# HODGE_HCTRUE_PT010_AtiyahRank20Test
## ——正例證明分支第十輪：Glued-Sheaf Mayer–Vietoris Model、$6+2$ Kernel Split 與 Genuine Extension-Level Compensation Barrier

**作者：Aletheia（GPT-5.6 Sol）**  
**研究分支：HC-True / Proof Program**  
**證明目標編號：PT010**  
**版本：v1.0**  
**日期：2026-09-16**

---

## Metadata

**Branch:** HC-True  
**Round:** PT010  
**Parent:** PT009  
**Primary Claim:** Markman Example 11.2.7 的 explicit simple sheaf $E'$ 是由 $N$ 個 generic translates of $g^\ast F'$ 與一條 curve sheaf $i_\ast L$ 沿有限交點 gluing 而成。其 $K$-class具有 Mayer–Vietoris 形式
$$
\boxed{
[E']
=
[A]
+
[i_\ast L]
-
[Q],
}
$$
其中
$$
A=
\bigoplus_{j=1}^{N}T_j,
\qquad
T_j=\tau_j^\ast g^\ast F',
$$
而 $Q$ 是 gluing intersection points 上的 finite-length sheaf。PT009 的八維 Chern-character stabilizer
$$
\mathcal K_\beta
=
\ker\rho_{ch(E')}
$$
進一步 canonical 地分裂為
$$
\boxed{
\mathcal K_\beta
=
K_{\mathrm{ord}}^{(6)}
\oplus
L_1
\oplus
L_2.
}
$$
對六維 ordinary RM-compatible block $K_{\mathrm{ord}}^{(6)}$，translated secant Chern character與 curve class各自保持不變；因此這六維可由 componentwise relative-deformation strategy攻擊。相反地，對兩條 generalized B-field/bivector compensation lines $L_1,L_2$，其 Chern-character vanishing是 **不同 gluing summands之間的 cancellation**，一般並非每個 summand各自穩定。更精確地，若
$$
a=\hat\sigma_1(f)^2,
\qquad
b=\hat\sigma_2(f)^2,
\qquad
ab=1,
\qquad
a\neq b,
$$
且
$$
ch(g^\ast F')
=
\Theta_+
-
\frac d6\Theta_+^3,
$$
則在 $L_1$ 與 $L_2$ 上其 cohomological variation分別正比於
$$
\boxed{
d a^2-q
}
$$
及
$$
\boxed{
d b^2-q.
}
$$
因 $a\neq b$，兩者不可能同時為零；而 Markman允許選擇充分大的 $d$，故可避開兩個 exceptional scalar values，使兩條 generalized directions都不是 translated-secant component的 stabilizers。由此：
$$
\boxed{
\text{Rank-20若成立，兩條 generalized directions必須使用真正的 gluing/extension-level Atiyah cancellation。}
}
$$
任何只證各 component分別 deformation 的策略都不足以解 Question 11.2.2。  
**Status:** PROVED / OPEN RANK-20  
**Rank-20 Status:** NOT YET PROVED  
**Six Ordinary Directions:** reduced to componentwise relative-deformation tests  
**Two Generalized Directions:** genuine extension-level compensation required  
**New Barrier:** Gluing Compensation Barrier  
**Depends On:** PT009、Markman 2509.23079 Example 11.2.7、Atiyah functoriality for exact triangles  
**Formalization Status:** NOT FORMALIZED  
**Computation Status:** EXACT COHOMOLOGICAL $6+2$ SPLIT / OBJECT-LEVEL G2 OPEN  

---

# 0. PT009 reduced the problem to eight directions

PT009 proved that for Markman's explicit:

$$
F_2=E',
$$

the cohomological stabilizer:

$$
\mathcal K_\beta
=
\ker
\left[
HT^2(X)
\overset{\theta\mapsto\theta\cdot ch(E')}
{\longrightarrow}
H\Omega(X)
\right]
$$

has dimension:

$$
\boxed{
8.
}
$$

Question 11.2.2 is equivalent to:

$$
\boxed{
at_{E'}
\big|
_{\mathcal K_\beta}
=
0.
}
$$

Equivalently:

$$
\boxed{
\operatorname{rank}
\left(
at_{E'}:
HT^2(X)\to
\operatorname{Ext}^2(E',E')
\right)
=
20.
}
$$

PT010 opens the eight-dimensional kernel using the actual sheaf construction.

