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arXiv:2610.37991

Reducing the cost of ancilla purification for Majorana quantum computation

Piotr Ćwikliński, Łukasz Fojcik, Michał Studziński

quant-phcond-mat.str-elSubmitted Oct 27, 2026• Announced Oct 29, 2026• 0 citations• Revised Oct 30, 2026 (v2)
v1 · Oct 27, 2026v2 · Oct 30, 2026
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Abstract

Braiding Majorana zero modes does not by itself provide a universal set of quantum gates. Additional operations can be supplied through ancillary states, whose preparation need not have the same protection as braiding. Here, we consider purification of the non-Gaussian ancilla used for an entangling gate in Bravyi's scheme. We keep his elementary braid-and-fusion comparison and change how its outputs are combined. An additional layer compares the product of the three stabilizer signs. The first accepted errors giving an incorrect output then require three faulty input blocks rather than two. As a result, the preparation error decreases cubically instead of quadratically, and the asymptotic raw-copy overhead is reduced. We also construct a preliminary sequence in which a processed block is paired with a fresh copy from the same noisy source. For independent inputs supported in the even-parity sector and ideal purification operations, this sequence establishes a sufficient distillability fidelity of 59.95 percent after free Gaussian twirling. At a common source fidelity, it reduces the expected cost of preparing an input for the recurrence by more than seven orders of magnitude relative to the balanced construction studied here. Finally, we examine imperfect purification operations in an effective syndrome-noise model. The additional layer leaves the leading operation-error coefficient unchanged, although a nonzero error floor remains.

AI Summary

The paper studies purification of Bravyi’s eight-Majorana non-Gaussian ancilla, which supplies an entangling Clifford gate; a separate resource is needed for non-Clifford gates. It retains the braid-and-fusion two-copy comparison and changes its composition, using Gaussian frame changes to select stabilizer products while retaining unequal syndrome populations between layers. A fourth layer compares the product of three stabilizers on two independently prepared three-layer outputs. Accepted incorrect outputs then require three faulty raw blocks rather than two, giving $\epsilon_{\mathrm{out}}=(384/343)\epsilon^3+O(\epsilon^4)$. The isotropic recurrence’s unstable fidelity fixed point decreases from $0.61560748$ to $0.60471167$, and its asymptotic expected-copy overhead becomes $O([\log(1/\delta)]^{\log_3 16})$, versus exponent $3$ previously. Integer fault enumerators, exact recurrence polynomials, and root counting establish these claims. A twelve-stage initialization sequence includes one comparison between a processed block and a fresh source copy. Exact rational verification certifies distillability for independent even-parity inputs with target overlap $F\geq0.5995$, after Gaussian twirling. At $F=0.5997$, its expected seed cost is about $1.04\times10^6$ copies, versus $1.76\times10^{13}$ for the stated balanced benchmark; neither construction is proved optimal. Near the certified endpoint, subsequent purification remains costly: the prescribed schedule needs about $2.78\times10^{20}$ copies to reach infidelity $10^{-6}$. An effective syndrome-noise model gives the same leading operation-error floor, $17\lambda/7$, for both recurrences, not a hardware threshold. Costs assume perfect storage and exclude routing and timing. Arbitrary correlated inputs and unconditioned parity noise are not covered. Distillability for the isotropic family remains unresolved between the convex-Gaussian boundary $F=1/2$ and $0.5995$.

