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Reconstructing the Type Ia Supernova Absolute Magnitude with Two-Probe Physics-Informed Neural Networks

Denitsa Staicova

Abstract

We apply two variants of Physics-Informed Neural Networks (PINNs) to reconstruct the Type Ia supernova absolute magnitude $M_B(z)$ from joint BAO and supernova data under four cosmological models ($Λ$CDM, CPL, GEDE, $Λ_s$CDM) and two DESI DR2 fiducial sets. A heteroscedastic single-network method tested across four constraint configurations establishes that the Etherington distance duality relation is more fundamental constraint than cosmological model priors, with DDR violations of 30--52 mmag under physical constraints versus 85--2330 mmag without. Under full constraints all models recover $M_B \approx -19.3$ mag with biases below 0.05 mag. A Fisher information-weighted two-network variant trains independent networks on BAO and SN data, providing clean probe separation and finding no significant $M_B$ evolution in $z \in [0.3, 1.5]$. The heteroscedastic method identifies a persistent $2-3σ$ residual at $z \sim 0.4-0.5$ that is consistent across all four models and both fiducials; the Fisher method finds no significant pointwise deviation in $z\in[0.3,1.5]$ but shows a systematic separation of redshift-binned $M_B$ distributions consistent with the same underlying tension. While the origin of this feature remains ambiguous, its model-independence and cross-method consistency warrant further investigation with forthcoming data.

Reconstructing the Type Ia Supernova Absolute Magnitude with Two-Probe Physics-Informed Neural Networks

Abstract

We apply two variants of Physics-Informed Neural Networks (PINNs) to reconstruct the Type Ia supernova absolute magnitude from joint BAO and supernova data under four cosmological models (CDM, CPL, GEDE, CDM) and two DESI DR2 fiducial sets. A heteroscedastic single-network method tested across four constraint configurations establishes that the Etherington distance duality relation is more fundamental constraint than cosmological model priors, with DDR violations of 30--52 mmag under physical constraints versus 85--2330 mmag without. Under full constraints all models recover mag with biases below 0.05 mag. A Fisher information-weighted two-network variant trains independent networks on BAO and SN data, providing clean probe separation and finding no significant evolution in . The heteroscedastic method identifies a persistent residual at that is consistent across all four models and both fiducials; the Fisher method finds no significant pointwise deviation in but shows a systematic separation of redshift-binned distributions consistent with the same underlying tension. While the origin of this feature remains ambiguous, its model-independence and cross-method consistency warrant further investigation with forthcoming data.
Paper Structure (35 sections, 28 equations, 6 figures, 4 tables)

This paper contains 35 sections, 28 equations, 6 figures, 4 tables.

Figures (6)

  • Figure 1: Goodness-of-fit summary for all models, configurations, and fiducials on the Pantheon+ dataset. Left and centre: $\chi^2/\mathrm{dof}$ for BAO and SN Ia (diagonal errors), respectively, on a shared logarithmic scale. The dotted line marks $\chi^2/\mathrm{dof} = 1$. Right: total variation $\sum|\Delta M_B(z)|$ of the reconstructed $M_B(z)$ curve, a measure of high-frequency oscillation. Filled circles indicate DESI+CMB fiducial; open triangles indicate DESI+PP. Colours denote the constraint configuration: H-TT (blue), H-TF (green), H-FT (red), H-FF (purple). See text for a discussion on the outliers
  • Figure 2: Summary of reconstructed mean $M_B$ for all models, configurations, and fiducials on the Pantheon+ dataset. Left panel shows DESI+CMB, right: DESI+PP. Colours denote the cosmological model; marker shapes denote the constraint configuration. Thick error bars show the scatter-based standard error on the mean $\sigma_\mathrm{err}$; thin error bars show the epistemic uncertainty from the network $\sigma_\mathrm{ep}$. The dashed line and the shaded band marks $M_{B,\mathrm{fid}} = -19.3 \pm 0.5$ mag.
  • Figure 3: Significance of $M_B(z)$ deviation from its mean value $|M_B(z) - \langle M_B\rangle|/\sigma_{M_B}$, for H-TT (solid) and H-TF (dashed) configurations. Left panel: DESI+CMB fiducial; right panel: DESI+PP fiducial. Colors indicate cosmological model. Gray shading marks the $< 1\sigma$ region. Horizontal dotted lines indicate $1\sigma$, $3\sigma$, and $5\sigma$ thresholds. The uncertainty $\sigma_{M_B}$ is the observationally-floored standard error of the mean per redshift bin (Eq. \ref{['eq:sigma_floor']}). The plot is restricted to $0.15 < z < 2$ where SN Ia coverage is reliable.
  • Figure 4: $M_B$ distributions reconstructed by the Fisher two-network method, colour-coded by redshift bin ($z \in [0.0, 0.3]$, $[0.3, 0.8]$, $[0.8, 1.5]$, $[1.5, 2.5]$). Top row: DESI+CMB fiducial; bottom row: Pantheon+ (DESI+PP) fiducial. GEDE and CPL show broader distributions reflecting additional dark energy freedom.
  • Figure 5: $\Delta M_B(z) = M_B(z) - M_B^\mathrm{fid}$ reconstructed by the Fisher method. Left: DESI+CMB fiducial; right: DESI+PP fiducial. Shaded bands show $1\sigma$ uncertainties. All models are consistent with zero deviation in $z \in [0.3, 2]$. The oscillatory feature at $z \lesssim 0.2$ is data-driven and common to all models. At $z > 1.5$ models diverge as SN coverage becomes sparse and reconstruction relies on BAO.
  • ...and 1 more figures