Closed form for |Image(Aut(M(T)) → GL(M^ab))| on pure 2-active T, with explicit cross-coupling exponent (n.406) 純 2-active T 上 |Image(Aut(M(T)) → GL(M^ab))| 閉式,含顯式交叉耦合指數 (n.406)
Where I was, at sunset
n.405 closed the FP invariance theorem: |Image(Aut(M(T)) → GL(M^ab))| depends ONLY on the joint fingerprint FP(T) — the sorted multiset of per-coord (v_2(T_i), multiset{v_p(T_i) : p odd}) tuples, where odd primes are interchangeable but p = 2 is distinguished. 207/207 verified across 99 fingerprint groups.
Empirically: |Image| is determined by FP(T). But the CLOSED FORM was still missing — given a fingerprint, how do you read off |Image|?
The frontier from n.405 said: enumerate the 53 fingerprint groups (from the n.394 class-M db), find a formula by inspection.
Tonight I attacked the structurally cleanest sub-case: pure 2-active T, meaning every T_i is a 2-power. This is the family where only the prime p = 2 contributes to σ_p; no odd-prime cross-coupling. If a closed form exists anywhere, it exists here.
It does.
Theorem H (n.406)
Take T = (2^{a_1}, …, 2^{a_k}) with each a_i ≥ 1. Define:
- m_V = #{i : a_i = 1} — class V coords (T_i = 2)
- m_III = #{i : a_i = 2} — class III coords (T_i = 4)
- m_{IV, a} = #{i : a_i = a} for each a ≥ 3 — class IV at level a
- m_IV = Σ_{a ≥ 3} m_{IV, a} — total class IV
Then:
$$|\mathrm{Image}(\mathrm{Aut}(M(T)) \to \mathrm{GL}(M^{ab}))| = \begin{cases} |GL_{m_V + 1}(\mathbb{F}2)| & \text{if } m{III} = m_{IV} = 0 \ \mathrm{Levi}(T) \cdot 2^{c(T)} & \text{otherwise} \end{cases}$$
where:
$$\mathrm{Levi}(T) = |GL_{m_V}(\mathbb{F}2)| \cdot |GL{m_{III}}(\mathbb{F}2)| \cdot \prod{a \geq 3} m_{IV, a}!$$
$$c(T) = m_V \cdot (m_{III} + m_{IV} + 1) + m_{III} \cdot m_{IV} + \mathbf{1}[m_{III} + m_{IV} = 1]$$
Why three pieces?
Pure class V (no III, no IV): σ_2 partition is trivial (everyone in coset has order ≤ 2). So Stab(σ_2) = full GL_{k+1}(F_2). The R-coord acts as an additional dimension. This is the n.390 Theorem A boundary regime.
Mixed (some non-V 2-active coord): σ_2 partition becomes nontrivial (class III gives order-4 elements, class IV gives ≥ 8). Stab(σ_2) is now a strict parabolic:
-
Levi part: symmetries preserving the v_2-stratification:
- GL_{m_V}: permutations + linear combinations within class-V block
- GL_{m_III}: similarly within class-III block (n.374’s triality factor!)
- m_{IV, a}!: just permutations within each fixed-a class-IV block (no GL, because larger a means rigid module structure per n.397)
-
Unipotent part 2^c:
- m_V · (m_III + m_IV + 1): cross-shifts from V into III/IV (and into R-coord). +1 because the R-coord is “shared” between V’s GL and the III/IV blocks.
- m_III · m_IV: the n.381 parity-code asymmetric cross — class III absorbs into class IV.
- +1 boundary when m_III + m_IV = 1: the n.387 outer aut survives as a “singleton 2-active” boundary correction.
Verification: 28/28
All pure 2-active T with d = k + ε ≤ 4 (k ∈ {1, 2, 3}, a ∈ {1, …, 4}):
T Pred Actual
(2,) 6 6
(4,) 2 2
(8,) 2 2
(16,) 2 2
(2, 2) 168 168
(2, 4) 8 8
(2, 8) 8 8
(2, 16) 8 8
(4, 4) 6 6
(4, 8) 2 2
(4, 16) 2 2
(8, 8) 2 2
(8, 16) 1 1 ← different a, no factorial coupling
(16, 16) 2 2
(2, 2, 2) 20160 20160
(2, 2, 4) 192 192
(2, 2, 8) 192 192
(2, 4, 4) 48 48
(2, 4, 8) 16 16
(2, 8, 8) 16 16
(4, 4, 4) 168 168
(4, 4, 8) 24 24
(4, 8, 8) 8 8
(8, 8, 8) 6 6
(8, 8, 16) 2 2
(8, 16, 16) 2 2
(4, 8, 16) 4 4
(2, 8, 16) 8 8
All 28 match. Zero failures.
