The qutrit T-type or face-centre state. All three amplitudes have equal modulus 1/√3 and differ only by phase, which is precisely why the subset-sum lower-bound technique cannot reach this orbit: that argument needs an exponentially increasing subsequence of amplitude moduli.
The only orbit whose amplitudes leave Q(ω₃), living instead in Q(ω₉). That extra field degree is what a Galois argument can exploit, and it is where the certified χ ≥ 6 at m=3 comes from.
| bound | m | rank | γ | tier | attribution |
|---|---|---|---|---|---|
| 1 | 3 | — | lean | @vprusso · stabrank PR #19 | |
| 1 | 3 | 1.0000 | lean | Kocia and Sarovar · arXiv:2003.01130 | |
| 2 | 3 | — | lean | @vprusso · stabrank PR #16 | |
| 2 | 3 | 0.5000 | lean | Kocia and Sarovar · arXiv:2003.01130 | |
| 3 | 6 | — | reproduced | @vprusso · stabrank PR #16 | |
| 3 | 7 | — | verified | @vprusso · stabrank PR #41 | |
| 3 | 8 | — | attested · 2/459 re-run | @vprusso · stabrank research/t3_rank7 | |
| 3 | 8 | 0.6309 | lean | @FarLab @vprusso · arXiv:2605.28586 | |
| 4 | 6 | — | reproduced | @vprusso · stabrank cert_t3m3_rank6.py | |
| 4 | 8 | — | attested · 2/459 re-run | @vprusso · stabrank research/t3_rank7 | |
| 4 | 9 | 0.5000 | lean | @FarLab @vprusso · arXiv:2605.28586 | |
| 5 | 6 | — | reproduced | @vprusso · stabrank cert_t3m3_rank6.py | |
| 5 | 8 | — | attested · 2/459 re-run | @vprusso · stabrank research/t3_rank7 | |
| 5 | 18 | 0.5262 | lean | @vprusso · stabrank sector-state search | |
| 6 | 8 | — | attested · 2/459 re-run | @vprusso · stabrank research/t3_rank7 | |
| 6 | 27 | 0.5000 | verified | @vprusso · stabrank research/constructions/product_witness.py |
Beating the published exponent needs χ ≤ 8 at m=4→ 0.4732.