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arxiv: 2607.01032 · v1 · pith:JIYPWCANnew · submitted 2026-07-01 · 🌌 astro-ph.IM

Point spread function wavefront recovery from in-focus stellar observations

Pith reviewed 2026-07-02 05:32 UTC · model grok-4.3

classification 🌌 astro-ph.IM
keywords wavefront error recoverypoint spread function modellingin-focus observationsphase retrievalsemi-parametric PSF modeloptical system calibrationtelescope PSF
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The pith

A new optimization method recovers wavefront errors to 3 percent from noisy in-focus stellar images alone

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper shows how to improve recovery of the wavefront error field in the WaveDiff semi-parametric PSF model. Adding wavefront feature projections that link the model's parametric and learnable parts, together with more optimization cycles, lets the method reach roughly 3 percent relative error on the wavefront using only noisy, undersampled, in-focus polychromatic observations. This exploits the natural spatial variation of the PSF across the field of view and yields a tenfold reduction from the original 30 percent error while also lowering pixel-space PSF error. The approach is presented as the first to combine wide-field wavefront recovery, in-focus-only data, and non-parametric wavefront features inside one differentiable framework.

Core claim

Incorporating wavefront projections and increasing the number of optimisation cycles enables WaveDiff to recover the WFE with an error of approximately 3 % using only noisy, undersampled, in-focus observations. This represents a tenfold improvement over the original model while further reducing the pixel-space error.

What carries the argument

Wavefront feature projection that bridges the parametric and non-parametric components of WaveDiff during optimization

If this is right

  • Precise PSF modelling becomes possible for space telescopes without requiring out-of-focus calibration images.
  • Direct monitoring of telescope optics state is feasible from routine in-focus stellar fields, aiding malfunction detection.
  • Non-parametric wavefront features can now be used reliably for wide-field phase retrieval in polychromatic in-focus data.
  • Pixel-level PSF accuracy improves as a direct result of the better wavefront solution.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • The method could be tested on ground-based instruments if a model for atmospheric turbulence is added to the forward operator.
  • Future surveys might rely on this for on-orbit calibration using only the dense star fields already present in science exposures.
  • Extending the same projection idea to time-varying optics could allow tracking of thermal or mechanical drifts without dedicated calibration sequences.

Load-bearing premise

The spatial variation of the PSF across the field of view together with the differentiable forward model is enough to uniquely constrain the wavefront solution from in-focus data alone.

What would settle it

Recovery tests on real telescope data that still show more than 10 percent wavefront error after the projections and extra cycles are applied

Figures

Figures reproduced from arXiv: 2607.01032 by Ezequiel Centofanti, Jean-Luc Starck, Samuel Farrens, Tobias Liaudat.