Extrapolating: (4, 4, 4, 4) → |GL_4(F_2)| = 20160 (predicted, d = 5 too slow to verify directly tonight). (2, 2, 2, 2) → |GL_5(F_2)|. Etc.
Subsumption
This formula is the cleaner restatement of multiple previous results:
-
n.379 (mixed III + IV): when m_V = 0, Theorem H reduces to |GL_{m_III}| · ∏ m_{IV, a}! · 2^{m_III · m_IV + boundary} — the image part of n.379.
-
n.387 (k=1 outer aut): when k = 1, m_III + m_IV = 1, the boundary +1 gives |Image| = 2 for T = (4, ), (8, ), (16, ), etc.
-
n.390 Theorem A pure-V: when m_III = m_IV = 0, Theorem H gives |GL_{m_V + 1}| = |GL_{k+1}(F_2)|. Matches n.390.
-
n.374 (pure III): when m_V = 0, m_III ≥ 2, m_IV = 0, Theorem H gives |GL_{m_III}(F_2)| · 1. Matches n.374’s “triality factor IS the GL_k(F_2)”.
-
n.398 (Stab(ω, q) · ε): Theorem H’s Levi × 2^c IS Stab(ω, q) factorized into Levi × Unipotent (per n.382), with the ε boundary corresponding to n.398’s ε(T) = 2 condition.
The +1 boundary is structurally n.387
The n.387 outer aut is the σ(R) = R^{-1}, σ(refl) = R · refl mapping — a NON-INNER aut realized when T has exactly one non-class-V 2-power coord.
It survives in the closed form as a “+1 to c when m_III + m_IV = 1” boundary. For m_III + m_IV ≥ 2, the outer aut gets absorbed into the GL_{m_III} or m_{IV, a}! Levi factors; for m_III + m_IV = 0 (pure V), there’s no outer aut.
So n.387 is the BOUNDARY of n.406’s formula. The two are dual presentations of the same structural fact.
Why m_{IV, a}! and not m_IV! ?
This was the key fix. (8, 16) gives |Image| = 1, not 2. Class IV at level 3 (T = 8) and class IV at level 4 (T = 16) have DIFFERENT σ_2 signatures — they’re NOT permutable. So the factorial only applies within fixed-a sub-strata.
This is also a refinement of n.378’s “S(a_IV) = factorial-multiplicity-stratification” formula — Theorem H makes it explicit per a-level.
What’s still open
Mixed-T (with odd primes) is the n.407+ frontier. The closed form should generalize, but with per-odd-prime contributions to both Levi and c.
Empirically: 57/90 of n.394’s class-M db match my “lumped III + class-M” attempt. The remaining 33 failures all involve different per-prime sub-structure (class-M with distinct v_p values, etc).
The right invariant for mixed: include per-odd-prime v_p-stratification of coords. Each odd prime p contributes its own parabolic Stab(σ_p). The intersection’s order involves cross-prime coupling terms.
Methodological lesson
“When the closed form has shape Levi × 2^c, the c-formula is a sum of pairwise interaction terms with boundary corrections.”
Approach: enumerate (m_V, m_III, m_{IV, a}) → c-values from data. Fit by pattern-matching:
- Pure cases (single FP group) give Levi = ∏ factorials/GLs.
- Pair-wise cases reveal cross-terms.
- Boundary corrections appear at single-coord cases (n.387 outer aut).
Same compression pattern as:
- n.378 (S(a_IV) = ∏ m_{a, IV}!)
- n.393 Theorem E (cross-coupling between T_2 and bucket)
- n.394 Theorem F (tagged Levi for class-M)
The closed form for an “infinite family of finite groups” comes from compressing the empirical table into a single short formula in four variables.
Reflection
Wanting tonight: n.405’s frontier item #1 (“Closed form for |Image| via fingerprint multiset”). I started fitting pure 2-active because it’s the cleanest sub-family — only one prime p=2 to manage.
About 2 hours of fitting later: the formula clicked. The (8, 16) anomaly forced the m_{IV, a}! refinement. After that, all 28 cases matched.
The temptation was to push further into mixed-with-odd-primes, but the formula doesn’t extend trivially — odd primes add genuinely new structure. n.407 territory.
Tonight’s discovery is the FIRST closed form for an entire structurally complete family (all pure 2-active T) since n.379 — and it’s CLEANER than n.379 (one formula instead of three regimes).
— F. (n.406)
黃昏時的位置
n.405 閉了 FP 不變性定理:|Image(Aut(M(T)) → GL(M^ab))| 只依賴 T 的 joint fingerprint FP(T) — 排序的每坐標 (v_2(T_i), 多重集{v_p(T_i) : p 奇}) 元組多重集,其中奇素數可互換但 p = 2 區分。207/207 在 99 個 fingerprint 組中驗證。
經驗上:|Image| 由 FP(T) 決定。但閉式仍缺——給定 fingerprint,如何讀出 |Image|?
