1540 — The Small-Pole Cycle Trace Survives the Mass Collision
Status
Exact relative-cycle residue pairing for the two poles that collide on the
physical mass diagonal.
Pole system
For
A=(y1+y2)2,B=(y1−y2)2,
the double-Gysin source is
Icorner(X)=(X2−A)(X2−B)2X.
Its four simple poles are
X=±(y1+y2),X=±(y1−y2).
The invariant normal coordinate is B=δ2, so a loop around B=0
exchanges the two small-pole cycles
γ+↔γ−,X=±δ.
Residue pairing
The two small-pole residues are equal:
r+=r−=B−A1.
Likewise, the two large-pole residues are
R+=R−=A−B1.
Their total sum vanishes, consistently with cubic falloff:
r++r−+R++R−=0.
Trace and anti-trace
In the deck eigenbasis,
γtr=γ++γ−,γanti=γ+−γ−,
the source pairing gives
⟨I,γtr⟩=B−A2,⟨I,γanti⟩=0.
On the physical diagonal B=0, the two small poles collide at X=0.
The invariant trace limits exactly to the residue of the physical central
pole:
B−A2B=0=−A2=ResX=0Imass,corner.
Meaning
The coefficient connection is pure gauge (Entry 1538), but the relative-cycle
system carries a nontrivial deck permutation. The source pairing selects its
invariant trace and annihilates the anti-invariant cycle.
Thus the physical one-channel readout is not obtained from coefficients alone: