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Using Universal Frame Randomization and Randomized Compilation to Mitigate Errors in Quantum Optimization

Rachel E. Johnson, Joshua A. Job, Steve Adachi

TL;DR

This work addresses error mitigation for quantum optimization on NISQ devices by applying two twirling techniques—universal frame randomization and Randomized Compilation—to a QAOA circuit with $p=1$ solving a frustrated Ising ring. By implementing these methods on IBM superconducting hardware (with TKET for universal frame randomization and True-Q for randomized compilation) and comparing to simulators, the study demonstrates that both approaches can shift energy estimates closer to the noiseless baseline, achieving extremal energies of $5.25 \pm 0.145$ and $4.08 \pm 0.36$ respectively, versus $2.63 \pm 0.068$ without mitigation and $5.676 \pm 0.006$ for the noiseless case. The experimental setup maps a 12-node ring to 12 qubits and samples a 289-point parameter grid ($17 \times 17$) with $5000$ shots per circuit to build an energy landscape. Overall, the results indicate that universal frame randomization and Randomized Compilation are effective, practical error-mitigation strategies for QAOA on current quantum hardware, and motivate further exploration of combining techniques and tuning compilation counts for improved performance.

Abstract

Error mitigation is essential for near-term quantum devices, and two promising techniques are universal frame randomization and Randomized Compilation. These methods insert random twirling gates into a circuit to reduce errors while preserving unitarity and depth. We apply universal frame randomization and Randomized Compilation to the quantum approximate optimization algorithm (QAOA) with $p=1$ on a superconducting quantum circuit system, demonstrating its potential to improve energy calculations. Specifically, we investigate the use of QAOA to calculate the lowest energy state of a frustrated Ising ring system and compare the results of randomized circuits generated using both techniques. Our results show that both methods can mitigate errors, with expected extremal energy values of $5.25\pm0.145$ and $4.08\pm0.36$, for Randomized Compilation and universal frame randomization respectively, compared to $2.63\pm0.068$ without randomization and $5.676\pm0.006$ with a noiseless simulator.

Using Universal Frame Randomization and Randomized Compilation to Mitigate Errors in Quantum Optimization

TL;DR

This work addresses error mitigation for quantum optimization on NISQ devices by applying two twirling techniques—universal frame randomization and Randomized Compilation—to a QAOA circuit with solving a frustrated Ising ring. By implementing these methods on IBM superconducting hardware (with TKET for universal frame randomization and True-Q for randomized compilation) and comparing to simulators, the study demonstrates that both approaches can shift energy estimates closer to the noiseless baseline, achieving extremal energies of and respectively, versus without mitigation and for the noiseless case. The experimental setup maps a 12-node ring to 12 qubits and samples a 289-point parameter grid () with shots per circuit to build an energy landscape. Overall, the results indicate that universal frame randomization and Randomized Compilation are effective, practical error-mitigation strategies for QAOA on current quantum hardware, and motivate further exploration of combining techniques and tuning compilation counts for improved performance.

Abstract

Error mitigation is essential for near-term quantum devices, and two promising techniques are universal frame randomization and Randomized Compilation. These methods insert random twirling gates into a circuit to reduce errors while preserving unitarity and depth. We apply universal frame randomization and Randomized Compilation to the quantum approximate optimization algorithm (QAOA) with on a superconducting quantum circuit system, demonstrating its potential to improve energy calculations. Specifically, we investigate the use of QAOA to calculate the lowest energy state of a frustrated Ising ring system and compare the results of randomized circuits generated using both techniques. Our results show that both methods can mitigate errors, with expected extremal energy values of and , for Randomized Compilation and universal frame randomization respectively, compared to without randomization and with a noiseless simulator.

Paper Structure

This paper contains 9 sections, 2 equations, 11 figures, 1 table.

Figures (11)

  • Figure 1: Circuit and cycles for randomized compilation on a simple quantum circuit. Each cycle is circled with a dashed line.
  • Figure 2: Circuit with randomized frames around each cycle. Arbitrary random gates are inserted before and after each cycle to "frame" the cycle.
  • Figure 3: Frustrated Ising ring Roberts_2020. Nodes are connected by coupling terms denoted $J$, $J_L$, and $-J_R$. The negative coupling term causes frustration. Red nodes are in one state (spin up) and the blue node is in the other state (spin down).
  • Figure 4: Circuit diagram for QAOA. Gates parameterized by $\beta$ and $\gamma$ are iterated over the length of the circuit. The first complete layer of the circuit is circled with a dashed line.
  • Figure 5: Energy Landscape generated by running QAOA on a closed IBM quantum simulator with no noise model (Fall 2022).
  • ...and 6 more figures