Skip to content
DraconiticResearch
Search Sources API
203,234 studies31 sourcesUpdated 17 min ago
PreprintCC BY 4.0arXiv

Improved bounds on stabilizer extent and Clifford rank

Abstract

We prove that every pure state of stabilizer rank at most k has stabilizer extent at most 2O(√(klog(k+1))), and establish the analogous bound for the squared Clifford coefficient norm of Clifford-rank-k operators. This implies stabilizer fidelity at least 2−O(√(klog(k+1))), resolving the quantitative conjecture of (Mehraban-Tamasbi, STOC, 2025), and proves an Ω(n2/log n) lower bound for the approximate stabilizer rank of tensor powers of any non-stabilizer qubit state. The latter result generalizes the best-known lower bound for tensor powers of T-states (Mehraban-Tamasbi, STOC, 2024) to arbitrary non-stabilizer qubit states, including magic states. As a consequence of the Clifford rank--norm inequality, we obtain an Ω(n2/log n) lower bound for exact representations of n-bit AND function by quadratic phases, improving the previous best-known linear bound. Further consequences rule out pseudorandom state and unitary ensembles with approximate stabilizer and Clifford rank O((log n)2/loglog n), respectively, a log n improvement over prior work (Kalra-Sinha, Quantum, 2026). We also obtain tomography algorithms for states of stabilizer rank at most k, with poly(n)2O(√(klog(k+1))) time and copy complexity, a nearly square-root improvement in the exponent over the best-known algorithm.

Related

  1. Clifford-hierarchy stabilizer formalism with applications to twisted quantum doubles
    Christopher Fechisin, Kieran Cooney, Mathi Raja +4
    arXivPreprintCC BY 4.0Full textCondensed matterQuantum physics & quantum informationarXiv
  2. A three-eighths upper bound on the stabilizer-rank exponent of face-center magic states
    Samuel Bevins
    arXivPreprintCC BY 4.0Full textQuantum physics & quantum informationarXiv
  3. A note on tomography of states with low stabilizer rank
    Arkopal Dutt
    arXivPreprintarXiv licenceFull textQuantum physics & quantum informationarXiv
  4. Stabilizer entropy cones as self-dual slices of linear rank cones: a five-party gap and dependence on the local dimension
    Xidan Song, Ruifeng Cao
    arXivPreprintarXiv licenceFull textCombinatorics & discrete mathematicsQuantum physics & quantum informationarXiv
  5. Improved Transversal Non-Clifford Gates from Cup Products
    Louis Golowich, Itzhak Tamo, Guanyu Zhu
    arXivPreprintarXiv licenceFull textGeneral mathematicsQuantum physics & quantum informationarXiv
BibTeX
@misc{sinha2026improved,
  title = {{Improved bounds on stabilizer extent and Clifford rank}},
  author = {Pulkit Sinha and Benjamin Lovitz},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2610.06819},
  eprint = {2610.06819},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2610.06819},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - Improved bounds on stabilizer extent and Clifford rank
AU  - Pulkit Sinha
AU  - Benjamin Lovitz
PY  - 2026
DA  - 2026/10/05
PB  - arXiv
DO  - 10.48550/arxiv.2610.06819
UR  - https://arxiv.org/abs/2610.06819
AB  - We prove that every pure state of stabilizer rank at most k has stabilizer extent at most 2^O(√(klog(k+1))), and establish the analogous bound for the squared Clifford coefficient norm of Clifford-rank-k operators. This implies stabilizer fidelity at least 2^−O(√(klog(k+1))), resolving the quantitative conjecture of (Mehraban-Tamasbi, STOC, 2025), and proves an Ω(n^2/log n) lower bound for the approximate stabilizer rank of tensor powers of any non-stabilizer qubit state. The latter result generalizes the best-known lower bound for tensor powers of T-states (Mehraban-Tamasbi, STOC, 2024) to arbitrary non-stabilizer qubit states, including magic states. As a consequence of the Clifford rank--norm inequality, we obtain an Ω(n^2/log n) lower bound for exact representations of n-bit AND function by quadratic phases, improving the previous best-known linear bound. Further consequences rule out pseudorandom state and unitary ensembles with approximate stabilizer and Clifford rank O((log n)^2/loglog n), respectively, a log n improvement over prior work (Kalra-Sinha, Quantum, 2026). We also obtain tomography algorithms for states of stabilizer rank at most k, with poly(n)2^O(√(klog(k+1))) time and copy complexity, a nearly square-root improvement in the exponent over the best-known algorithm.
ER  -