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21 pages, 3 figures

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Braiding Majorana zero modes does not by itself provide a universal set of quantum gates. Additional operations can be supplied through ancillary states, whose preparation need not have the same protection as braiding. Here, we consider purification of the non-Gaussian ancilla used for an entangling gate in Bravyi's scheme. We keep his elementary braid-and-fusion comparison and change how its outputs are combined. An additional layer compares the product of the three stabilizer signs. The first accepted errors giving an incorrect output then require three faulty input blocks rather than two. As a result, the preparation error decreases cubically instead of quadratically, and the asymptotic raw-copy overhead is reduced. We also construct a preliminary sequence in which a processed block is paired with a fresh copy from the same noisy source. For independent inputs supported in the even-parity sector and ideal purification operations, this sequence establishes a sufficient distillability fidelity of 59.95 percent after free Gaussian twirling. At a common source fidelity, it reduces the expected cost of preparing an input for the recurrence by more than seven orders of magnitude relative to the balanced construction studied here. Finally, we examine imperfect purification operations in an effective syndrome-noise model. The additional layer leaves the leading operation-error coefficient unchanged, although a nonzero error floor remains.
The paper studies purification of Bravyi’s eight-Majorana non-Gaussian ancilla, which supplies an entangling Clifford gate; a separate resource is needed for non-Clifford gates. It retains the braid-and-fusion two-copy comparison and changes its composition, using Gaussian frame changes to select stabilizer products while retaining unequal syndrome populations between layers.
A fourth layer compares the product of three stabilizers on two independently prepared three-layer outputs. Accepted incorrect outputs then require three faulty raw blocks rather than two, giving ϵout=(384/343)ϵ3+O(ϵ4)\epsilon_{\mathrm{out}}=(384/343)\epsilon^3+O(\epsilon^4)ϵout​=(384/343)ϵ3+O(ϵ4). The isotropic recurrence’s unstable fidelity fixed point decreases from 0.615607480.615607480.61560748 to 0.604711670.604711670.60471167, and its asymptotic expected-copy overhead becomes O([log⁡(1/δ)]log⁡316)O([\log(1/\delta)]^{\log_3 16})O([log(1/δ)]log3​16), versus exponent 333 previously. Integer fault enumerators, exact recurrence polynomials, and root counting establish these claims.
A twelve-stage initialization sequence includes one comparison between a processed block and a fresh source copy. Exact rational verification certifies distillability for independent even-parity inputs with target overlap F≥0.5995F\geq0.5995F≥0.5995, after Gaussian twirling. At F=0.5997F=0.5997F=0.5997, its expected seed cost is about 1.04×1061.04\times10^61.04×106 copies, versus 1.76×10131.76\times10^{13}1.76×1013 for the stated balanced benchmark; neither construction is proved optimal. Near the certified endpoint, subsequent purification remains costly: the prescribed schedule needs about 2.78×10202.78\times10^{20}2.78×1020 copies to reach infidelity 10−610^{-6}10−6.
An effective syndrome-noise model gives the same leading operation-error floor, 17λ/717\lambda/717λ/7, for both recurrences, not a hardware threshold. Costs assume perfect storage and exclude routing and timing. Arbitrary correlated inputs and unconditioned parity noise are not covered. Distillability for the isotropic family remains unresolved between the convex-Gaussian boundary F=1/2F=1/2F=1/2 and 0.59950.59950.5995.
Effectively managing various types of decoherence is crucial for leveraging entanglement in quantum information processing and quantum computing. In this paper, we propose purification circuits that deterministically produce a maximally entangled state from a single copy of an imperfect entangled pair affected by various noise sources. Unlike conventional methods, our approach eliminates the need for multiple copies of the entangled state, pre-purification operations, and imposes no restrictions on the initial entanglement fidelity of the imperfect pair. Our method utilizes ancilla qubits and CNOT gates to address errors from Pauli X and Z (bit flip and phase flip), as well as combinations of these errors that create general mixed entangled states and amplitude-damped entangled states. Our analysis shows that noisy CNOT gates impact fidelity minimally, with only the final two gates being critical. We validate our approach through mathematical analysis and practical implementation in Qiskit, demonstrating its effectiveness and robustness.
Protecting quantum information from noise is essential for reliable quantum computation and quantum memories. Quantum state purification addresses this challenge by processing multiple noisy copies of an unknown quantum state to produce an output state of higher fidelity. Here we establish nearly tight upper and lower bounds on the non-Clifford resources required to implement the symmetric-projection purification protocol. For nnn copies of a ddd-dimensional system, we construct a Clifford+T circuit that block-encodes the symmetric projector with operator-norm error at most εεε using O~(n)\widetilde{O}(n)O(n) T gates, where the tilde-OOO notation suppresses polylogarithmic factors in nnn, ddd, and 1/ε1/ε1/ε. Conversely, using stabilizer nullity, we prove that any Clifford+T implementation of such a block encoding with error ε<121−1/nε<\frac{1}{2}\sqrt{1-1/n}ε<21​1−1/n​ requires at least 2n−22n-22n−2 T gates, even allowing arbitrary positive normalization and clean stabilizer ancillas. Taken together, these results establish the nearly optimal scaling of non-Clifford cost with the number of copies and uncover the fundamental resource requirements for coherent symmetry projection in quantum state purification.
