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February 20, 2026Monthly Notices of the Royal Astronomical Society2 citationsOpen Access

BayeSN-TD: Time Delay and H 0 Estimation for Lensed SN H0pe

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MGMatthew GraylingSTS ThorpKMK S Mandel

Key Points

  • The central goal is to enhance the estimation of time delays and H0 for lensed type Ia supernovae using a probabilistic model.
  • Development of the BayeSN-TD software for modeling gravitationally lensed SN Ia.
  • Fitting for magnifications and time delays across multiple images while accounting for microlensing effects.
  • Application of BayeSN-TD to the photometry of the glSN Ia SN H0pe.
  • Inferred time delays of 121.9 days between images BA and 63.2 days between images BC.
  • Calculated absolute magnifications: β_A = 2.38, β_B = 5.27, β_C = 3.93.
  • Estimated H0 values of 69.3 km s−1 Mpc−1 and 66.8 km s−1 Mpc−1 with additional constraints.

Abstract

Abstract We present BayeSN-TD, an enhanced implementation of the probabilistic type Ia supernova (SN Ia) BayeSN SED model, designed for fitting multiply-imaged, gravitationally lensed type Ia supernovae (glSNe Ia). BayeSN-TD fits for magnifications and time-delays across multiple images while marginalising over an achromatic, Gaussian process-based treatment of microlensing, to allow for time-dependent deviations from a typical SN Ia SED caused by gravitational lensing by stars in the lensing system. BayeSN-TD is able to robustly infer time delays and produce well-calibrated uncertainties, even when applied to simulations based on a different SED model and incorporating chromatic microlensing, strongly validating its suitability for time-delay cosmography. We then apply BayeSN-TD to publicly available photometry of the glSN Ia SN H0pe, inferring time delays between images BA and BC of T₁₀=121. 9^+9. 5-₇. ₅ days and T₁₂=63. 2^+3. 2-₃. ₃ days along with absolute magnifications β for each image, A = 2. 38^+0. 72-₀. ₅₄, B=5. 27^+1. 25-₁. ₀₂ and C=3. 93^+1. 00-₀. ₇₅. Combining our constraints on time-delays and magnifications with existing lens models of this system, we infer H₀=69. 3^+12. 6-₇. ₈ km s−1 Mpc−1, consistent with previous analysis of this system; incorporating additional constraints based on spectroscopy yields H₀=66. 8^+13. 4-₅. ₄ km s−1 Mpc−1. While this is not yet precise enough to draw a meaningful conclusion with regard to the ‘Hubble tension’, upcoming analysis of SN H0pe with more accurate photometry enabled by template images, and other glSNe, will provide stronger constraints on H0; BayeSN-TD will be a valuable tool for these analyses. The BayeSN-TD code is available at https: //github. com/bayesn/bayesn-td.

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Cite This Study

Grayling et al. (2026) studied this question.

synapsesocial.com/papers/6997f9ddad1d9b11b3452ad9https://doi.org/10.1093/mnras/stag340
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