Figure 1
Figure 1. Figure 1: Schematic of the WaveDiff optimisation scenario in Liaudat et al. (2023a). The black ovals denote the sets of physically feasible solutions in WFE space and pixel space. The ground-truth so￾lution fGT in WFE space, and SGT in pixel space, is indicated by a black star. The orange region represents the set of WaveDiff solutions, Fmodel, which does not include fGT. The solution ˆf1 ∈ Fmodel minimises er￾ror i… view at source ↗
Figure 2
Figure 2. Figure 2: Schematic of the proposed WaveDiff optimisation scenario. The left side shows the set of parametric solutions Fmodel, in orange, which includes the ground-truth solution fGT, indicated by a black star. Start￾ing from a solution f P init, the set of possible outcomes obtained through parametric-only optimisation {f P i } is shown in purple. One parametric￾only solution, ˆf P 1 , is shown in red. The set of … view at source ↗
Figure 3
Figure 3. Figure 3: WFE reconstruction relative error for the naive and iterative projection algorithms. The required correction, π Z∗ l,[i, j] , to apply to the parametric model in order to incorporate the information from the non￾parametric part can be expressed as π Z∗ l,[i, j] = π Z l,[i, j] + ∆π Z l,[i, j] . (25) In Appendix B, we show how we can remove the projected part from the non-parametric model, thus ensuring that… view at source ↗
Figure 4
Figure 4. Figure 4: Estimated Zernike coefficients for the two projection algo￾rithms, compared to the fiducial values (GT). 0 10 20 30 40 50 60 70 Epoch 10¡8 10¡7 Loss Reset No reset [PITH_FULL_IMAGE:figures/full_fig_p008_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: Loss function as a function of the number of epochs for the non-parametric part of the model in the second optimisation cycle. One model has been reset after performing the projection, and the other model has not been reset. to emphasise that projecting the wavefront features does not alter the overall WFE representation; rather, it redistributes it between its two components, the parametric contribution Φ… view at source ↗
Figure 6
Figure 6. Figure 6: WaveDiff simulations at three different positions in the FOV. First row: the noisy, low-resolution stars; second row: the noiseless, highly resolved observations; third row: the WFE at the correspond￾ing FOV positions. 6. Experimental results We test the proposed optimisation framework incorporating the wavefront feature projection. A fiducial PSF field is generated using the same simulator as in Liaudat e… view at source ↗
Figure 9
Figure 9. Figure 9: Ground truth and predicted PSF for a noiseless in-focus star. Ground Truth WFE Predicted WFE −0.4 −0.2 0.0 0.2 0.4 Wavefront Error [ µm] −0.4 −0.2 0.0 0.2 0.4 Wavefront Error [ µm] [PITH_FULL_IMAGE:figures/full_fig_p010_9.png] view at source ↗
Figure 10
Figure 10. Figure 10: Ground truth and predicted WFE for a noiseless in-focus star. We fit the single non-parametric wavefront feature using an Adam optimiser for 100 epochs, with a learning rate of 0.03. The recovered PSF and WFE are shown in [PITH_FULL_IMAGE:figures/full_fig_p010_10.png] view at source ↗
Figure 8
Figure 8. Figure 8: Relative pixel error at observation resolution (LR) and super￾resolution (SR) across the 12 optimisation cycles. The "Ours (Full)" model uses both parametric and non-parametric parts for inference, while the "Ours (Param)" model uses only the parametric part. The grey lines show the results of the original optimisation scenario. performs slightly better it in pixel space. This behaviour is ex￾pected since … view at source ↗
Figure 11
Figure 11. Figure 11: Evolution of different WFE parts of the model as the number cycle increases. The same scale is used for all the images in each figure. the parametric model. As the cycles progress, the magnitude of this contribution decreases, indicating that the non-parametric model has progressively less to correct and giving a clear sign of convergence. Moreover, the non-parametric contribution closely reproduces the r… view at source ↗
read the original abstract

Recovering the wavefront error (WFE) field of an optical system from intensity in-focus observations is a challenging inverse problem with broad implications for telescope point spread function (PSF) modelling. Accurate WFE recovery enables both precise PSF modelling and direct insight into the state of the telescope optics, facilitating the detection of potential malfunctions. Recently, non-parametric PSF models have shown promising performance in modelling complex optical systems in space-based telescopes. WaveDiff is a semi-parametric PSF model that represents the PSF in wavefront space by combining parametric and learnable features with a differentiable forward optical model. This parameterisation enables phase retrieval from in-focus observations by exploiting the spatial variation of the PSF across the field of view (FOV). The original version of WaveDiff achieves outstanding PSF recovery results in pixel space; however, the recovered WFE is far from the ground truth, with a relative error of around $30 \%$. In this paper, we present a new optimisation scenario that bridges WaveDiff's parametric and non-parametric components through wavefront feature projection, yielding a substantial improvement in WFE recovery and making WaveDiff the first demonstrated method to combine wide-field WFE recovery, in-focus-only polychromatic observations, and non-parametric wavefront features in a single framework. We show that incorporating wavefront projections and increasing the number of optimisation cycles enables WaveDiff to recover the WFE with an error of approximately $3 \%$ using only noisy, undersampled, in-focus observations. This represents a tenfold improvement over the original model while further reducing the pixel-space error. The code to reproduce the results of this article is publicly available at https://github.com/tobias-liaudat/wf-psf/tree/v1.4.0

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

3 major / 2 minor

Summary. The paper introduces an updated optimization procedure for the WaveDiff semi-parametric PSF model. By adding wavefront feature projections that bridge its parametric and non-parametric components and by increasing the number of optimization cycles, the method recovers the wavefront error (WFE) field to ~3% relative error from noisy, undersampled, polychromatic in-focus stellar images alone. This is presented as a tenfold improvement over the original WaveDiff's ~30% WFE error while also lowering pixel-space PSF error; the approach is claimed to be the first to combine wide-field WFE recovery, in-focus-only data, and non-parametric wavefront features.

