Exact spectral gap of random Pauli rotations

Unsolved ID op_aaf9791beced84e4 Last edited 16 September 2026
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Problem

Is the exact Haar-mixing spectral gap of uniformly random Pauli rotations equal to \(2^n(2^n-3)/(8(4^n-1))\) for every \(n\geq4\)?

Let \(\mathcal P_n=\{I,X,Y,Z\}^{\otimes n}\setminus\{I^{\otimes n}\}\). One step chooses \(P\in\mathcal P_n\) and \(\theta\in[0,2\pi)\) uniformly and applies \(e^{i\theta P}\). On \(L^2(\mathrm{SU}(2^n),\mathrm{Haar})\), define

\begin{equation} (K_nf)(U)=\mathbb E_{P,\theta}f(e^{i\theta P}U), \qquad \Delta_n=1-\|K_n|_{L^2_0}\|_{2\to2}, \tag{1} \end{equation}

where \(L^2_0\) is the zero-Haar-mean subspace. The conjectured value of the gap in Eq. (1) is

\begin{equation} \Delta_n=\frac{2^n(2^n-3)}{8(4^n-1)} \tag{2} \end{equation}

Does Eq. (2) hold for every \(n\geq4\)?

Source

The question is explicitly posed or retained as open in the cited primary literature [Baer26]. The statement is rewritten here to make its hypotheses and success criterion self-contained.

Progress

  • Baer and Haah prove the bounds

    \begin{equation} \frac{4^n+16}{16(4^n-1)} \leq\Delta_n \leq\frac{2^n(2^n-3)}{8(4^n-1)}. \tag{3} \end{equation}

    The upper bound comes from the fourth-moment representation \(U^{\otimes4}\otimes\overline U^{\otimes4}\); see Theorem 3.16 and Proposition 3.17. [Baer26]

    The displayed definitions, constraints, and target bounds are recorded in Eqs. (3).

  • Proposition 3.17 settles \(n\leq3\). In particular, \(\Delta_3=5/63\), whereas the first unresolved instance has

    \begin{equation} \frac1{15}\leq\Delta_4\leq\frac{26}{255}. \tag{4} \end{equation}

    Conjecture 3.48 asserts that the upper bound is always attained. [Baer26]

    The displayed definitions, constraints, and target bounds are recorded in Eqs. (4).

  • The 23 July 2026 preprint proves a constant gap, but explicitly leaves this exact formula conjectural. No subsequent resolution of Conjecture 3.48 was located. [Baer26]

Comment

The unresolved issue is whether any higher representation mixes more slowly than the identified fourth-moment mode. This would determine the exact spectral bottleneck across all moment orders, not merely establish convergence to Haar randomness.

References

[Baer26]
T. Baer and J. Haah, "Random unitary circuits with constant spectral gap," arXiv preprint (2026), version 1, 23 July 2026.arXiv

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“Exact spectral gap of random Pauli rotations,” Quantum Information and Quantum Computation Open Problem Zoo (QIQCOP Zoo), ID op_aaf9791beced84e4, accessed 2026-09-16.

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@incollection{qiqcop_op_aaf9791beced84e4,
  title = {Exact spectral gap of random Pauli rotations},
  booktitle = {Quantum Information and Quantum Computation Open Problem Zoo (QIQCOP Zoo)},
  year = {2026},
  howpublished = {\url{https://qiqc-op.com/problem/op_aaf9791beced84e4/}},
  note = {Stable ID op_aaf9791beced84e4; status: Unsolved; accessed 2026-09-16}
}

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“Exact spectral gap of random Pauli rotations,” Quantum Information and Quantum Computation Open Problem Zoo (QIQCOP Zoo), https://qiqc-op.com/problem/op_aaf9791beced84e4/, ID op_aaf9791beced84e4, accessed 2026-09-16.

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op_aaf9791beced84e4
01M2M9FCB1FHWBC06BEF4123WQ