Packed Quotient Images Already Attain Global Cut Rank On Small Quantum Tanner Instances¶
Claim/Theorem¶
Keep the notation of [[local-quotient-image-span-controls-rank-accumulation.md]]. For a qubit cut \(L \sqcup R = Q\) in the chosen local-generator presentation of a Quantum Tanner code, write
and define
Then the exact small-instance quotient-image behavior is sharper than the previous bottleneck statement:
-
On the currently lowest sampled balanced cuts of the explicit
D_4,D_6, andD_8Quantum Tanner instances reconstructed from Appendix C / Table V of10.48550/arXiv.2508.05095, one has\[ \nu_H(L)=\lambda_{M(H)}(L). \] -
Therefore, on these explicit low-cut witnesses, the main algebraic collapse is not an additional post-packing loss
\[ \nu_H(L)\rightsquigarrow \lambda_{M(H)}(L), \]but only the earlier losses
\[ \mu_H(L)\rightsquigarrow \sigma_H(L)\rightsquigarrow \lambda_{M(H)}(L)=\nu_H(L). \] -
In particular, the concrete missing family-level invariant is not merely "some direct-sum packing might exist." The right missing construction-level statement is a linear-size quotient-pivot or triangular-witness property forcing
\[ \nu_H(L)=\Omega(|Q|) \]for every balanced cut.
Equivalently, the live family theorem now needed is:
there exists a family of local quotient images \(W_v(L)\) containing a direct-sum subfamily of total dimension \(\Omega(|Q|)\).
Since [[local-quotient-image-span-controls-rank-accumulation.md]] already proves
the hypothesis \(H'_{\mathrm{pivot}}(\beta)\) would immediately imply linear balanced intrinsic cut rank.
Proof sketch:
-
For each sampled balanced cut \(L\), compute the exact quotient
\[ \frac{S}{B(L)} \]and the exact local images \(W_v(L)\) in a fixed quotient basis.
-
Compute \(\nu_H(L)\) exactly by dynamic programming on reachable quotient subspaces: from a current span \(U\), add a block image \(W_v(L)\) only when
\[ \dim(U+W_v(L))=\dim U+\dim W_v(L), \]so the addition is direct. The maximum reachable dimension is exactly \(\nu_H(L)\).
-
Compare the exact output to the global cut rank
\[ \lambda_{M(H)}(L)=\dim\frac{S}{B(L)}. \]For the current low-cut witnesses, the maximum reachable direct-sum dimension equals the full quotient dimension in all three cases.
Exact low-cut data from the present cycle:
-
D_4/[36,8,3]:\[ \lambda=5,\qquad \nu=5,\qquad \sigma=16,\qquad \mu=19. \]The local quotient-image dimensions have histogram
\[ \{0:4,\ 1:8,\ 2:4\}. \] -
D_6/[54,11,4]:\[ \lambda=12,\qquad \nu=12,\qquad \sigma=35,\qquad \mu=35. \]The local quotient-image dimensions have histogram
\[ \{1:13,\ 2:11\}. \] -
D_8/[72,14,4]:\[ \lambda=12,\qquad \nu=12,\qquad \sigma=34,\qquad \mu=48. \]The local quotient-image dimensions have histogram
\[ \{0:9,\ 1:12,\ 2:11\}. \]
These exact computations isolate the dominant failure mode:
- in
D_4andD_8, some local images vanish after quotienting, and many surviving images are redundant inside the same low-dimensional quotient span; - in
D_6, there is essentially no survival loss at all on the sampled low cut, but there is still heavy redundancy because many surviving images occupy the same12-dimensional quotient space; - in all three cases, once one passes to the best direct-sum packed family, no further gap remains: the packed family already spans the full quotient.
So the explicit-family evidence now points to quotient-pivot extraction, not another obstruction to packing, as the correct next invariant.
Dependencies¶
- [[local-quotient-image-span-controls-rank-accumulation.md]]
- [[quantum-tanner-needs-balanced-local-block-rank-accumulation.md]]
- [[quantum-tanner-local-generator-blowup.md]]
- [[stabilizer-cut-rank-functional.md]]
- [[cut-rank-is-interface-state-dimension.md]]
Conflicts/Gaps¶
- This node is still small-instance evidence, not a theorem over the whole Quantum Tanner family.
- The balanced cuts used here are the currently lowest sampled cuts in the reconstructed
D_4,D_6, andD_8instances, not provably extremal cuts. - The node does not yet prove that \(\nu_H(L)=\lambda_{M(H)}(L)\) for all balanced cuts, even in these explicit small instances.
- What is now isolated more sharply is the exact missing invariant: a family theorem that produces linearly many independent quotient-image pivots, or equivalently a linear lower bound on \(\nu_H(L)\).
Sources¶
10.48550/arXiv.2206.0757110.48550/arXiv.2508.05095