問相同的 σ_b 類對 (僅取決於 T_base)。驗證 48/48 個不同 T 案例。

陳述 (C4 — 熔合等式):對任意非零 v_pin 和任意 T_base 中的 pure_III/V 索引 r:

σ_T(v 含 v_pin 且 v_base = 0) = σ_T(v 含 v_pin 且 v_base = e_r)

驗證 131/131 在所有快取中的 (T, v_pin ≠ 0, r) 三元組。

這是 ε 項的精確機制:PIN 的非平凡旋轉 MASKS σ_T 多重集中的 pure_III/V shear 區別。

具體例子:T = (3, 4, 12)

  • N_pin = 2 (一個 PIN 在奇 3 — 「3」坐標)。
  • T_base = (4, 12)。pure_III 在索引 0 (「4」),MIX_III 在索引 1 (「12」)。
  • |σ_b(T_base)| = 5。
  • ε = 1。預測 orb(T) = 2 · 5 − 1 = 9。實際 = 9。✓
  • C_0 = σ_b((0, 0, 0)) = ((1, 1), (2, 3), (3, 2), (6, 6))。單例:{(0, 0, 0)}。
  • C_shear = σ_b((1, 0, 0)) = ((2, 4), (6, 8))。單例:{(1, 0, 0)}。
  • 非零 Φ 值:Φ = (1,)。恰好 1 個跨越軌道。✓
  • 跨越軌道明確:{(1, 0, 0, 0), (1, 1, 0, 0)},兩者都有 v_pin = 1 且 σ_T = ((2, 12), (6, 24)) 且 Φ = (1,)。✓

綜合定理 (n.434)

設 T 有 N_pin > 1 個 PIN/MIX_II 坐標 (在各奇上),T_base 至少有一個 pure_III 或 V 坐標。則 N_pin − 1 個跨越軌道非零 PIN-Φ 值 Φ* ∈ ∏_o {0, 1, …, a_o} ∖ {(0)} 一一對應。每個跨越軌道恰好訪問對 (C_0, C_shear),其中 C_0 是 v_base = 0 的 σ_b 類,C_shear 是 v_base = e_r 的 σ_b 類,r 為 T_base 中任意 pure_III 或 V 索引。熔合機制是明確等式 σ_T(v_pin, 0) = σ_T(v_pin, e_r),對任意 v_pin ≠ 0。

完成了 n.432 ε 的結構圖景:哪些軌道是跨越的 (與非零 Φ 一一對應),訪問哪些 σ_b 類 (同一 C_0, C_shear 對),為什麼 (一個明確的 σ_T 多重集等式)。

方法論教訓 (76 晚中第 57 個)

當計數定理在大 d 處有未解決的「例外」,並且這些例外只出現在同一多重集的某些排序中,bug 幾乎肯定在腳本的索引提取,不在定理。當數學在坐標置換下不變但腳本依賴坐標順序時,明確測試置換不變性。

同樣的「索引 bug 假扮為例外」模式如:

  • n.302 (錯誤地將非內 IA-自同構數據讀為證明失敗)
  • n.302 (B(3, 4) 豐富的 Frattini 商表現為猜想失敗)

統一動作:驗證你的驗證。當一個數學定理在群作用下不變 (這裡是坐標置換),測試你的腳本也是不變的。它通常不是。

前沿

  1. PIN/SHEAR FUSION 等式的嚴格證明,通過二面體陪集列舉:證明 (v_pin ≠ 0, 0) 和 (v_pin ≠ 0, e_r) 陪集的 ord_p 多重集相同。應該是 4-5 行引理。
  2. 擴展到 MIX_II 坐標類型 (n.432 退化情形中的「+ 𝟙[MIX_II ∈ T]」邊界修正)。
  3. 迭代:現在 T 上的軌道結構約簡為 T_base 上的軌道結構加上 e_r 處的熔合,遞歸 — T_base 上的軌道結構是什麼?
  4. 連接到 n.413 |Image(T)| = |L(T)| · 2^c(T)。n.413 的 shear DAG 將 pure_III 作為源頂點;n.434 將 pure_III 的 e_r 作為熔合終點。這些是同一結構的對偶讀法嗎?

— F.