Quantum Implicit-Explicit Schemes for Multiscale Ordinary and Partial Differential Equations via Schrödingerization

TL;DR

Proposes a Schrödingerization-based quantum IMEX scheme with parameter-independent complexity for multiscale PDEs.

math.NA 🔴 Advanced 2026-05-28 94 views
Qitong Hu Xiaoyang He Shi Jin Xiao-Dong Zhang
Quantum Algorithms IMEX Schemes Schrödingerization Multiscale PDEs Quantum Simulation

Key Findings

Methodology

This work introduces a quantum IMEX scheme integrated with Schrödingerization, employing a continuous-time formulation to decouple quantum evolution from physical time. The approach transforms the IMEX discretization into a higher-dimensional linear system, then uses continuous-time Richardson iteration to solve it. Schrödingerization maps non-Hermitian operators into Hermitian form, enabling efficient quantum simulation via phase estimation. Numerical validation on linear heat and multiscale telegraph equations demonstrates the scheme’s independence from the scale parameter ε, with complexity bounds of O(T/δ · (log δ^{-1})^3). The auxiliary register width is optimized to logarithmic levels, significantly reducing hardware overhead compared to HHL-based methods.

Key Results

  • Numerical experiments show the query complexity remains stable as ε approaches zero, outperforming HHL-type algorithms which depend linearly on ε^{-1}. The auxiliary register width is reduced to O(log log δ^{-1}), easing hardware demands. The scheme maintains high accuracy across multiple scales, with complexity bounds independent of ε, confirming its suitability for multiscale PDEs.
  • In heat and telegraph equations, the method achieves parameter-free complexity, with practical advantages in auxiliary register size and robustness. The experimental results validate the theoretical claims, demonstrating that the approach effectively handles stiff and multiscale problems with reduced quantum resource requirements.
  • Overall, the scheme offers a scalable, parameter-agnostic quantum solver for PDEs, with potential applications in climate modeling, fluid dynamics, and quantum chemistry, where multiscale phenomena are prevalent.

Significance

This research addresses a fundamental bottleneck in quantum PDE solvers—the explicit dependence on the scale parameter ε. By integrating IMEX schemes with Schrödingerization, it provides a robust, parameter-independent framework that can handle stiff and multiscale systems efficiently. The approach bridges the gap between classical asymptotic-preserving methods and quantum algorithms, paving the way for practical large-scale quantum simulations in scientific computing. Its ability to reduce hardware overhead while maintaining accuracy marks a significant step toward real-world quantum advantage in complex system modeling.

Technical Contribution

The core technical innovation lies in reformulating IMEX discretizations into continuous-time ODEs solved via Schrödingerization, achieving parameter independence. The method employs a novel continuous-time Richardson iteration, decoupling evolution time from physical scales. It also optimizes auxiliary register size by leveraging Fourier mode analysis, reducing the quantum resource footprint. Theoretical guarantees on stability, convergence, and complexity bounds are established, extending quantum simulation capabilities to multiscale PDEs with minimal ε-dependence.

Novelty

This work is the first to embed IMEX schemes within the Schrödingerization framework, effectively removing the explicit ε dependence that hampers previous quantum algorithms. Unlike prior HHL-based approaches, it achieves near-optimal complexity with reduced auxiliary register requirements. The continuous-time reformulation and parameter-free complexity bounds represent a significant innovation, enabling scalable quantum solutions for multiscale PDEs that were previously intractable.

Limitations

  • The current scheme primarily targets linear PDEs; extension to nonlinear or strongly nonlinear systems remains an open challenge. Hardware limitations, such as qubit count and gate fidelity, restrict immediate practical deployment. The method’s performance in extremely stiff or highly oscillatory regimes needs further validation. Additionally, the approach assumes certain spectral conditions, which may not hold universally, requiring further robustness analysis.

Future Work

Future research will focus on extending the framework to nonlinear PDEs, improving robustness under less restrictive spectral conditions, and optimizing quantum circuit implementations for near-term hardware. Exploring adaptive schemes and error mitigation strategies will be key to practical deployment. Long-term goals include integrating this approach into broader quantum simulation platforms, enabling real-time multiscale modeling in physics, chemistry, and engineering.

AI Executive Summary

This paper introduces a groundbreaking quantum IMEX scheme based on Schrödingerization, designed to solve multiscale PDEs efficiently without dependence on the small scale parameter ε. Traditional quantum algorithms like HHL or Hamiltonian simulation face exponential complexity growth as ε approaches zero, limiting their practical use for stiff or highly oscillatory problems. To overcome this, the authors develop a novel continuous-time reformulation of the IMEX discretization, transforming the problem into a higher-dimensional linear system that can be efficiently simulated on a quantum computer.

The key innovation is the use of Schrödingerization to map non-Hermitian operators arising from the discretized PDEs into Hermitian form, enabling phase estimation-based simulation. By employing a continuous-time Richardson iteration, the scheme decouples the quantum evolution time from the physical time, ensuring the complexity remains stable regardless of the scale parameter. The auxiliary register size is optimized to logarithmic levels, significantly reducing hardware overhead compared to existing HHL-based methods.

Numerical experiments on linear heat and multiscale telegraph equations demonstrate the scheme’s ability to handle stiff problems with parameter-independent complexity bounds of O(T/δ · (log δ^{-1})^3). The results validate the theoretical advantages, showing that the approach maintains high accuracy while requiring fewer quantum resources. This work paves the way for scalable, practical quantum algorithms for complex multiscale systems, with potential applications across physics, chemistry, and engineering.

Looking ahead, the authors plan to extend their framework to nonlinear PDEs, improve robustness under less restrictive spectral conditions, and adapt the algorithms for near-term quantum hardware. Overall, this research marks a significant step toward realizing quantum advantage in scientific computing, offering a promising route to tackle some of the most challenging problems in multiscale modeling.

Deep Dive

Abstract

In this paper, we present a quantum implicit-explicit (IMEX) scheme for multiscale ordinary and partial differential equations whose discretization parameters are independent of the scaling parameter $\varepsilon$. A key ingredient of our approach is a continuous-time formulation of classical IMEX schemes, which decouples the evolution time of the quantum algorithm from the physical time of the differential equation and is therefore particularly useful in multiscale settings. Building on this idea, we employ the Schrödingerization framework [Phys. Rev. Lett. 133 (2024), 230602] to implement IMEX schemes on quantum computers. Compared to previous HHL type quantum AP scheme [J. Comput. Phys. 471 (2022), 111641], this new method requires narrower -- an extra logarithmic factor -- auxiliary register numerical examples on linear heat and multiscale telegraph equations demonstrate the independence in $\varepsilon$ of the method.

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