- Campbell, Earl T., Anwar, Hussain, Browne, Dan E.. Magic-State Distillation in All Prime Dimensions Using Quantum Reed-Muller Codes. Physical Review X, vol. 2, p. 041021, 2012 · arXiv:1205.3104
Distills the Howard-Vala eigenstates in every prime dimension; motivation for the p = 5 and p = 7 candidate orbits.
- Howard, Mark, Vala, Jiri. Qudit versions of the qubit pi/8 gate. Physical Review A, vol. 86, p. 022316, 2012 · arXiv:1206.1598
The qudit pi/8 gates and their eigenstates for every prime p; the p = 3 eigenstate is the T3 orbit.
- Bravyi, Sergey, Gosset, David. Improved Classical Simulation of Quantum Circuits Dominated by Clifford Gates. Physical Review Letters, vol. 116, p. 250501, 2016 · arXiv:1601.07601 · DOI
Approximate stabilizer rank and stabilizer extent only; carries no exact-rank value.
- Bravyi, Sergey, Smith, Graeme, Smolin, John A.. Trading Classical and Quantum Computational Resources. Physical Review X, vol. 6, p. 021043, 2016 · arXiv:1506.01396 · DOI
Introduces stabilizer rank and the six-copy decomposition of the qubit H-type state.
- Bravyi, Sergey, Browne, Dan, Calpin, Padraic, Campbell, Earl, Gosset, David, Howard, Mark. Simulation of quantum circuits by low-rank stabilizer decompositions. Quantum, vol. 3, p. 181, 2019 · arXiv:1808.00128 · DOI
Source of the seven-copy value chi(H^7) <= 12 recorded in the Qassim, Pashayan, and Gosset table; superseded by the 9 that the partial decomposition of kissinger2022partial gives.
- Huang, Yifei, Love, Peter. Approximate stabilizer rank and improved weak simulation of Clifford-dominated circuits for qudits. Physical Review A, vol. 99, p. 052307, 2019 · arXiv:1808.02406
Approximate-rank exponents 2^{0.23 t}, 3^{0.32 t}, 5^{0.41 t}, 7^{0.40 t} for the qudit magic state at d = 2, 3, 5, 7; the d-term Clifford-orbit decomposition.
- Jain, Akalank, Prakash, Shiroman. Qutrit and Ququint Magic States. 2020 · arXiv:2003.07164
Complete list of single-qutrit and single-ququint Clifford eigenstates; no strange-state analogue for any prime p > 3. Source list for p = 5 candidate orbits.
- Kocia, Lucas. Improved Strong Simulation of Universal Quantum Circuits. 2020 · arXiv:2012.11739
Twelve-copy decomposition of the qubit H-type state into 47 stabilizer states, exponent log_2(47)/12 = 0.463.
- Prakash, Shiroman. Magic state distillation with the ternary {Golay} code. Proceedings of the Royal Society A, vol. 476, p. 20200187, 2020 · arXiv:2003.02717
Golay-code distillation of the strange and Norrell states; no rank content.
- Heimendahl, Arne, Montealegre-Mora, Felipe, Vallentin, Frank, Gross, David. Stabilizer extent is not multiplicative. Quantum, vol. 5, p. 400, 2021 · arXiv:2007.04363 · DOI
Extent is strictly sub-multiplicative for generic high-dimensional states; carries no exact-rank value.
- Kocia, Lucas, Sarovar, Mohan. Improved Simulation of Quantum Circuits by Fewer Gaussian Eliminations. Physical Review A, vol. 103, p. 022603, 2021 · arXiv:2003.01130
Qutrit stabilizer-rank numerics; records chi(T3^3) as 8? and flags the search as possibly unconverged.
- Qassim, Hammam, Pashayan, Hakop, Gosset, David. Improved upper bounds on the stabilizer rank of magic states. Quantum, vol. 5, p. 606, 2021 · arXiv:2106.07740 · DOI
Contracted cat states; source of the log2(3)/4 exponent.
- Seddon, James R., Regula, Bartosz, Pashayan, Hakop, Ouyang, Yingkai, Campbell, Earl T.. Quantifying quantum speedups: improved classical simulation from tighter magic monotones. PRX Quantum, vol. 2, p. 010345, 2021 · arXiv:2002.06181
Dyadic negativity, mixed-state extent and generalized robustness; no exact-rank value.
- Kissinger, Aleks, van de Wetering, John. Simulating quantum circuits with {ZX}-calculus reduced stabiliser decompositions. Quantum Science and Technology, vol. 7, p. 044001, 2022 · arXiv:2109.01076
Consumes the BBCCGH and QPG decompositions inside ZX simplification; no new rank value.
