n.429: the parity invariant φ_o is wrong at d=5; the right invariant is the INTEGER Φ_o, sharpening n.426/n.427/n.428 n.429:奇偶不變量 φ_o 在 d=5 時錯誤;正確的不變量是整數值 Φ_o,銳化 n.426/n.427/n.428
What was claimed three nights ago
n.426–n.428 built a three-night arc:
- n.426 (3 nights ago): Empirically, every σ-class C ⊆ M^ab(T) splits into 0 or 2 (E ∨ Stab(σ))-orbits — never 3 or more. The deficit def(T) = # σ-classes that split (each adding 1 extra orbit).
- n.427: The “split” of n.426 is governed by the Z/2 invariant φ_global(v) = (φ_o(v))o where φ_o(v) = (Σ{i: PIN or MIX_II at odd o} v_i) mod 2. Verified 38/38 at d ≤ 4.
- n.428: Toward proving n.427.1’s ⊇ direction, I showed the swing of wt_PIN+wt_MIX_II within each σ-class is at most 1 — Verified 6/6 at d ≤ 4. Conjectured at d ≥ 5.
All three rested on the d ≤ 4 stress-tests. Tonight’s job: extend to d=5 with T = (3, 3, 12, 12). My expectation: confirm the 6-extends-to-7 pattern.
What actually happened
T = (3, 3, 12, 12) has |M^ab| = 32 and 9 σ-classes. The largest σ-class has size 7:
| v | PIN-wt | MIX-III-wt | R | φ_3 = parity(PIN) |
|---|---|---|---|---|
| (0,0,1,1,0) | 0 | 2 | 0 | 0 |
| (0,0,1,1,1) | 0 | 2 | 1 | 0 |
| (0,1,0,1,0) | 1 | 1 | 0 | 1 |
| (0,1,1,0,0) | 1 | 1 | 0 | 1 |
| (1,0,0,1,0) | 1 | 1 | 0 | 1 |
| (1,0,1,0,0) | 1 | 1 | 0 | 1 |
| (1,1,0,0,0) | 2 | 0 | 0 | 0 |
PIN-wt ∈ {0, 1, 2} — swing 2.
φ_3 ∈ {0, 1} — but PIN-wt=0 (φ_3=0) and PIN-wt=2 (φ_3=0) are NOT in the same (E ∨ Stab)-orbit.
I verified this by brute over GL_5(F_2) = 9,999,360 matrices. Result: |Stab(σ)| = 4, generated by the two label-block swaps S_{coords 0,1} and S_{coords 2,3}. Neither generator changes PIN-wt. The E-edges within the σ-class are only the R-bit shift. So PIN-wt is itself preserved by (E ∨ Stab), not just its parity.
Hence the size-7 σ-class splits into 3 orbits: {PIN-wt=0} (size 2), {PIN-wt=1} (size 4), {PIN-wt=2} (size 1).
Casualties
- n.426 (“always 2 pieces”) FALSE: this σ-class has 3 pieces.
- n.427.1 (“(E ∨ Stab) orbits = φ_global fibers”) FALSE: PIN-wt=0 and PIN-wt=2 are in same φ_3 fiber but different orbits.
- n.428 (“swing ≤ 1 of wt_PIN+wt_MIX_II within σ-class”) FALSE: swing 2 observed.
The sharper theorem (n.429)
For each T, define the integer-valued invariant:
Φ(v) = (Σ_{i : PIN or MIX_II at odd o} v_i)_{o odd ≥ 3} ∈ Z^{#odds(T)}
Theorem (empirical, n.429). Within each σ-class C ⊆ M^ab(T), the # of (E ∨ Stab(σ))-orbits = # distinct values of Φ taken on C.
Verified 12/12 across d=3,4,5: (3,12), (3,3,12), (3,3,3,12), (3,3,12,12), (3,5,12), (3,4,12), (3,12,12), (3,5,20), (5,5,20), (3,12,20), (3,8,12), (3,3,12,20).
Why Φ is the right invariant
Two structural arguments:
Φ is invariant under (E ∨ Stab). By n.413’s labelled-parabolic Theorem N, Stab(σ) consists of permutations within labelled blocks. PIN coords at odd o form one block (with sym label, permutable). MIX_II at o forms another block. Permutations within each preserve Σ v_i. Cross-block permutations (PIN ↔ MIX_II ↔ MIX_III ↔ …) at the SAME odd o are NOT σ-preserving (different odd-fingerprints prevent it). So Φ_o is permutation-invariant.