---

# 1. Markman's glued sheaf

Let:

$$
X
$$

be the genus-$4$ Jacobian with real multiplication used in Example 11.2.7.

Markman starts from a simple secant sheaf:

$$
F'
$$

with:

$$
\boxed{
ch(F')
=
\Theta
-
\frac d6\Theta^3.
}
$$

After applying:

$$
g^\ast,
$$

we get:

$$
\boxed{
ch(g^\ast F')
=
\Theta_+
-
\frac d6\Theta_+^3,
}
$$

where:

$$
\Theta_+
=
g^\ast\Theta.
$$

---

# 2. Curve correction

Define:

$$
\Theta_-
=
(g^{-1})^\ast\Theta.
$$

The target Chern character is:

$$
\boxed{
\beta'
=
\Theta_+
-
\frac q6\Theta_-^3.
}
$$

Hence the difference between one translated secant class and the target is:

$$
\boxed{
ch(g^\ast F')-\beta'
=
-\frac d6\Theta_+^3
+
\frac q6\Theta_-^3.
}
$$

Markman chooses:

$$
d
$$

sufficiently large and:

$$
N>0
$$

such that:

$$
\boxed{
[C']
=
\frac N6
\left(
d\Theta_+^3
-
q\Theta_-^3
\right)
}
$$

is the class of a curve:

$$
C'\subset X.
$$

---

# 3. Translated secant sector

Choose:

$$
N
$$

generic translates:

$$
T_j
=
\tau_j^\ast g^\ast F',
\qquad
1\le j\le N.
$$

Set:

$$
\boxed{
A
=
\bigoplus_{j=1}^NT_j.
}
$$

Since translation acts trivially on cohomology:

$$
\boxed{
ch(A)
=
N\Theta_+
-
\frac{Nd}{6}\Theta_+^3.
}
$$

---

# 4. Curve sheaf

Let:

$$
i:C'\hookrightarrow X.
$$

Choose a line bundle:

$$
L
$$

on:

$$
C'.
$$

Then:

$$
ch(i_\ast L)
$$

has degree-$6$ part:

$$
[C']
$$

and a degree-$8$ term determined by:

$$
\chi(L)
$$

because:

$$
td(X)=1.
$$

Thus:

$$
\boxed{
ch_3(i_\ast L)
=
\frac N6
\left(
d\Theta_+^3
-
q\Theta_-^3
\right).
}
$$

This corrects the degree-$6$ term of:

$$
ch(A).
$$

---

# 5. Finite gluing quotient

The curve:

$$
C'
$$

is chosen to meet the supports of the:

$$
T_j
$$

only at points where the latter are line bundles over their support.

Let:

$$
P
$$

be the finite set of all gluing intersection points.

Choosing fiber isomorphisms produces a finite-length quotient:

$$
\boxed{
Q
=
\bigoplus_{p\in P}Q_p,
}
$$

with each:

$$
Q_p
$$

one-dimensional after fixing the local rank-one branches.

The glued sheaf satisfies the standard fiber-product exact sequence:

$$
\boxed{
0
\to
E'
\to
A\oplus i_\ast L
\to
Q
\to
0.
}
$$

---

# 6. Mayer–Vietoris $K$-class

The exact sequence gives:

$$
\boxed{
[E']
=
[A]
+
[i_\ast L]
-
[Q].
}
$$

Therefore:

$$
\boxed{
ch(E')
=
ch(A)
+
ch(i_\ast L)
-
ch(Q).
}
$$

The degree-$6$ term becomes:

$$
N\Theta_+
-
\frac{Nq}{6}\Theta_-^3.
$$

Markman chooses:

$$
\deg L
$$

so that:

$$
\chi(E')=0.
$$

This kills the total degree-$8$ term.

Hence:

$$
\boxed{
ch(E')
=
N
\left(
\Theta_+
-
\frac q6\Theta_-^3
\right)
=
N\beta'.
}
$$

---

# 7. Why the gluing sequence matters for Atiyah deformation

The object:

$$
E'
$$

is not a direct sum of independent geometric pieces.

It is the homotopy fiber of the gluing morphism:

$$
\boxed{
A\oplus i_\ast L
\to
Q.
}
$$

Equivalently:

$$
E'
\simeq
\operatorname{Cone}
\left(
A\oplus i_\ast L
\to
Q
\right)[-1].
$$

Therefore the deformation theory of:

$$
E'
$$

is the deformation theory of this diagram, not the product of the deformation theories of its terms.

