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Non-Abelian Mixer for QAOA on Hybrid Oscillator-Qubit Quantum Processors

Thinh Le, Hansika Weerasena, Jianqing Liu (NC State Univ.) · arXiv:2605.30234 · new submission, 2026-05-29 · score 9/10 (HIGH)

Abstract

The realization of universal control in hybrid oscillator-qubit quantum processors enables the systematic design and implementation of quantum algorithms. However, the algorithmic development for such platforms remains at an early stage. While the Quantum Approximate Optimization Algorithm (QAOA) has been extensively studied in both continuous-variable (CV) and discrete-variable (DV) quantum systems, its development in the hybrid CV-DV setting remains limited. In this paper, we propose a hardware-native non-Abelian mixer for QAOA on hybrid CV-DV quantum processors and develop a corresponding hybrid ansatz for the Max-Cut problem. We evaluate the proposed ansatz on unweighted Erdős–Rényi graphs and benchmark it against the standard transverse-field mixer using the approximation ratio and optimal-solution probability. Across all graph sizes and Fock cutoffs in our simulations, the proposed non-Abelian mixer consistently improves both expected solution quality and the probability of sampling an optimal solution relative to the transverse-field mixer.

Executive summary

The authors port QAOA to hybrid continuous-variable / discrete-variable (CV-DV) hardware (think superconducting cavities + transmon ancillas) and propose a new non-Abelian mixer built from conditional displacements along the non-commuting and oscillator quadratures, with GKP-encoded logical qubits providing the computational basis. On unweighted Erdős–Rényi Max-Cut instances (N=4,5), the mixer consistently beats the standard transverse-field mixer — mean approximation ratio improves by ≈0.13 and optimal-solution probability by ≈0.155 across all tested Fock cutoffs. For Yuan, this is a direct method overlap with Y1 (QAOA on Max-Cut) and Y2 (hard / constraint-aware mixer design), opening a credible CV-DV avenue for warm-started or iterative variants in future work.

Main contribution

The paper introduces (i) a hardware-native non-Abelian QSP (NA-QSP) mixer composed of alternating conditional displacements CD(iβₓ, σ_φₓ) and CD(β_p, σ_φ_p) interleaved with single-qubit X-rotations on each oscillator–qubit pair, and (ii) a full hybrid CV-DV QAOA layer in which GKP-encoded logical states are coupled to ancilla qubits via the non-Abelian readout operation 𝓔ₓ(√π/2, Δ), the Max-Cut cost unitary U_C(γₖ) is applied on the ancilla register as a product of logical R_ZZ gates, and the inverse operation transfers phases back to the GKP modes before the local mixer acts. At depth d=0 the mixer reduces to the transverse-field baseline; at d≥1 it exploits the non-commutativity of [x̂, p̂] to generate richer dynamics on the encoded state manifold.

Key algorithms / building blocks

Detailed walkthrough

Section §II lays out the phase-space ISA for hybrid CV-DV processors: each oscillator mode is described by quadratures x̂, p̂ with [x̂, p̂] = i/2, and the elementary primitives are single-qubit rotations R_n̂(θ) and conditional displacements CD(β, σ_φ) = exp[(β↠− β*â) ⊗ σ_φ] coupling an ancilla qubit to a bosonic mode. The qubit-only logical R_ZZ gate, needed for the Max-Cut cost unitary, is synthesized via oscillator-mediated closed phase-space trajectories. Logical qubits are encoded in finite-energy GKP codewords |0⟩_GKP, |1⟩_GKP with envelope parameter Δ (smaller Δ → sharper but higher-energy peaks).

Section §III is the methodological heart. The key insight is that with non-Abelian QSP one can build a mixer that is not simply a sum of transverse-field X_i terms but instead a sequence of alternating - and -coupled conditional displacements (Eq. 7). The mixer is local (acts on each (m_i, q_i) pair) but the parameter set Θ_k is shared across pairs within a layer; at depth d=0 it collapses to e^{−iβ₀ Σ_i X_i}, reproducing the standard QAOA mixer. The complete circuit (Fig. 2 / Eq. 11) interleaves the readout map 𝓔ₓ(√π/2, Δ) that lifts the GKP logical info into the ancilla register, applies U_C(γ_k), transfers the relative phases back via 𝓔ₓ†, and then mixes via U_M directly on the oscillator phase space.

Section §IV reports the numerics. Setup: Erdős–Rényi graphs with edge probability 0.5, sizes N∈{4,5}, Fock cutoffs N_max∈{6,8,10,12}, QAOA depth P=2, mixer depth d=2, 20 random graph instances per (N, N_max). Two metrics: approximation ratio ⟨H_C⟩ / max_z ⟨z|H_C|z⟩ and optimal-solution probability P_opt = Σ_{z: C(z)=C_max} Pr(z). The headline results (§IV-B): the NA-QSP mixer yields a positive improvement in every (N, N_max) cell; averaged across cutoffs, the mean approximation-ratio improvement is ≈0.132 for N=4 and ≈0.128 for N=5, with corresponding P_opt improvements of ≈0.156 and ≈0.155.

Section §IV-C analyses the effect of mixer depth d and envelope Δ. The most dramatic gain happens at d=0 → d=1: at N_max=10 the mean P_opt jumps from 0.149 to 0.353 and the approximation ratio from 0.555 to 0.718. Further depth gives only marginal improvement, and at fixed depth performance saturates with N_max once the truncation is large enough. Larger Δ helps slightly (mean P_opt ≈0.438 at Δ=0.65, d=4) because broader GKP states are easier to represent in a truncated Fock space.

The conclusion (§V) frames the result as a design principle: algorithms on hybrid CV-DV hardware should exploit the native phase-space ISA rather than mimic qubit-only constructions. Future work flagged: more expressive non-Abelian mixers, trainability vs. depth, and larger problem instances.

Figures

Schematic of hybrid CV-DV processor
Figure 1. Schematic of a hybrid CV-DV quantum processor, illustrated with superconducting microwave resonators locally coupled to superconducting qubits and neighboring resonators coupled by beam splitters.
Hybrid CV-DV QAOA circuit
Figure 2. Hybrid CV-DV QAOA circuit. In each layer k, 𝓔ₓ(√π/2,Δ) couples GKP-encoded oscillator modes to the ancilla register, U_C(γₖ) applies graph-dependent phases, 𝓔ₓ† transfers the phases back to GKP, then the local non-Abelian mixers U_M^(i)(Θₖ) act on each pair. A final 𝓔ₓ is applied before qubit readout.
Approximation-ratio improvement vs Fock cutoff
Figure 3a. Improvement in approximation ratio of the NA-QSP mixer over the transverse-field baseline across Fock cutoffs N_max∈{6,8,10,12} and graph sizes N=4,5, over 20 random ER instances.
P_opt improvement vs Fock cutoff
Figure 3b. Improvement in optimal-solution probability P_opt of the NA-QSP mixer over the transverse-field baseline, same axes as Fig. 3a.
Performance vs mixer depth
Figure 3c. Mean approximation ratio (lines) and P_opt (bars) vs mixer depth d∈{0,1,2,3,4} at fixed N=4, Δ=0.45. d=0 is the transverse-field baseline.
Performance vs GKP envelope Δ
Figure 3d. Mean approximation ratio (lines) and P_opt (bars) vs GKP envelope parameter Δ∈{0.25,…,0.65} at fixed N=4, N_max=10.

Citations to Yuan's papers

No direct citation to any of Y1–Y6 found in bibliography.

Overlap with Y1–Y6

Recommended action for Yuan