- Kissinger, Aleks, van de Wetering, John, Vilmart, Renaud. Classical Simulation of Quantum Circuits with Partial and Graphical Stabiliser Decompositions. vol. 232, p. 5:1--5:13, 2022 · arXiv:2202.09202
chi(cat_4) = 2 used as a 2^{0.25 t} decomposition when the cat_4 pattern appears; a partial decomposition of T^5 into three terms each keeping one T, so chi(T^t) <= 3 chi(T^(t-4)): chi(H^7) <= 9 and chi(H^8) <= 12 on the board, and the glued cat_10 gives chi(H^10) <= 18.
- Kocia, Lucas, Tulloch, Genele. More Optimal Simulation of Universal Quantum Computers. 2022 · arXiv:2202.01233
Weak-simulation prefactor via correlated sampling; quotes chi(T^4) = 4, chi(T^8) <= 12, chi(T^16) <= 108 from the cat-state construction.
- Labib, Farrokh. Stabilizer rank and higher-order Fourier analysis. Quantum, vol. 6, p. 645, 2022 · arXiv:2107.10551 · DOI
Omega(n) exact-rank lower bound at every prime p; the p=3 magic state is the T3 orbit.
- Lovitz, Benjamin, Steffan, Vincent. New Techniques for Bounding Stabilizer Rank. Quantum, vol. 6, p. 692, 2022 · arXiv:2110.07781 · DOI
Prop. 3.7 bounds exact rank from the field of definition of stabilizer coordinates, over Q(i).
- Peleg, Shir, Shpilka, Amir, Volk, Ben Lee. Lower Bounds on Stabilizer Rank. Quantum, vol. 6, p. 652, 2022 · arXiv:2106.03214 · DOI
Subset-sum route; needs amplitudes attaining different values across Hamming-weight layers.
- Koch, Mark, Yeung, Richie, Wang, Quanlong. Speedy Contraction of {ZX} Diagrams with Triangles via Stabiliser Decompositions. 2023 · arXiv:2307.01803
Tensored ZX star edges (triangle nodes, each of stabilizer rank 2) decomposed with 2^{0.774 t} terms; the only sub-product bound found for a CCZ-like resource, transfer to chi(|CCZ>^k) unconfirmed.
- Kliuchnikov, Vadym, Sch{\"o}nnenbeck, Sebastian. Stabilizer operators and {Barnes-Wall} lattices. 2024 · arXiv:2404.17677
Minimal vectors of the Barnes-Wall lattices are stabilizer states; the lattice input to the Kalra-Sinha bounds.
- Mehraban, Saeed, Tahmasbi, Mehrdad. Quadratic Lower Bounds on the Approximate Stabilizer Rank. Proceedings of the 56th Annual ACM Symposium on Theory of Computing (STOC), 2024 · arXiv:2305.10277
Omega~(n^2) for approximate rank, which carries to exact rank.
- de Silva, Nadish, Yin, Ming, Strelchuk, Sergii. Bases for optimising stabiliser decompositions of quantum states. 2024 · arXiv:2311.17384
The space of linear dependencies of n-qubit stabilizer states has a basis of three-term dependencies; every decomposition is reachable by adding dependent triples. Qubit only.
- Camillo, Giulio, Peres, Filipa C. R., Heinrich, Markus, Bermejo-Vega, Juani. Symmetry-Accelerated Classical Simulation of Clifford-Dominated Circuits. 2025 · arXiv:2510.18977
Optimal extent decompositions of real, diagonal and real-diagonal unitaries lie in the matching Clifford subgroup; extents up to seven qubits. Extent, not exact rank.
- Codsi, Julien, Laakkonen, Tuomas. Unifying Graph Measures and Stabilizer Decompositions for the Classical Simulation of Quantum Circuits. 2026 · arXiv:2603.06377
Tree-width and rank-width simulation bounds; no exact-rank value.
- Kalra, Arnav, Sinha, Makrand. Stabilizer Ranks, Barnes Wall Lattices and Magic Monotones. Quantum, vol. 10, p. 2179, 2026 · arXiv:2503.04101
Omega(n / log n) lower bound on the approximate rank of the H-type state via a quantitative stabilizer-fidelity bound.
- Labib, Farrokh, Russo, Vincent. Stabilizer rank bounds for magic-state orbits. 2026 · arXiv:2605.28586
Per-copy exponents for the four qutrit orbits; the baselines this challenge is measured against.
- de Colnet, Alexis, Geerts, Floris, Hai, Rihan, Laarman, Alfons, Lee, Joon Hyung, P{\'e}rez, Guillermo A.. Quadratic Sums-of-Powers for Fixed-Parameter Tractable Quantum-Circuit Simulation. 2026 · arXiv:2605.29944
Rank-width dynamic program with a stabilizer-rank optimization that takes the QPG decomposition as a black box.
- {dring-05}. qutrit-t3-structural-obstructions: exact structural obstructions for four-copy qutrit {T} stabilizer rank. 2026
Two restricted theorems on decompositions of |T3>^4 (fixed-foliation and unique-crossing); does not claim chi(T3^4) >= 9. Not a paper; not re-run here.