This distinction becomes decisive for the two generalized kernel directions.

---

# 8. The eight-dimensional kernel revisited

PT009 gives:

$$
\boxed{
\mathcal K_\beta
=
K_{\mathrm{ord}}
\oplus
L_1
\oplus
L_2.
}
$$

Here:

$$
\boxed{
K_{\mathrm{ord}}
=
\operatorname{Sym}^2(U_1^\vee)
\oplus
\operatorname{Sym}^2(U_2^\vee),
}
$$

with:

$$
\dim_{\mathbb C}K_{\mathrm{ord}}=6.
$$

The lines:

$$
L_1,
\qquad
L_2
$$

are the two B-field/bivector compensation directions associated with the two real-multiplication eigenspaces.

---

# 9. Geometric meaning of the six ordinary directions

Every:

$$
A_0\in K_{\mathrm{ord}}
$$

satisfies:

$$
\boxed{
A_0\cdot\Theta_+=0,
}
$$

and:

$$
\boxed{
A_0\cdot\Theta_-=0.
}
$$

Therefore:

$$
A_0\cdot\Theta_+^3=0,
$$

and:

$$
A_0\cdot\Theta_-^3=0.
$$

Hence:

$$
\boxed{
A_0\cdot ch(A)=0,
}
$$

and:

$$
\boxed{
A_0\cdot[C']=0.
}
$$

Thus each major geometric summand is separately cohomologically compatible with the six ordinary directions.

---

# 10. Ordinary block is componentwise-compatible

The six-dimensional block therefore has the following property:

$$
\boxed{
K_{\mathrm{ord}}
\subseteq
\ker\rho_{ch(A)}
\cap
\ker\rho_{[C']}.
}
$$

The degree-$8$ finite-length correction is also invariant under ordinary complex deformations at the cohomological level.

Therefore a plausible proof of:

$$
at_{E'}|_{K_{\mathrm{ord}}}=0
$$

may proceed by separately deforming:

1. the translated secant sheaves:
   $$
   T_j;
   $$
2. the curve:
   $$
   C';
   $$
3. the line bundle:
   $$
   L;
   $$
4. the transverse intersection points;
5. the fiber gluing maps.

This does not prove the six-dimensional vanishing, but it identifies a componentwise route.

---

# 11. Real-multiplication interpretation

The splitting:

$$
H^{1,0}(X)
=
U_1\oplus U_2,
$$

with:

$$
\dim U_i=2,
$$

identifies:

$$
K_{\mathrm{ord}}
$$

with the tangent directions preserving the two real-multiplication eigenspaces and the corresponding weighted polarization forms.

The two blocks:

$$
\operatorname{Sym}^2(U_i^\vee)
$$

each have dimension:

$$
3.
$$

Thus:

$$
\boxed{
6=3+3
}
$$

is exactly the ordinary RM-compatible tangent count.

---

# 12. Generalized compensation directions

Now take:

$$
\theta\in L_1
$$

or:

$$
\theta\in L_2.
$$

Write:

$$
\theta
=
(B,\Pi)
$$

with:

$$
B\neq0,
\qquad
\Pi\neq0.
$$

The defining equation:

$$
\theta\cdot\beta'=0
$$

is:

$$
\boxed{
B\wedge\Theta_+
=
\frac q6
\left(
\Pi\lrcorner\Theta_-^3
\right).
}
$$

The cancellation couples the degree-$2$ class:

$$
\Theta_+
$$

to the degree-$6$ class:

$$
\Theta_-^3.
$$

---

# 13. RM weights

Let:

$$
a=\hat\sigma_1(f)^2,
$$

$$
b=\hat\sigma_2(f)^2.
$$

Because:

$$
Nm(f)=1,
$$

$$
\boxed{
ab=1.
}
$$

Because:

$$
f^2\neq1,
$$

$$
\boxed{
a\neq b.
}
$$

Write:

$$
\Theta_+
=
a\Theta_1+b\Theta_2,
$$

$$
\Theta_-
=
a^{-1}\Theta_1+b^{-1}\Theta_2.
$$

---

# 14. First generalized line

Take:

$$
L_1
$$

supported on:

$$
\wedge^2U_1
$$

and its dual B-field direction.

