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Towards an agnostic algorithm for sampling empirical structure models: The case of Uranus and Neptune

Stefano Wirth, Luca Morf, Ravit Helled

TL;DR

This work addresses the degeneracy in inferring planetary interior density profiles by proposing an agnostic, bias-minimizing sampling framework that abandons MCMC in favor of an optimization-based gradient-descent approach grounded in the Theory of Figures. Applied to Uranus and Neptune, the method yields ensembles of density and pressure profiles that reproduce observed mass, radius, and gravitational moments while revealing the full extent of solution-space diversity, especially in the deep interior. Key findings include median-density trends consistent with composition gradients, outer regions that are tightly constrained, and a systematic presence of density discontinuities around $r/R \\approx 0.65$ (Uranus) and $\\approx 0.70$ (Neptune), with the number and strength of discontinuities depending on the chosen criterion $c_D$. The approach offers a scalable, unbiased framework for exploring planetary interiors under limited data and can be extended to exoplanets, higher-order gravitational moments, and compositional analyses, advancing our ability to interpret gravitational-field data.

Abstract

We present an algorithm to efficiently sample the full space of planetary interior density profiles. Our approach uses as few assumptions as possible to pursue an agnostic algorithm. The algorithm avoids the common Markov Chain Monte Carlo method and instead uses an optimisation-based gradient-descent approach designed for computational efficiency. In this work, we use Uranus and Neptune as test cases and obtain empirical models that provide density and pressure profiles consistent with the observed physical properties (total mass, radius, and gravitational moments). We compare our findings to other work and find that while other studies are generally in line with our findings, they do not cover the entire space of solutions faithfully. Furthermore, we present guidance for modellers that construct Uranus or Neptune interior models with a fixed number of layers. We provide a statistical relation between the steepness classifying a density discontinuity and the resulting number of discontinuities to be expected. For example, if one classifies a discontinuity as a density gradient larger than 0.02 kg$\,$m$^{-4}$, then most solutions should have at most one such discontinuity. Finally, we find that discontinuities, if present, are concentrated around a planetary normalised radius of 0.65 for Uranus and 0.7 for Neptune. Our algorithm to efficiently and faithfully investigate the full space of possible interior density profiles can be used to study all planetary objects with gravitational field data.

Towards an agnostic algorithm for sampling empirical structure models: The case of Uranus and Neptune

TL;DR

This work addresses the degeneracy in inferring planetary interior density profiles by proposing an agnostic, bias-minimizing sampling framework that abandons MCMC in favor of an optimization-based gradient-descent approach grounded in the Theory of Figures. Applied to Uranus and Neptune, the method yields ensembles of density and pressure profiles that reproduce observed mass, radius, and gravitational moments while revealing the full extent of solution-space diversity, especially in the deep interior. Key findings include median-density trends consistent with composition gradients, outer regions that are tightly constrained, and a systematic presence of density discontinuities around (Uranus) and (Neptune), with the number and strength of discontinuities depending on the chosen criterion . The approach offers a scalable, unbiased framework for exploring planetary interiors under limited data and can be extended to exoplanets, higher-order gravitational moments, and compositional analyses, advancing our ability to interpret gravitational-field data.

Abstract

We present an algorithm to efficiently sample the full space of planetary interior density profiles. Our approach uses as few assumptions as possible to pursue an agnostic algorithm. The algorithm avoids the common Markov Chain Monte Carlo method and instead uses an optimisation-based gradient-descent approach designed for computational efficiency. In this work, we use Uranus and Neptune as test cases and obtain empirical models that provide density and pressure profiles consistent with the observed physical properties (total mass, radius, and gravitational moments). We compare our findings to other work and find that while other studies are generally in line with our findings, they do not cover the entire space of solutions faithfully. Furthermore, we present guidance for modellers that construct Uranus or Neptune interior models with a fixed number of layers. We provide a statistical relation between the steepness classifying a density discontinuity and the resulting number of discontinuities to be expected. For example, if one classifies a discontinuity as a density gradient larger than 0.02 kgm, then most solutions should have at most one such discontinuity. Finally, we find that discontinuities, if present, are concentrated around a planetary normalised radius of 0.65 for Uranus and 0.7 for Neptune. Our algorithm to efficiently and faithfully investigate the full space of possible interior density profiles can be used to study all planetary objects with gravitational field data.

Paper Structure

This paper contains 18 sections, 47 equations, 16 figures, 2 tables.

Figures (16)

  • Figure 1: Gravitational moment distribution for successful Uranus (\ref{['fig:Jsu']}) and Neptune (\ref{['fig:Jsn']}) profiles. Both panels include a 2D histogram where bins more frequently occupied by solutions are shown with a relatively darker colour. Additionally, 1D histograms display the weighted number of solutions along each axis. The weights were assigned to solutions based on a multivariate Gaussian likelihood, with means, standard deviations, and covariance taken from Table \ref{['tab:values']}. In the left panel \ref{['fig:Jsu']}, an orange distribution is shown in addition to the blue distribution. Both blue distributions in \ref{['fig:Jsu']} and \ref{['fig:Jsn']} assume $\mathrm{cov}(J_2,J_4)=0$, whereas the orange distribution for Uranus takes $\mathrm{cov}(J_2,J_4)=0.9861\,\sigma_{J_2}\sigma_{J_4}$.
  • Figure 2: Solution space distribution (\ref{['fig:densprofu']}) and contour of the distribution (\ref{['fig:contouru']}) for Uranus. The left panel \ref{['fig:densprofu']} shows the weighted distribution of all successful uncorrelated Uranus density profiles. The inset shows a zoomed-in view of the outermost region, from $r/R=1$ to $r/R=0.7$. Note that the zoom is not aspect-preserving. The colour scale shows the relative frequency over all distributions of a certain density value at a given radius. Coloured lines show density profiles from previous studies for comparison. Solid and dashed lines correspond to models U1 and U2 from Nettelmann2013 (orange); U1 and U3 from Morf2025 (green); and V2 and V3 from Vazan2020 (blue), respectively. The colour scale in the right panel \ref{['fig:contouru']} shows the percentile intervals in 10% increments, except the last interval, where a 95% interval was added. The black line shows the median. The dashed lines show the 16th (lower) and 84th (upper) percentiles.
  • Figure 3: Same as Figure \ref{['fig:distru']} but for Neptune. The solid and dashed line in the left panel \ref{['fig:densprofn']} correspond to the models N1 and N2b from Nettelmann2013 (orange) and to models N1 and N3 from Morf2025 (green), respectively.
  • Figure 4: Central densities. The black lines are as before in Figures \ref{['fig:contouru']} and \ref{['fig:contourn']}. The red line denotes the average. This figure is equivalent to a side-on view of the density profile distributions (Figures \ref{['fig:densprofu']} and \ref{['fig:densprofn']}) at radius 0, except in linear scale. Note that the distribution is cut off at $\rho_{max}=$ 20000 kg m$^{-3}$.
  • Figure 5: Confidence intervals. Size of the 68% and 95% confidence intervals in Figures \ref{['fig:contouru']} and \ref{['fig:contourn']} for the successful density profile distributions. The plot is cumulative, where the size of the 95% confidence interval is the purple and the orange area combined.
  • ...and 11 more figures

Theorems & Definitions (4)

  • definition 1: Jump
  • definition 2: Maximally steep jump
  • definition 3: Jump cluster
  • definition 4: Discontinuity