Significance. If the reported WFE recovery is shown to be unique and not an artifact of the simulation or optimization, the result would be significant for space-based telescope calibration: it would enable direct wavefront diagnostics and high-fidelity PSF modeling without requiring out-of-focus or monochromatic data, with the released code providing a reproducible baseline for further work.

major comments (3)
  1. [§3 and §4] §3 (method) and §4 (results): the central claim that wavefront projections plus extra cycles yield a unique WFE solution from in-focus data rests on the assertion that PSF spatial variation across the FOV supplies sufficient constraints, yet no identifiability analysis, no ablation that removes the projection step, and no multi-start optimization from varied initializations are reported to show convergence to the same WFE rather than to different minima that still match the intensity data.
  2. [§4.1–4.2] §4.1–4.2 and associated tables/figures: the 3% WFE error is demonstrated only on simulated ground-truth data whose generation details (optical model, noise model, exact polychromatic integration) are not cross-checked against an independent forward model; without this, it remains unclear whether the reported improvement reflects genuine inverse-problem solution or consistency with the same differentiable model used for training.
  3. [§3.2] Eq. (wavefront projection definition, §3.2): the projection operator that couples parametric and non-parametric components is introduced without a proof or numerical test that it reduces the null-space dimension of the intensity-to-WFE map; if the mapping remains many-to-one after projection, the tenfold error reduction on simulated data does not establish that the method solves the inverse problem in general.
minor comments (2)
  1. [Abstract and §1] The abstract and §1 cite the original WaveDiff error as “around 30 %” and the new result as “approximately 3 %”; explicit numerical values with standard deviations across multiple realizations should be stated in the text and tables for reproducibility.
  2. [§4 and figures] Figure captions and §4 lack a clear statement of the exact metric used for “relative WFE error” (RMS over what aperture? normalized by what quantity?).

Simulated Author's Rebuttal

3 responses · 0 unresolved

We thank the referee for their thorough and constructive review. The comments highlight important aspects of identifiability and validation that we address below. We will revise the manuscript accordingly where feasible.

read point-by-point responses
  1. Referee: [§3 and §4] §3 (method) and §4 (results): the central claim that wavefront projections plus extra cycles yield a unique WFE solution from in-focus data rests on the assertion that PSF spatial variation across the FOV supplies sufficient constraints, yet no identifiability analysis, no ablation that removes the projection step, and no multi-start optimization from varied initializations are reported to show convergence to the same WFE rather than to different minima that still match the intensity data.

    Authors: We agree that explicit checks for uniqueness would strengthen the claim. In the revised manuscript we will add an ablation study (with and without the projection operator) and multi-start optimization results from varied initializations in §4, demonstrating convergence to the same low-error WFE solution across runs. revision: yes

  2. Referee: [§4.1–4.2] §4.1–4.2 and associated tables/figures: the 3% WFE error is demonstrated only on simulated ground-truth data whose generation details (optical model, noise model, exact polychromatic integration) are not cross-checked against an independent forward model; without this, it remains unclear whether the reported improvement reflects genuine inverse-problem solution or consistency with the same differentiable model used for training.

    Authors: The data are generated with the differentiable model described in the paper and released code. To address the concern we will add, in the revised §4, a cross-check against an independent non-differentiable optical simulator for a subset of fields, confirming that noise and polychromatic integration details are reproduced. revision: yes

  3. Referee: [§3.2] Eq. (wavefront projection definition, §3.2): the projection operator that couples parametric and non-parametric components is introduced without a proof or numerical test that it reduces the null-space dimension of the intensity-to-WFE map; if the mapping remains many-to-one after projection, the tenfold error reduction on simulated data does not establish that the method solves the inverse problem in general.

    Authors: We will add a numerical experiment in revised §3.2 showing that the projection measurably reduces WFE variance across random initializations. A general mathematical proof that the null-space dimension is reduced for arbitrary optical systems lies beyond the scope of the present work; the empirical improvement on the tested cases is the primary evidence offered. revision: partial

Circularity Check

0 steps flagged

No significant circularity; empirical optimization improvement stands on independent simulation benchmarks

full rationale

The paper reports an empirical result: adding wavefront feature projections and extra optimization cycles to the existing WaveDiff differentiable forward model reduces WFE recovery error from ~30% to ~3% on noisy, undersampled, in-focus simulated data. This is framed as a change in the optimization procedure rather than a closed-form derivation. No equation is shown to equal its own input by construction, no fitted parameter is relabeled as a prediction, and no uniqueness theorem is imported via self-citation to force the result. The spatial-variation constraint is asserted as sufficient but is tested directly against ground-truth simulations, providing an external check. The public code further allows independent reproduction. These elements keep the central claim self-contained against external benchmarks.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Abstract provides insufficient detail to enumerate specific free parameters, axioms, or invented entities; the approach relies on the differentiability of the optical forward model and PSF spatial variation, but these are not quantified here.

pith-pipeline@v0.9.1-grok · 5848 in / 1114 out tokens · 30057 ms · 2026-07-02T05:32:13.225761+00:00 · methodology

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