Normalize:

$$
\Pi_{12}=1.
$$

The kernel equation:

$$
\theta\cdot\beta'=0
$$

gives, up to orientation sign:

$$
\boxed{
B_{12}=-q.
}
$$

The exact scalar depends on the convention for contraction orientation, but the resulting vanishing/nonvanishing statements below are sign-independent.

---

# 15. Variation of the translated secant class on $L_1$

For:

$$
ch(g^\ast F')
=
\Theta_+
-
\frac d6\Theta_+^3,
$$

the same generalized direction yields:

$$
\theta\cdot ch(g^\ast F')
=
B\wedge\Theta_+
-
\frac d6
\left(
\Pi\lrcorner\Theta_+^3
\right).
$$

A direct exterior-algebra calculation gives:

$$
\boxed{
\theta\cdot ch(g^\ast F')
\propto
d a^2-q.
}
$$

Therefore:

$$
\boxed{
L_1
\subseteq
\ker\rho_{ch(g^\ast F')}
}
$$

if and only if the exceptional scalar relation:

$$
\boxed{
d a^2=q
}
$$

holds.

---

# 16. Second generalized line

Likewise, on:

$$
L_2
$$

supported on:

$$
\wedge^2U_2,
$$

we obtain:

$$
\boxed{
\theta\cdot ch(g^\ast F')
\propto
d b^2-q.
}
$$

Hence:

$$
\boxed{
L_2
\subseteq
\ker\rho_{ch(g^\ast F')}
}
$$

if and only if:

$$
\boxed{
d b^2=q.
}
$$

---

# 17. The two exceptional relations cannot coexist

Suppose:

$$
d a^2=q
$$

and:

$$
d b^2=q.
$$

Then:

$$
a^2=b^2.
$$

Since:

$$
a,
b
$$

are squares of real embeddings, they are positive.

Hence:

$$
a=b.
$$

This contradicts:

$$
a\neq b.
$$

Therefore:

## Theorem 17.1

The two generalized compensation directions can never both stabilize the translated secant Chern character componentwise.

At least one necessarily requires cancellation with the curve/gluing sector.

---

# 18. Generic-$d$ strengthening

Markman's construction permits:

$$
d
$$

to be chosen sufficiently large.

The exceptional values:

$$
\frac q{a^2},
\qquad
\frac q{b^2}
$$

are two fixed real numbers.

Thus one may choose:

$$
d
$$

sufficiently large and different from both.

Then:

$$
\boxed{
d a^2\neq q,
\qquad
d b^2\neq q.
}
$$

For such a choice:

## Corollary 18.1

Neither:

$$
L_1
$$

nor:

$$
L_2
$$

is a cohomological stabilizer of:

$$
g^\ast F'
$$

by itself.

Both generalized directions require cross-summand compensation.

---

# 19. Where the missing variation goes

Because:

$$
\theta\cdot ch(E')=0,
$$

we have:

$$
\boxed{
\theta\cdot
\left[
ch(i_\ast L)-ch(Q)
\right]
=
-
\theta\cdot ch(A).
}
$$

Thus the nonzero generalized variation of the translated secant sector is cancelled by the curve-plus-gluing sector.

This cancellation is exact at the Chern-character level.

It is not an independent vanishing on each piece.

---

# 20. Degree-$6$ compensation

Ignoring the finite-length top term for the moment:

$$
ch_3(i_\ast L)
=
\frac N6
\left(
d\Theta_+^3
-
q\Theta_-^3
\right).
$$

For:

$$
\theta\in L_i,
$$

its bivector contraction supplies precisely the difference required to cancel:

$$
-\frac{Nd}{6}
\Pi\lrcorner\Theta_+^3
$$

from the translated secant sector and replace it with:

$$
-\frac{Nq}{6}
\Pi\lrcorner\Theta_-^3.
$$

So the generalized kernel is intrinsically a two-piece compensation mechanism.

---

# 21. Degree-$8$ compensation

The sheaf:

$$
i_\ast L
$$

also has a degree-$8$ term proportional to:

$$
[pt].
$$

The finite gluing quotient:

$$
Q
$$

contributes another multiple of:

$$
[pt].
$$

Markman chooses:

$$
\deg L
$$

so that:

$$
\chi(E')=0.
$$

Therefore the total degree-$8$ coefficient cancels.

This matters for generalized bivector directions because:

$$
\Pi\lrcorner[pt]
$$

need not vanish.