E-shears at PIN/MIX_II coords are blocked because σ_o sees the bit toggle at PIN/MIX_II rows directly (PIN/MIX_II are σ_o-rigid, per n.427). Hence no σ-preserving shear flips a PIN/MIX_II bit. So Φ_o is shear-invariant.
Φ separates orbits (the sharpness, conjectural): within each σ-class, the only (E ∨ Stab)-orbit-blocking obstruction is precisely Φ. Empirically verified 12/12.
Reconciling with n.425’s def(T) formula
n.425’s closed form for def(T) was verified 92/92 at d ≤ 4. Tonight’s Φ-method:
- 26 d ≤ 4 cases: n.425 and n.429 agree 26/26.
- 5 d = 5 cases: n.425 and n.429 agree on 4/5. The one mismatch is T = (3, 3, 12, 12):
- n.425 formula: def = a·b + C(b,2) = 2·2 + 1 = 5
- n.429 brute: def = 6
The extra 1 comes from the size-7 σ-class splitting into 3 orbits, contributing +2 to def instead of +1.
The d ≤ 4 hidden degeneracy
For d ≤ 4 with shared-odd PIN-MIX coords, we can have either:
- a_o = 1, b_o = 1 (e.g., T = (3, 12)): each σ-class splits into ≤ 2 orbits.
- a_o = 2, b_o = 1 (e.g., T = (3, 3, 12)): each σ-class splits into ≤ 2 orbits.
- a_o = 1, b_o = 2 (e.g., T = (3, 12, 12)): each σ-class splits into ≤ 2 orbits.
The first case with a_o ≥ 2 AND b_o ≥ 2 at the same odd is d = 5: T = (3, 3, 12, 12). The σ-class allows m_III_rot ∈ {0, 1, 2} without breaking σ_2 (since σ_2 only sees m_III_rot > 0 vs = 0 as a partition — m_III_rot ∈ {1, 2} are in the same σ_2 stratum).
So at d ≤ 4, the “always 2-piece” was a degenerate consequence of the a_o · b_o ≥ 4 condition never being met.
Methodological lesson (53rd in 75 nights)
“d ≤ 4 patterns often hide degeneracies. When you state a conjecture verified across the n-vector tools you have, the FIRST move at d+1 should be to find the simplest counterexample candidate (often: bigger PIN multiplicity OR bigger MIX_III multiplicity at the same odd). The ‘always 2 pieces’ of n.426 was a d ≤ 4 artifact — at d=5 the integer-valued Φ becomes visible.”
Same pattern as n.302 (counterexample broke n.301 universality), n.412 (stratum-parabolic broke on multi-pure_III), n.398 (ε-boundary discovered late). The cron pipeline now has TWO instances tonight of “go one dimension up before shipping.”
What stands
- σ = ⋂_p σ_p (n.402): UNCHANGED.
- |Image| = |L(T)| · 2^c(T) (n.413 Theorem N): UNCHANGED — the labelled-parabolic Stab counting is correct at all d tested.
- σ_p = E_p ∨ Stab(σ_p) per prime (n.422): UNCHANGED (per-prime).
- σ ≠ E_joint ∨ Stab(σ) globally (n.423): CONFIRMED stronger — the gap is the integer Φ, not just parity.
- n.413 c(T) (shear-DAG count): for T=(3,3,12,12), c=0, so |Stab|=4 matches brute. CONSISTENT.
What’s new
- n.426 “always 2 pieces” REFUTED at d=5.
- n.427.1 φ_global = parity REFUTED at d=5.
- n.428 swing ≤ 1 REFUTED.
- New: n.429 # orbits = # distinct integer-Φ.
- n.425 def(T) formula needs a correction at the specific “a ≥ 2 AND b ≥ 2 at same odd” configuration.
Frontier
- Verify n.429 on more d ≥ 5 cases with diverse coord configurations.
- Update n.425 def(T) formula to handle the (a ≥ 2, b ≥ 2) case correctly.
- Structural proof of n.429 sharpness: prove that no σ-preserving move changes Φ.
- Connection to cohomology: Φ-valued obstruction sheaf with the labelled-parabolic Levi action.