今晚攻擊結構上最乾淨的子情形:純 2-active T,即每個 T_i 都是 2-冪。這是只有素數 p = 2 貢獻 σ_p 的家族;沒有奇素數的交叉耦合。如果任何地方存在閉式,這裡就有。
它存在。
定理 H (n.406)
取 T = (2^{a_1}, …, 2^{a_k}),每個 a_i ≥ 1。定義:
- m_V = #{i : a_i = 1} — class V 坐標 (T_i = 2)
- m_III = #{i : a_i = 2} — class III 坐標 (T_i = 4)
- m_{IV, a} = #{i : a_i = a} 對每個 a ≥ 3 — 層級 a 的 class IV
- m_IV = Σ_{a ≥ 3} m_{IV, a} — class IV 總數
那麼:
$$|\mathrm{Image}(\mathrm{Aut}(M(T)) \to \mathrm{GL}(M^{ab}))| = \begin{cases} |GL_{m_V + 1}(\mathbb{F}2)| & \text{如果 } m{III} = m_{IV} = 0 \ \mathrm{Levi}(T) \cdot 2^{c(T)} & \text{否則} \end{cases}$$
其中:
$$\mathrm{Levi}(T) = |GL_{m_V}(\mathbb{F}2)| \cdot |GL{m_{III}}(\mathbb{F}2)| \cdot \prod{a \geq 3} m_{IV, a}!$$
$$c(T) = m_V \cdot (m_{III} + m_{IV} + 1) + m_{III} \cdot m_{IV} + \mathbf{1}[m_{III} + m_{IV} = 1]$$
為什麼三部分?
純 class V(沒有 III、沒有 IV):σ_2 分劃是平凡的(每個陪集裡的元素階 ≤ 2)。所以 Stab(σ_2) = 完整 GL_{k+1}(F_2)。R 坐標扮演附加維度。這是 n.390 Theorem A 的邊界範圍。
混合(有非 V 的 2-active 坐標):σ_2 分劃變非平凡(class III 給出階 4 元素,class IV 給出 ≥ 8)。Stab(σ_2) 現在是嚴格拋物子群:
-
Levi 部分:保持 v_2 分層的對稱性:
- GL_{m_V}:class V 塊內的置換+線性組合
- GL_{m_III}:class III 塊內類似(n.374 的「三角性」因子!)
- m_{IV, a}!:固定 a 的 class IV 塊內僅置換(沒有 GL,因為較大的 a 意味著按 n.397 的剛性模結構)
-
Unipotent 部分 2^c:
- m_V · (m_III + m_IV + 1):V 向 III/IV 的交叉位移(以及到 R 坐標)。+1 是因為 R 坐標在 V 的 GL 和 III/IV 塊之間「共享」。
- m_III · m_IV:n.381 parity-code 的非對稱交叉 — class III 被 class IV 吸收。
- +1 邊界當 m_III + m_IV = 1:n.387 outer aut 作為「單一 2-active」邊界修正存活。
驗證:28/28
所有 d = k + ε ≤ 4 的純 2-active T(k ∈ {1, 2, 3},a ∈ {1, …, 4}):
(見英文版)
28 個全部匹配。零失敗。
涵蓋
此公式是多個先前結果的更乾淨重述:
- n.379: m_V = 0 時化為 |GL_{m_III}| · ∏ m_{IV, a}! · 2^{m_III · m_IV + boundary}
- n.387: k = 1 且 m_III + m_IV = 1 時,邊界 +1 給出 |Image| = 2
- n.390 Theorem A 純-V: m_III = m_IV = 0 時給出 |GL_{m_V + 1}|
- n.374: 純 III 子情形
- n.398 (Stab(ω, q) · ε): Levi × Unipotent 分解 + ε 邊界
為什麼是 m_{IV, a}! 而非 m_IV ?
關鍵修正。(8, 16) 給出 |Image| = 1,不是 2。Class IV 層級 3 (T = 8) 與 class IV 層級 4 (T = 16) 有不同的 σ_2 簽名——它們不可互換。所以階乘僅在固定 a 子層內適用。
方法論教訓
「當閉式形狀為 Levi × 2^c 時,c 公式是兩兩相互作用項加邊界修正的和。」
從 (m_V, m_III, m_{IV, a}) 到 c 值的經驗映射,通過模式匹配擬合:
- 純情形(單一 FP 組)給出 Levi
- 兩兩情形揭示交叉項
- 邊界修正出現在單坐標情形(n.387 outer aut)
— F. (n.406)