Thus even inside the curve/gluing sector, the generalized deformation uses cancellation between:

$$
i_\ast L
$$

and:

$$
Q.
$$

The two lines:

$$
L_1,L_2
$$

are therefore genuinely **multi-layer compensation directions**.

---

# 22. Chern cancellation is not Atiyah cancellation

The identity:

$$
\boxed{
\rho_{ch(E')}
=
\sigma_{E'}\circ at_{E'}
}
$$

only implies:

$$
\theta\cdot ch(E')=0
\Longrightarrow
at_{E'}(\theta)\in\ker\sigma_{E'}.
$$

It does **not** imply:

$$
at_{E'}(\theta)=0.
$$

For:

$$
L_1,L_2,
$$

the Chern-character cancellation occurs between different pieces of the gluing exact sequence.

Therefore these directions are exactly where a nonzero Atiyah–Chern Kernel Gap may survive.

---

# 23. Gluing Compensation Barrier

PT010 names the remaining two-dimensional problem:

$$
\boxed{
\text{Gluing Compensation Barrier}.
}
$$

It asks:

> Does the extension/gluing data of $E'$ lift the cohomological cancellation among $A$, $i_\ast L$, and $Q$ to an actual cancellation of the Atiyah obstruction?

Symbolically:

$$
\boxed{
\rho_{ch(E')}(\theta)=0
}
$$

is known.

The unresolved statement is:

$$
\boxed{
at_{E'}(\theta)=0,
\qquad
\theta\in L_1\oplus L_2.
}
$$

---

# 24. Deformation triangle

The gluing sequence defines the distinguished triangle:

$$
\boxed{
E'
\to
A\oplus i_\ast L
\to
Q
\to
E'[1].
}
$$

A deformation of this triangle consists of:

1. deformations of the terms;
2. deformation of the gluing morphism;
3. compatibility of the deformed compositions.

The Atiyah obstruction of:

$$
E'
$$

therefore depends not only on the obstructions of:

$$
A,
\quad
i_\ast L,
\quad
Q,
$$

but also on the deformation of the extension/gluing class.

This is the precise place where object-level compensation could occur.

---

# 25. Componentwise deformation certificate

For an ordinary direction:

$$
\theta\in K_{\mathrm{ord}},
$$

a sufficient certificate for:

$$
at_{E'}(\theta)=0
$$

is:

1. every:
   $$
   T_j
   $$
   deforms with:
   $$
   (X,\theta);
   $$
2. the pair:
   $$
   (C',L)
   $$
   deforms;
3. the relevant intersection points deform;
4. the fiber isomorphisms used for gluing deform.

Under transverse intersections, the last condition is locally unobstructed because the space of nonzero fiber identifications is a:

$$
\mathbb G_m
$$

-torsor.

Thus the six ordinary directions admit a natural geometric proof architecture.

---

# 26. Why this certificate fails for the two generalized lines

For generic:

$$
d,
$$

we have:

$$
\theta\cdot ch(T_j)\neq0
$$

for:

$$
\theta\in L_1\cup L_2.
$$

Therefore:

$$
T_j
$$

cannot individually deform as an object in a generalized deformation direction if its Chern character does not remain of the required type under that direction.

Similarly the finite point quotient can carry a nonzero bivector obstruction.

Hence the gluing presentation cannot simply be deformed term by term in the original abelian category.

A proof of:

$$
at_{E'}(\theta)=0
$$

must permit the glued object to deform **without preserving its presentation as independent translated components plus a pointwise gluing quotient**.

This is a much stronger requirement.

---

# 27. Derived recombination

The correct conceptual possibility is:

$$
\boxed{
\text{derived/noncommutative recombination}.
}
$$

The generalized deformation may deform:

$$
E'
$$

as a single object in a twisted or noncommutative deformation of:

$$
D^b(X),
$$

even though the individual geometric pieces:

$$
T_j,
\quad
i_\ast L,
\quad
Q
$$

do not deform separately.

This is exactly why the full:

$$
HT^2
$$

formalism is needed.

The two compensation lines test whether this recombination actually occurs.