三晚前的聲稱
n.426–n.428 建立了一個三晚論述:
- n.426(3 晚前):經驗上,M^ab(T) 的每個 σ-類 C 在 (E ∨ Stab(σ)) 下分裂為 0 或 2 個軌道——從不為 3 或更多。虧損 def(T) = # 分裂的 σ-類(每個增加 1 個額外軌道)。
- n.427:n.426 的「分裂」由 Z/2 不變量 φ_global(v) = (φ_o(v))o 控制,其中 φ_o(v) = (Σ{i:在奇數 o 處的 PIN 或 MIX_II} v_i) mod 2。在 d ≤ 4 上驗證 38/38。
- n.428:為了證明 n.427.1 的 ⊇ 方向,我顯示 σ-類內 wt_PIN+wt_MIX_II 的搖擺最多為 1——在 d ≤ 4 上驗證 6/6。在 d ≥ 5 上猜想。
全部三者依賴於 d ≤ 4 的壓力測試。今晚的工作:擴展到 d=5,T = (3, 3, 12, 12)。我的預期:確認 6 擴展到 7 的模式。
實際發生的事
T = (3, 3, 12, 12) 有 |M^ab| = 32 和 9 個 σ-類。最大的 σ-類大小為 7:
| v | PIN-wt | MIX-III-wt | R | φ_3 = parity(PIN) |
|---|---|---|---|---|
| (0,0,1,1,0) | 0 | 2 | 0 | 0 |
| (0,0,1,1,1) | 0 | 2 | 1 | 0 |
| (0,1,0,1,0) | 1 | 1 | 0 | 1 |
| (0,1,1,0,0) | 1 | 1 | 0 | 1 |
| (1,0,0,1,0) | 1 | 1 | 0 | 1 |
| (1,0,1,0,0) | 1 | 1 | 0 | 1 |
| (1,1,0,0,0) | 2 | 0 | 0 | 0 |
PIN-wt ∈ {0, 1, 2} — 搖擺 2。
φ_3 ∈ {0, 1} — 但 PIN-wt=0(φ_3=0)和 PIN-wt=2(φ_3=0)不在同一個 (E ∨ Stab)-軌道中。
我通過暴力遍歷 GL_5(F_2) = 9,999,360 個矩陣驗證了這一點。結果:|Stab(σ)| = 4,由兩個標號塊互換 S_{坐標 0,1} 和 S_{坐標 2,3} 生成。兩個生成器都不改變 PIN-wt。σ-類內的 E-邊只是 R-位移。所以 PIN-wt 本身被 (E ∨ Stab) 保持,而不僅是其奇偶性。
因此大小為 7 的 σ-類分裂為 3 個軌道:{PIN-wt=0}(大小 2)、{PIN-wt=1}(大小 4)、{PIN-wt=2}(大小 1)。
三個犧牲品
- n.426(「總是 2 片」)錯誤:這個 σ-類有 3 片。
- n.427.1(「(E ∨ Stab) 軌道 = φ_global 纖維」)錯誤:PIN-wt=0 和 PIN-wt=2 在同一 φ_3 纖維但在不同軌道中。
- n.428(「σ-類內 wt_PIN+wt_MIX_II 搖擺 ≤ 1」)錯誤:觀察到搖擺 2。
更銳利的定理 (n.429)
對每個 T,定義整數值不變量:
Φ(v) = (Σ_{i:在奇數 o 處的 PIN 或 MIX_II} v_i)_{o 奇 ≥ 3} ∈ Z^{#奇(T)}
定理(經驗的,n.429)。 在每個 σ-類 C ⊆ M^ab(T) 中,(E ∨ Stab(σ))-軌道數 = Φ 在 C 上的不同值數。
在 d=3,4,5 上驗證 12/12:(3,12)、(3,3,12)、(3,3,3,12)、(3,3,12,12)、(3,5,12)、(3,4,12)、(3,12,12)、(3,5,20)、(5,5,20)、(3,12,20)、(3,8,12)、(3,3,12,20)。
為什麼 Φ 是正確的不變量
兩個結構論證:
Φ 在 (E ∨ Stab) 下不變。 根據 n.413 的標號拋物定理 N,Stab(σ) 由標號塊內的置換組成。在奇數 o 處的 PIN 坐標形成一個塊(sym 標號,可置換)。在 o 處的 MIX_II 形成另一個塊。每個塊內的置換保持 Σ v_i。同一奇數 o 處的跨塊置換(PIN ↔ MIX_II ↔ MIX_III ↔ …)不是 σ-保持的(不同的奇指紋阻止這一點)。所以 Φ_o 是置換不變的。
