- The paper introduces UMPIRE-Net, an ADMM-unrolled MRI reconstruction network that separately learns magnitude and sign priors with a smoothed, Nesterov-accelerated data-fidelity unit.
- UMPIRE-Net consistently outperforms a matched complex-valued baseline, achieving up to 1.77 dB higher PSNR, improved SSIM, and approximately 4° lower phase error at acceleration rates of 6 and 8.
- The results show that explicit phase-aware modeling can recover missing partial-Fourier k-space data under self-supervised training, although benefits decrease for noisier fat-saturated knee images.
UMPIRE-Net addresses a structural limitation of physics-driven deep learning (PD-DL) reconstruction for accelerated MRI: conventional unrolled networks regularize the complex-valued image with a single learned prior, implicitly coupling magnitude and phase. In partial Fourier (PF) imaging—where recovery of the omitted asymmetric k-space region depends critically on image phase—this coupling may be suboptimal. The paper, presented at the 2026 IEEE MLSP workshop (2608.14422), proposes an ADMM-unrolled network with separate learned proximal operators for magnitude and sign components, plus a differentiable data-fidelity (DF) unit tailored to this decomposition, and demonstrates consistent gains over a complex-valued PD-DL baseline under self-supervised training.
Classical PF methods such as homodyne reconstruction and POCS explicitly exploit phase information to synthesize missing asymmetric k-space samples. Prior separate magnitude/phase approaches either operate in non-DL optimization frameworks (CS with dedicated phase regularization, or phase cycling against phase wrapping) or place neural networks outside a physics-driven unrolled loop. UMPIRE-Net's positioning is to combine both: explicit magnitude/phase decomposition inside an algorithm-unrolling framework. The authors also note a practical training concern—in self-supervised setups such as MM-SSDU, the non-acquired PF region is excluded from the loss mask, giving the network limited direct supervision for recovering those samples; explicit phase modeling is hypothesized to mitigate this.
Method
The reconstruction problem is reformulated with independent regularizers on magnitude and sign:
argxmin∥yΩ−EΩx∥22+Rm(∣x∣)+Rp(∣x∣x)
Regularizing the sign rather than the phase follows prior CS work, since direct phase regularization yields a non-convex objective with spurious local minima from periodicity. ADMM splitting produces three subproblems: magnitude and sign proximal updates (implemented as neural networks) and a DF update that is itself non-convex due to the ∣⋅∣ and sign terms. The authors derive the Wirtinger (CR-calculus) gradient after replacing ∣x∣ with a quadratic smoothing approximation, (x⊙xH+ϵ)1/2, with ϵ scaled to the zero-filled image energy.
Because the DF subproblem is non-convex, plain gradient descent can stall in local minima. The paper therefore unrolls Nesterov-accelerated GD with learnable step sizes and momentum for the DF unit. All DF parameters (β1, β2, γ, steps ξ, dual coefficients λ1, ∣⋅∣0) are learned and unshared across the ∣⋅∣1 outer unrolls; the DF itself runs 10 inner iterations. Proximal networks use time-embedded U-Nets (TE-UNet) with a ReLU output constraint for magnitude non-negativity.
Experimental setup
Evaluation uses fastMRI coronal proton-density knee data with and without fat saturation (Cor-PD, Cor-PDFS), 300 training slices from 10 subjects and 392 test slices, with retrospective equispaced in-plane undersampling at ∣⋅∣2 (24 ACS lines) combined with PF ∣⋅∣3 along the phase-encoding direction. Training is multi-mask self-supervised (MM-SSDU, loss-mask ratio ∣⋅∣4) with the PF region held out of the training masks, using a normalized ∣⋅∣5-∣⋅∣6 loss. The conventional PD-DL baseline is a modified TE-UNet in the same ADMM unrolling with 10 CG iterations per DF step, isolating the contribution of the inverse-problem formulation and DF design.
Results
Across both datasets and both acceleration rates, UMPIRE-Net with Nesterov-accelerated DF achieves the best PSNR, SSIM, and phase accuracy. Representative numbers:
| Method |
Cor-PD R=6 PSNR/SSIM/∣⋅∣7 |
Cor-PD R=8 |
Cor-PDFS R=6 |
Cor-PDFS R=8 |
| Conv. PD-DL (CG) |
35.55 / 0.914 / 19.80° |
33.64 / 0.893 / 20.96° |
32.54 / 0.750 / 30.80° |
31.47 / 0.729 / 31.57° |
| UMPIRE (GD) |
36.42 / 0.914 / 16.60° |
35.11 / 0.896 / 16.90° |
32.69 / 0.763 / 27.55° |
32.18 / 0.746 / 28.79° |
| UMPIRE (Nesterov) |
36.76 / 0.919 / 15.93° |
35.41 / 0.902 / 16.82° |
32.83 / 0.768 / 26.78° |
32.26 / 0.763 / 27.43° |
The largest magnitude gains occur on Cor-PD at R=8 (+1.77 dB PSNR), and phase error drops consistently by roughly 4° across all settings. Notably, these gains are achieved under self-supervised training with no fully sampled reference, and the DF region is never directly supervised—supporting the claim that the decomposition itself improves inference of missing PF k-space. Gains on Cor-PDFS are milder, which the authors attribute to lower SNR and noisier phase; this is a candid limitation on how much benefit phase-aware regularization provides when phase estimation is intrinsically difficult. Qualitatively, residual artifacts from conventional PD-DL are partially reduced by UMPIRE with plain GD and eliminated with Nesterov acceleration, indicating the momentum-based DF is a material component of the result rather than an implementation detail.
An ablation of smoothing operators for the DF (Cor-PD, R=8) shows quadratic smoothing (35.11 dB / 0.896 SSIM) outperforming Huber (34.63 / 0.886) and Log-Exp (32.53 / 0.880), suggesting the specific smoothing choice near zero is consequential for the non-convex DF.
Limitations and open questions
The paper concedes several points. Evaluation is restricted to Cartesian knee data at PF ∣⋅∣8 with equispaced undersampling; generalization to other anatomies, trajectories, and PF factors is untested. The benefit shrinks on noisier, fat-saturated data, leaving open how the method behaves in strongly phase-varying regimes such as multi-echo or off-resonance imaging—exactly the settings the authors identify for future evaluation. The DF subproblem remains non-convex even with smoothing and Nesterov momentum, and no convergence guarantees are provided for the unrolled non-convex ADMM. The choice of sign (rather than phase) as the regularized component is inherited from CS practice and is not ablated against alternative decompositions.
Conclusion
UMPIRE-Net shows that decoupling magnitude and phase regularization within a physics-driven unrolled framework, paired with a smoothed, Nesterov-accelerated DF unit, yields measurable improvements—up to +1.77 dB PSNR and ~4° lower phase error—over a matched complex-valued PD-DL baseline for self-supervised partial Fourier MRI reconstruction. The results support the premise that explicit phase-aware modeling reduces reliance on externally estimated phase information, while leaving the extension to spatially varying phase applications and the theoretical behavior of the non-convex DF as open questions.