We consider the realization of universal quantum computation through braiding of Majorana fermions supplemented by unprotected preparation of noisy ancillae. It has been shown by Bravyi (2006 Phys. Rev. A 73 042313) that under the assumption of perfect braiding operations, universal quantum computation is possible if the noise rate on a particular four-fermion ancilla is below 40%. We show that beyond a noise rate of 89% on this ancilla the quantum computation can be efficiently simulated classically: we explicitly show that the noisy ancilla is a convex mixture of Gaussian fermionic states in this region, while for noise rates below 53% we prove that the state is not a mixture of Gaussian states. These results are obtained by generalizing concepts in entanglement theory to the setting of Gaussian states and their convex mixtures. In particular, we develop a complete set of criteria, namely the existence of a Gaussian-symmetric extension, which determine whether a state is a convex mixture of Gaussian states.
Quantum gates executed on physical hardware are inevitably degraded by environmental noise. While state purification effectively distills static quantum resources, the dynamic execution of quantum algorithms requires a higher-order approach to mitigate errors on the operations themselves. In this work, we investigate universal unitary purification: the task of utilizing a quantum higher-order operation to partially restore the ideal action of an unknown unitary corrupted by a known noise model. We consider deterministic purification of unknown single-qubit unitaries under independent depolarizing noise with ideal auxiliary operations. We prove that within the indefinite causal order (ICO) framework, no nontrivial 2-slot higher-order operation can universally purify the set of single-qubit unitaries. Overcoming this strict limitation, we establish that a 3-slot parallel architecture provides the minimal realization for nontrivial purification. We analytically derive the optimal average fidelity over all 3-slot ICO strategies and show that a parallel strategy attains it, strictly surpassing trivial strategies through input encoding and joint decoding of the channel outputs and a quantum memory. Furthermore, we provide a concrete quantum circuit construction attaining this optimum. Our results clarify the possibilities and limitations of purifying unknown qubit unitaries under depolarizing noise, offering insights for robust gate design.
Adiabatic braiding of Majorana zero modes can be used for topologically protected quantum information processing. While extremely robust to many environmental perturbations, these systems are vulnerable to noise with high-frequency components. Ironically, slower processes needed for adiabaticity allow more noise-induced excitations to accumulate, resulting in an antiadiabatic behavior that limits the precision of Majorana gates if some noise is present. In a recent publication (2017 Phys. Rev. B 96 075158), fast optimal protocols were proposed as a shortcut for implementing the same unitary operation as the adiabatic braiding in a low-energy effective model. These shortcuts sacrifice topological protection in the absence of noise but provide performance gains and remarkable robustness to noise due to the shorter evolution time. Nevertheless, gates optimized for vanishing noise are suboptimal in the presence of noise. If we know the noise strength beforehand, can we design protocols optimized for the existing unavoidable noise, which will effectively correct the noise-induced errors? We address this question in the present paper, focusing on the same low-energy effective model. We find such optimal protocols using simulated-annealing Monte Carlo simulations. The numerically found pulse shapes, which we fully characterize, are in agreement with Pontryagin's minimum principle, which allows us to arbitrarily improve the approximate numerical results (due to discretization and imperfect convergence) and obtain numerically exact optimal protocols. The protocols are bang–bang (sequence of sudden quenches) for vanishing noise, but contain continuous segments in the presence of multiplicative noise due to the nonlinearity of the master equation governing the evolution. We find that such noise-optimized protocols completely eliminate the above-mentioned antiadiabatic behavior. The final error corresponding to these optimal protocols monotonically decreases with the total time (in three different regimes). A liner fit to 1/ τ indicates extrapolation of the cost function to finite value in the limit. However, quadratic and cubic fits are more suggestive of the cost function extrapolating to zero in the limit of infinite time. Our results set the precision limit of the device as a function of the noise strength and total time.
Fault-tolerant preparation of non-Clifford resource states is a major contributor to the overhead of quantum computation, motivating protocols that achieve high output fidelity with minimal qubit and circuit costs. We introduce a low-cost magic-state preparation protocol in which the choice of stabilizer generators is co-designed with the flag gadgets, allowing the syndrome-extraction circuit itself to filter correlated faults across a non-Clifford layer. The protocol prepares a logical plus state in the 15-qubit quantum Reed-Muller code, applies a transversal T gate, and gauge-fixes the same register into the seven-qubit Steane code. By reorganizing equivalent Z-type stabilizer generators into jointly flagged measurement groups, the protocol eliminates all accepted logical-error contributions arising from one or two circuit faults under destructive error detection. Under a uniform circuit-level depolarizing noise model, the postselected infidelity is 210.2p3+O(p4)210.2p^3+O(p^4)210.2p3+O(p4). At p=10−3p=10^{-3}p=10−3, exact low-order enumeration combined with stratified sampling bounds the infidelity by 2.2×10−72.2\times10^{-7}2.2×10−7 at 99.9% joint confidence, while retaining an acceptance probability of 86.9%. The complete circuit requires only 19 qubits and 82 CNOT gates. These results demonstrate that stabilizer-generator design can substantially reduce the cost of postselected magic-state preparation, although corrected operation and the fidelity of an unmeasured output block require separate analysis.