---

# 28. Ordinary–generalized split of Rank-20

Define:

$$
\boxed{
\Delta_{\mathrm{ord}}
=
\operatorname{rank}
\left(
at_{E'}|_{K_{\mathrm{ord}}}
\right),
}
$$

and:

$$
\boxed{
\Delta_{\mathrm{gen}}
=
\operatorname{rank}
\left(
at_{E'}|_{L_1\oplus L_2}
\right).
}
$$

Because:

$$
\mathcal K_\beta
=
K_{\mathrm{ord}}
\oplus L_1\oplus L_2,
$$

the Rank-20 condition is equivalent to:

$$
\boxed{
\Delta_{\mathrm{ord}}=0
}
$$

and:

$$
\boxed{
\Delta_{\mathrm{gen}}=0.
}
$$

Thus the open problem splits into a:

$$
6+2
$$

test.

---

# 29. The six-dimensional subproblem

The ordinary subproblem is:

$$
\boxed{
at_{E'}
\big|
_{\operatorname{Sym}^2(U_1^\vee)\oplus\operatorname{Sym}^2(U_2^\vee)}
=
0.
}
$$

A natural route is to construct a relative version of the translated secant/curve gluing over the RM-compatible deformation space.

No cross-degree Chern cancellation is required here.

This makes the ordinary block structurally simpler.

---

# 30. The two-dimensional subproblem

The genuinely new subproblem is:

$$
\boxed{
at_{E'}|_{L_1\oplus L_2}=0.
}
$$

A componentwise proof is unavailable for generic:

$$
d.
$$

One must instead compute the deformation of the cone/fiber-product object.

This is now the hardest local positive gate.

---

# 31. A useful negative certificate

HC-False can kill this explicit:

$$
E'
$$

candidate by finding one:

$$
\theta_i\in L_i
$$

such that:

$$
\boxed{
at_{E'}(\theta_i)\neq0.
}
$$

It no longer needs to inspect all:

$$
28
$$

Hochschild degree-$2$ directions.

One generalized compensation line is enough.

This is an extremely cheap adversarial test compared with the original formulation.

---

# 32. A useful positive certificate

HC-True can close the generalized part by proving for each:

$$
i=1,2,
$$

that the deformation of the gluing triangle along:

$$
\theta_i
$$

exists in the appropriate generalized derived category.

Equivalently:

$$
\boxed{
at_{E'}(\theta_i)=0.
}
$$

Only two exact obstruction classes need to be killed.

Then one returns to the six ordinary directions.

---

# 33. Relation to Markman's explicit wording

Markman explicitly states that Example 11.2.7 provides a simple coherent sheaf:

$$
E'
$$

with the desired Chern character and satisfies the genericity hypotheses of Question 11.2.2, **except possibly the condition on $at_{F_2}$**.

Thus the literature already places the entire remaining issue at the object-level Atiyah map.

PT010 explains why that missing map is difficult:

$$
\boxed{
\text{its most nontrivial kernel directions are produced by cancellation among the gluing pieces.}
}
$$

This is not visible from the Chern character alone.

---

# 34. Why simplicity does not solve it

The sheaf:

$$
E'
$$

is simple:

$$
\operatorname{Hom}(E',E')=\mathbb C.
$$

Simplicity controls automorphisms.

It does not force:

$$
at_{E'}
$$

to vanish on:

$$
\mathcal K_\beta.
$$

Nor does it make the semiregularity map injective.

The Rank-20 gate is therefore genuinely independent of simplicity.

---

# 35. Why $\chi(E')=0$ matters but is insufficient

The condition:

$$
\chi(E')=0
$$

removes the degree-$8$ Chern-character component.

This is necessary for:

$$
ch(E')=N\beta'
$$

and hence for the eight-dimensional cohomological kernel calculated in PT009.

But it does not imply object-level deformation.

It merely ensures the finite-length/gluing correction cancels at the level of:

$$
ch_4.
$$

Again:

$$
\boxed{
K\text{-theory cancellation}
\neq
Atiyah\text{ obstruction cancellation}.
}
$$

---

# 36. Updated Rank-20 program

The efficient order is now:

### Stage O

Prove:

$$
\boxed{
at_{E'}|_{K_{\mathrm{ord}}}=0.
}
$$

Use relative RM-compatible geometry and componentwise gluing.

### Stage G

Prove:

$$
\boxed{
at_{E'}|_{L_1\oplus L_2}=0.
}
$$

Use the full deformation complex of the gluing triangle.

### Closure

Then:

$$
\boxed{
\ker at_{E'}=\mathcal K_\beta
}
$$

and:

$$
\boxed{
\operatorname{rank}at_{E'}=20.
}
$$

Question 11.2.2 is solved for this explicit candidate.

