The First Joint Conductor--Elliptic--Soft Cospan Corner Closes
Question
Entry 367 replaced strict Cut--nearby commutation by a filtered cospan whose unique common geometric line is (e_6). The first hostile support test is where the total-energy elliptic node, both conductor discriminants, and one site-soft normal meet. The hard-to-vary claim tested here is
We compute the iterated nearby object
The (x=0, y\ne0) branch follows by the frozen source involution. The simultaneous double-soft point is not included.
Conductor behavior
At (E=0), the exact conductor discriminants of Entry 307 become
Both vanish to order two. Therefore each Kummer connection restricts to
with integral residue and trivial semisimple monodromy around (t=0):
Thus the conductor collision introduces no new character. Its integral half-sum lattice remains the existing ((\mathbb Z/2)^2) occurrence saturation.
Logarithmic cospan leg
At (E=0), put
After multiplying the two wall columns by their source-derived soft Rees normal (t), and stripping only units on (x(x+t)\ne0), integral representatives are
At (t=0), the minor on rows ((e_4,e_2,e_6)) is
a unit on the chosen generic soft branch. Hence the regularized logarithmic leg retains rank three and has no additional soft invariant factor.
Cut--nearby cospan leg
In enhanced coordinates, the physical Cut leg is
Its ordinary special fiber has rank two, while its exact Rees/Smith type is
The missing ordinary direction survives at the next (t)-grade. No new torsion prime or irreducible support factor occurs.
Bridge and elliptic typing
The ordinary special logarithmic span uses
while the ordinary Cut span uses ((e_5,e_6)). Their intersection remains
Thus the second-Rees bridge of Entry 367 survives the joint corner in ordinary grade zero.
Entry 352 independently proves that the soft principal parts of the marked rank-twelve columns have zero infinity-Gysin image. Therefore the joint corner creates no new marked-to-elliptic supported extension. This does not compute the pure elliptic variation at the further soft degeneration; it keeps that block separate.
Verdict
The tested failure claim is falsified on the first individual soft branch:
with the independent elliptic block and no new carrier datum.
Classification
| Datum | Classification |
|---|---|
| (Delta_i\sim t^2) | existing conductor/soft coefficient support |
| trivial conductor soft monodromy | even Kummer order |
| logarithmic special rank three | saturated marked extension |
| ((1,2,2t)) | existing occurrence factors and soft Rees normal |
| (e_6) | surviving second-Rees bridge |
| marked-to-elliptic supported rank | zero |
| new support or torsion | none |
| new carrier datum | none |
Update to H2 versus H3
This is a high-value success for filtered H2. At the first locus where conductor, elliptic total-energy, Cut--nearby, and soft structures meet, the two cospan legs remain controlled by the same predeclared support-sensitive calculus. No sector-specific operation is needed.
The result remains narrower than a full joint-nearby theorem because the order (E\to0) then (t\to0) is fixed and the pure elliptic soft block has not been recomputed.
Evidence
research/benincasa/marici-gm/src/bin/joint_soft_conductor_elliptic_cospan.rs;research/benincasa/joint-soft-conductor-elliptic-cospan-certificate.json;- Entries 307--308, 352--355, and 367.
Next falsifier
Compute the genuinely two-parameter nearby object in ((E,t)), rather than only the iterated (E)-then-(t) specialization. Compare both operation orders and retain:
- the pure elliptic nilpotent;
- the two conductor Kummer characters;
- the marked rank-three cospan legs;
- the (e_6) second-Rees line; and
- the integral half-sum lattice.
A nonzero order commutator outside the already known algebraic exceptional class, or a new mixed factor not generated by (E,t,2), would be the next H2-to-H3 update. After that, the simultaneous (x=y=0) point is the final triangle soft corner.