The qubit H-type state, the edge centre of the stabilizer octahedron. Clifford-equivalent to the phase state (|0〉 + eiπ/4|1〉)/√2, which is what the literature usually means by 'the T state'.
The most studied cell in the field: χ ≤ 7 at six copies underpins the standard 20.47n figure, and the cat-state rank 6 there (exponent 0.431, Qassim, Pashayan, and Gosset, arXiv:2106.07740) refuted the conjecture that 7 was optimal. The published exponent log₂3/4 comes from their asymptotic contracted-cat-state family rather than from any single m, so every finite-m entry here sits above it. The ZX restatement of Kissinger, van de Wetering, and Vilmart (arXiv:2202.09202) adds a partial decomposition of |T〉⊗5 into three terms that each keep one |T〉, so χ(Tt) ≤ 3χ(Tt−4); it gives 9 at m=7 and 12 at m=8, and the glued |cat₁₀〉 gives 18 at m=10 (exponent 0.417).
| bound | m | rank | γ | tier | attribution |
|---|---|---|---|---|---|
| 1 | 2 | — | verified | @vprusso · stabrank verify_challenge | |
| 1 | 2 | 1.0000 | verified | @vprusso · stabrank research/constructions/data | |
| 2 | 2 | — | lean | @vprusso · stabrank verify_challenge | |
| 2 | 2 | 0.5000 | lean | Bravyi, Smith, and Smolin · arXiv:1506.01396 | |
| 3 | 3 | — | reproduced | @vprusso · stabrank PR #18 | |
| 3 | 3 | 0.5283 | lean | Bravyi, Smith, and Smolin · arXiv:1506.01396 | |
| 4 | 3 | — | reproduced | @vprusso · stabrank PR #18 | |
| 4 | 4 | — | reproduced | @vprusso · stabrank rank_exclusion.py | |
| 4 | 4 | 0.5000 | lean | @FarLab @vprusso · arXiv:2605.28586 | |
| 5 | 4 | — | reproduced | @vprusso · stabrank rank_exclusion.py | |
| 5 | 5 | — | reproduced · 3600 s | @vprusso · stabrank slice_lift.py | |
| 5 | 6 | — | attested · 2/323 re-run | @vprusso · stabrank research/h5_rank5 | |
| 5 | 6 | 0.5170 | lean | Bravyi, Smith, and Smolin · arXiv:1506.01396 | |
| 6 | 4 | — | reproduced | @FarLab @vprusso · arXiv:2605.28586 | |
| 6 | 6 | — | attested · 2/180 re-run | @vprusso · stabrank research/h6_rank5 | |
| 6 | 6 | 0.4308 | lean | Qassim, Pashayan, and Gosset · arXiv:2106.07740 | |
| 6 | 7 | 0.4679 | verified | Bravyi, Smith, and Smolin · arXiv:1506.01396 | |
| 7 | 6 | — | attested · 2/180 re-run | @vprusso · stabrank research/h6_rank5 | |
| 7 | 9 | 0.4528 | lean | Kissinger, van de Wetering, and Vilmart · arXiv:2202.09202 | |
| 8 | 6 | — | attested · 2/180 re-run | @vprusso · stabrank research/h6_rank5 | |
| 8 | 12 | 0.4481 | lean | Kissinger, van de Wetering, and Vilmart · arXiv:2202.09202 | |
| 9 | 6 | — | attested · 2/180 re-run | @vprusso · stabrank research/h6_rank5 | |
| 9 | 18 | 0.4633 | verified | @vprusso · arXiv:2106.07740, arXiv:2202.09202 | |
| 10 | 6 | — | attested · 2/180 re-run | @vprusso · stabrank research/h6_rank5 | |
| 10 | 18 | 0.4170 | lean | Kissinger, van de Wetering, and Vilmart · arXiv:2202.09202 |
Beating the published exponent needs χ ≤ 6 at m=7→ 0.3693.