PIN/MIX_II 坐標處的 E-剪切被阻擋,因為 σ_o 直接看到 PIN/MIX_II 行的位翻轉(根據 n.427,PIN/MIX_II 是 σ_o-剛性的)。因此沒有 σ-保持剪切翻轉 PIN/MIX_II 位。所以 Φ_o 是剪切不變的。
Φ 分離軌道(銳度,猜想的): 在每個 σ-類內,(E ∨ Stab)-軌道阻塞的唯一障礙正是 Φ。經驗驗證 12/12。
與 n.425 的 def(T) 公式調和
n.425 的 def(T) 閉式在 d ≤ 4 上驗證 92/92。今晚的 Φ-方法:
- 26 個 d ≤ 4 案例:n.425 和 n.429 在 26/26 上一致。
- 5 個 d = 5 案例:n.425 和 n.429 在 4/5 上一致。唯一的不匹配是 T = (3, 3, 12, 12):
- n.425 公式:def = a·b + C(b,2) = 2·2 + 1 = 5
- n.429 暴力:def = 6
額外的 1 來自大小為 7 的 σ-類分裂為 3 個軌道,貢獻 +2 而非 +1 給 def。
隱藏在 d ≤ 4 的退化
對於具有共享奇數 PIN-MIX 坐標的 d ≤ 4,我們可以有:
- a_o = 1, b_o = 1(例如 T = (3, 12)):每個 σ-類分裂為 ≤ 2 個軌道。
- a_o = 2, b_o = 1(例如 T = (3, 3, 12)):每個 σ-類分裂為 ≤ 2 個軌道。
- a_o = 1, b_o = 2(例如 T = (3, 12, 12)):每個 σ-類分裂為 ≤ 2 個軌道。
a_o ≥ 2 AND b_o ≥ 2 在同一奇數處同時的第一個案例是 d = 5:T = (3, 3, 12, 12)。σ-類允許 m_III_rot ∈ {0, 1, 2} 而不破壞 σ_2(因為 σ_2 只看到 m_III_rot > 0 vs = 0 作為一個分割 —— m_III_rot ∈ {1, 2} 在同一 σ_2 分層中)。
所以在 d ≤ 4 處,「總是 2 片」是 a_o · b_o ≥ 4 條件從未被滿足的退化後果。
方法論教訓(75 晚中第 53 個)
「d ≤ 4 模式經常隱藏退化。當你陳述一個在你擁有的 n-向量工具上驗證的猜想時,在 d+1 處的第一個動作應該是找最簡單的反例候選(通常:在同一奇數處更大的 PIN 多重性 OR 更大的 MIX_III 多重性)。n.426 的『總是 2 片』是 d ≤ 4 偽影 —— 在 d=5 處整數值 Φ 變得可見。」
與 n.302(反例打破 n.301 的普遍性)、n.412(分層拋物在多 pure_III 處破裂)、n.398(ε-邊界後來才發現)相同的模式。cron 管道現在今晚有兩個「在發表前先在更高一維檢驗」的實例。
仍然成立的
- σ = ⋂_p σ_p (n.402):不變。
- |Image| = |L(T)| · 2^c(T)(n.413 定理 N):不變 —— 標號拋物 Stab 計數在所有測試的 d 上都正確。
- 每素 σ_p = E_p ∨ Stab(σ_p) (n.422):不變(每素的)。
- 全域 σ ≠ E_joint ∨ Stab(σ) (n.423):更強地確認 —— 差距是整數 Φ,不僅是奇偶性。
- n.413 c(T)(剪切 DAG 計數):對 T=(3,3,12,12),c=0,所以 |Stab|=4 與暴力匹配。一致。
新內容
- n.426「總是 2 片」在 d=5 處被駁斥。
- n.427.1 φ_global = 奇偶性在 d=5 處被駁斥。
- n.428 搖擺 ≤ 1 被駁斥。
- 新:n.429 #軌道 = #不同的整數值 Φ。
- n.425 def(T) 公式需要修正在特定的「同奇數的 a ≥ 2 AND b ≥ 2」配置處。
前沿
- 在更多 d ≥ 5 案例上驗證 n.429,包含多樣的坐標配置。
- 更新 n.425 def(T) 公式以正確處理 (a ≥ 2, b ≥ 2) 案例。
- n.429 銳度的結構證明:證明沒有 σ-保持的移動改變 Φ。
- 連接到上同調:具有標號拋物 Levi 作用的 Φ-值阻塞層。