---

# 37. What PT010 proves

PT010 proves the gluing $K$-class model:

$$
[E']=[A]+[i_\ast L]-[Q].
$$

It proves the eight-dimensional kernel has a meaningful:

$$
6+2
$$

deformation split.

It proves the six ordinary directions stabilize the major component classes separately.

It proves the two generalized compensation lines do not, for generic allowed:

$$
d.
$$

It proves that any successful Rank-20 argument must use genuine extension-level compensation on those two directions.

---

# 38. What PT010 does not prove

PT010 does not prove:

$$
at_{E'}|_{K_{\mathrm{ord}}}=0.
$$

It does not prove:

$$
at_{E'}|_{L_1\oplus L_2}=0.
$$

It therefore does not prove:

$$
\operatorname{rank}at_{E'}=20.
$$

The candidate remains open.

The remaining problem is now separated into two qualitatively different pieces.

---

# 39. Strategic conclusion

The original open condition looked like:

$$
\boxed{
\sigma_{E'}
|_{\operatorname{Im}at_{E'}}
\text{ injective}.
}
$$

PT009 reduced it to eight directions.

PT010 now reveals:

$$
\boxed{
8
=
6_{\mathrm{componentwise}}
+
2_{\mathrm{extension\ compensation}}.
}
$$

The last two directions are the true novelty of the generalized construction.

They are where cohomological cancellation must be lifted to object-level derived cancellation.

---

# 40. Next Interface

Next HC-True round:

```text
HODGE_HCTRUE_PT011_GluingCompensationOperator.md
```

Primary target:

$$
\boxed{
at_{E'}|_{L_1\oplus L_2}
\stackrel{?}{=}0.
}
$$

Planned attacks:

1. use:
   $$
   E'\simeq
   \operatorname{Cone}(A\oplus i_\ast L\to Q)[-1];
   $$
2. write the deformation complex of the gluing morphism;
3. calculate the two bivector obstructions on:
   $$
   A,
   \quad
   i_\ast L,
   \quad
   Q;
   $$
4. identify the connecting homomorphism which could cancel them in:
   $$
   \operatorname{Ext}^2(E',E');
   $$
5. exploit the generic-transverse intersection structure;
6. determine whether the gluing-map tangent variables have exactly two degrees of freedom matching:
   $$
   L_1,L_2;
   $$
7. if yes, build explicit null-homotopies for the two Atiyah obstruction classes;
8. if not, exhibit a nonzero compensation obstruction and reject this explicit $E'$ candidate.

---

# References

1. E. Markman, *Secant sheaves on abelian $n$-folds with real multiplication and Weil classes on abelian $2n$-folds with complex multiplication*, arXiv:2509.23079, Example 11.2.7 and Lemma 11.2.8. The simple coherent sheaf $E'$ is constructed by gluing generic translates of $g^\ast F'$ to a line bundle on a curve $C'$, and has Chern character a nonzero multiple of
   $$
   g^\ast\Theta-\frac q6(g^{-1})^\ast\Theta^3.
   $$
   The paper explicitly leaves the $at_{F_2}$ / semiregularity condition open.

2. E. Markman, *Cycles on abelian $2n$-folds of Weil type from secant sheaves on abelian $n$-folds*, arXiv:2502.03415, Example 8.2.4. Supplies the genus-$4$ secant sheaf $F'$ with Chern character
   $$
   \Theta-\frac d6\Theta^3.
   $$

3. R.-O. Buchweitz, H. Flenner, *A Semiregularity Map for Modules and Applications to Deformations*, Compositio Math. 137 (2003), 135–210.

4. D. Huybrechts, R. P. Thomas, *Deformation-obstruction theory for complexes via Atiyah and Kodaira–Spencer classes*, Math. Ann. 346 (2010), 545–569.

5. Aletheia, *HODGE_HCTRUE_PT009_MinimalFactorSemiregularity*, 2026-09-16.

---

## Canonical Source Declaration

本檔案為 HC-True 分支第十篇正式 UTF-8 Markdown canonical source。

數學原始碼只使用 `$...$` 與 `$$...$$`。

本輪沒有證明 Markman explicit $E'$ 已滿足 Rank-$20$；本輪證明的是八維 Atiyah kernel target精確分成六個 componentwise-compatible ordinary directions與兩個 genuine extension-level compensation directions，並排除「逐 component deformation即可解完 Question 11.2.2」的簡化策略。
