Frequency Reduced-Basis method: ROM for time-dependent problems

Standard reduced-order models for time-dependent problems build a basis from snapshots of the solution at successive time steps. For oscillatory or wave-like problems, this requires dense sampling over long time intervals — expensive, and still often insufficient to capture the full dynamics.

The Frequency Reduced-Basis (FRB) method samples in the frequency domain instead. Applying the Laplace transform converts the time-dependent problem into a set of independent elliptic problems parametrized by complex frequency. These can be solved in parallel, and the resulting basis is provably accurate for the time-dependent problem via a norm equivalence between the time and frequency domains (Paley-Wiener theorem).

Method

Offline stage (frequency domain):
  1. Apply Laplace transform to the PDE
       → elliptic problem: (s²M + A) û(s) = b̂(s) - su₀ - u₀'
  2. Sample frequencies: s_j = ζ + iλ cot(θ_j), θ_j ∈ (0,π)
  3. Solve each frequency problem independently (parallelisable)
  4. Build snapshot matrix S = {w_j û(s_j)}, w_j = 2λ/sin²(θ_j)
  5. Compute SVD of S → reduced basis Φ

Online stage (time domain):
  6. Project PDE onto span(Φ) → low-dimensional system
  7. Solve with any time integrator

Key properties:

  • Frequency solves are independent — fully parallelisable offline stage
  • Fewer samples needed for oscillatory problems than time-domain ROM
  • Basis construction is decoupled from the time discretization
  • Intrinsic stabilization for convection-dominated problems — no tuning required

Results

Wave equation in a polygonal domain — highly oscillatory solution with wave interference. The solution changes dramatically between time steps with no predictable pattern, making time-domain sampling inefficient.

Wave solution at three time steps Solution at t = 23, 24, 25. The interference pattern is complex and unpredictable.

Wave equation in a multi-ring domain — comparison of FRB against time-domain ROM with the same number of samples. The FRB accurately reproduces the solution; the time-domain ROM fails entirely.

Topology comparison: FE, time ROM, FRB symplectic, FRB real Top left: FE reference. Top right: time-domain ROM. Bottom left: FRB symplectic basis. Bottom right: FRB real basis.

Advection-dominated problem — the FRB solution is free of spurious oscillations with no explicit stabilization applied, performing comparably to VMS-stabilized finite element methods.

Advection stabilization comparison Top left: unstabilized FE. Top right: VMS. Bottom left: SUPG. Bottom right: FRB — oscillation-free without any stabilization.

Publication

R. Reyes, The Frequency Reduced-Basis method: reduced order models for time-dependent problems using the Laplace transform, Computational Mechanics, 2026. DOI: 10.1007/s00466-026-02795-6