2026A&A...705A.186D


Query : 2026A&A...705A.186D

2026A&A...705A.186D - Astronomy and Astrophysics, volume 705A186 (2026/1-1)

The light curve model fitting of Large Magellanic Cloud Cepheids: MESA-RSP versus Stellingwerf's code predictions.

DEKA M., MARCONI M., MOLINARO R., DE SOMMA G., BHARDWAJ A., TRENTIN E., DEB S., SICIGNANO T., MUSELLA I., RIPEPI V., LUONGO E. and KANBUR S.M.

Abstract (from CDS):

Context. A major challenge in modeling classical Cepheids is the treatment of convection, particularly its complex interplay with pulsation. This inherently three-dimensional (3D) process is typically approximated in one-dimensional (1D) hydrocodes, using dimensionless turbulent convection (TC) free parameters. Calibrating these parameters is essential for reproducing key observational features, such as the light curve amplitudes, secondary bumps, and the red edge of the instability strip (IS).
Aims. In this work, we calibrate the TC parameters adopted from the publicly available Modules for Experiments in Stellar Astrophysics-Radial Stellar Pulsations (MESA-RSP) code. We carried out a comparison using both the observational data of classical Cepheids and stellar parameter constraints from the Stellingwerf code. This is one of the few codes currently available that are capable of replicating a wide range of observed features of the classical pulsators.
Methods. We computed the multiband (V, I, and Ks) MESA-RSP light curves for 18 observed Large Magellanic Cloud (LMC) Cepheids, using stellar parameters determined on the basis of Stellingwerf's code. By fine-tuning the mixing-length and eddy viscosity parameters, we calibrated the TC treatment in MESA-RSP. We compared the resulting period-luminosity (PL), period-radius (PR), and period-mass-radius (PMR) relations with the prediction of Stellingwerf's model.
Results. We successfully reproduced the multiband (V, I, and Ks) light curves for 18 observed LMC Cepheids using the stellar parameters determined with Stellingwerf's code. We also finetuned the mixing-length and eddy viscosity parameters in MESA-RSP. Our models yielded PL, PR, and PMR relations that were consistent with the previous results. Interestingly, although our results are broadly in agreement with previous works, we explicitly identified distinct mass-luminosity (ML) relations for fundamental-mode (FU) and first-overtone (FO) Cepheids for the first time. This suggests that the macroscopic phenomena affecting the ML relation depend on the stellar mass itself and/or on the effective temperature range. Our investigation is focused on the calibration of the TC parameters, but we did not find a single set of convective parameter values that was sufficient to reproduce all the light curves. In addition, no statistically significant correlation was found between the stellar properties (e.g., the effectives temperature or the stellar mass) and the convection parameters, although subtle trends for the period and effective temperature have been noted. As for the inferred Cepheid distances, our application of the model-fitting technique yields reddened distance moduli, in good agreement with those reported in previous works. This result is not surprising, given that we adopted the same input stellar parameters, with only minor differences in the adopted model atmospheres.

Abstract Copyright: © The Authors 2026

Journal keyword(s): stars: distances - stars: fundamental parameters - stars: variables: Cepheids

Simbad objects: 20

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Number of rows : 20
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 NAME Magellanic Clouds GrG 03 00 -71.0           ~ 7988 0
2 SV* HV 2249 cC* 04 58 48.2636693328 -67 19 07.926287628     14.034   13.278 ~ 23 0
3 OGLE LMC-CEP-813 cC* 05 03 39.0113377104 -68 48 11.832525432   15.15 14.544 14.15 13.814 ~ 13 0
4 SV* HV 5589 cC* 05 06 39.1443126432 -68 57 46.980876888   16.37 15.868 15.49 15.155 ~ 22 0
5 SV* HV 5594 cC* 05 08 48.3739004760 -66 55 04.241068788   15.37 14.353   13.437 ~ 28 0
6 OGLE LMC-CEP-1124 cC* 05 09 29.7546031512 -68 58 15.405573360   16.43 15.812 15.30 14.993 ~ 22 0
7 OGLE LMC-CEP-1310 cC* 05 14 16.2321867552 -69 19 47.400580200     14.709   13.996 ~ 15 0
8 SV* HV 2431 cC* 05 17 06.9593547072 -70 06 24.657075828     15.194   14.440 ~ 9 0
9 OGLE LMC-CEP-1481 cC* 05 17 10.0099748448 -68 52 19.481567052   17.754 17.278   16.599 ~ 12 0
10 OGLE LMC-CEP-1523 cC* 05 18 01.4226427176 -71 09 11.038337928     16.883   16.271 ~ 13 0
11 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
12 SV* HV 2527 cC* 05 25 39.1090655328 -71 06 39.848203476   15.49 14.615 14.16 13.670 ~ 44 0
13 OGLE LMC-CEP-2012 cC* 05 26 49.9980347040 -69 45 52.857388944     15.061   14.136 ~ 28 0
14 SV* HV 2540 cC* 05 26 55.8896763936 -69 58 48.789627708     13.615 13.28 12.581 ~ 30 0
15 OGLE LMC-CEP-2138 cC* 05 29 28.1571268344 -71 09 23.994988308     16.206   15.460 ~ 16 0
16 SV* HV 2789 cC* 05 41 36.2324577576 -69 41 37.035217572     14.307   13.349 ~ 21 0
17 OGLE LMC-CEP-3004 cC* 05 42 44.1592017936 -68 33 15.319321848     17.154   16.474 ~ 13 0
18 SV* HV 12645 cC* 05 45 21.0656886144 -70 49 06.543410016     15.385   14.650 ~ 15 0
19 OGLE LMC-CEP-3113 cC* 05 45 35.3154599424 -70 42 29.506876596     16.082   15.338 ~ 15 0
20 OGLE LMC-CEP-3131 cC* 05 46 02.3310034080 -71 11 29.622709716     17.010   16.367 ~ 12 0

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