Mass Distribution of M31 from Its Rotation Curve up to 167 kpc
4 affiliations
- 1Peking University
- 2University of Chinese Academy of
- 3Chinese Academy of Sciences
- 4Department of Scientific Research, Beijing Planetarium, Beijing 100044,
Abstract
The mass distribution of the Andromeda galaxy (M31) is fundamental for understanding its dark matter content, assembly history, and dynamical role within the Local Group. However, estimates of M31’s total mass remain quite uncertain, partly because of limited dynamical constraints at large galactocentric radii. Moreover, M31’s recent merger history has produced abundant tidal substructures and may have left its outer halo out of dynamical equilibrium, complicating equilibrium-based mass estimates. We use over 8500 tracers with line-of-sight velocities to constrain the rotation curve (RC) of M31 over R = 2–167 kpc. In the disk, we derive the RC from a clean tracer sample using the Jeans equation and find good agreement with previous H i measurements. In the halo, we use Gaussian mixture modeling to account for tidal substructures and Galactic foreground contamination and constrain the kinematics of the residual dynamically hot halo. Assuming this halo population can be treated as an equilibrium tracer, we infer the outer RC and constrain M31’s mass distribution for different velocity anisotropies β and dark matter halo profiles. The Navarro–Frenk–White (NFW) and Dekel–Zhao (DZ) models yield broadly consistent total masses ranging from 1.1 2 − 0.10 + 0.11 × 1 0 12 M ⊙ to 1.6 3 − 0.17 + 0.21 × 1 0 12 M ⊙ for β = 0.3–0.7. In contrast, the Einasto profile favors substantially lower masses of 0.4 1 − 0.06 + 0.09 to 0.8 6 − 0.16 + 0.21 × 1 0 12 M ⊙ , highlighting significant dependence on the adopted halo profile, although Einasto solutions are more in tension with independent mass estimates based on M31 satellite galaxies than the NFW and DZ models at fixed β . Overall, our analysis provides a comprehensive measurement of M31’s mass distribution under the assumption of dynamical equilibrium, while also quantifying the systematic uncertainties associated with halo velocity anisotropy and the choice of dark matter density profile.
Related
- A Unified HI Rotation Curve Database for 122 Dwarf and Irregular Galaxies
- A Self-Consistent Jeans Analysis of the Milky Way Rotation Curve
- A Self-consistent Jeans Analysis of the Milky Way Rotation Curve
- The Rotation Curve of the Milky Way: State of the Art, the Keplerian Decline Debate, and Implications for Dark Matter
- Reconciling Galactic rotation curve constraints with stellar stream modeling
BibTeX
@article{wu2026mass,
title = {{Mass Distribution of M31 from Its Rotation Curve up to 167 kpc}},
author = {Hao Wu and Yang Huang and Huawei Zhang and Qikang Feng and Cheng Liu},
journal = {The Astrophysical Journal},
year = {2026},
month = oct,
doi = {10.3847/1538-4357/aeab7f},
url = {https://iopscience.iop.org/article/10.3847/1538-4357/aeab7f},
note = {CC BY 4.0},
}
RIS
TY - JOUR
TI - Mass Distribution of M31 from Its Rotation Curve up to 167 kpc
AU - Hao Wu
AU - Yang Huang
AU - Huawei Zhang
AU - Qikang Feng
AU - Cheng Liu
PY - 2026
DA - 2026/10/21
JO - The Astrophysical Journal
DO - 10.3847/1538-4357/aeab7f
UR - https://iopscience.iop.org/article/10.3847/1538-4357/aeab7f
AB - The mass distribution of the Andromeda galaxy (M31) is fundamental for understanding its dark matter content, assembly history, and dynamical role within the Local Group. However, estimates of M31’s total mass remain quite uncertain, partly because of limited dynamical constraints at large galactocentric radii. Moreover, M31’s recent merger history has produced abundant tidal substructures and may have left its outer halo out of dynamical equilibrium, complicating equilibrium-based mass estimates. We use over 8500 tracers with line-of-sight velocities to constrain the rotation curve (RC) of M31 over R = 2–167 kpc. In the disk, we derive the RC from a clean tracer sample using the Jeans equation and find good agreement with previous H i measurements. In the halo, we use Gaussian mixture modeling to account for tidal substructures and Galactic foreground contamination and constrain the kinematics of the residual dynamically hot halo. Assuming this halo population can be treated as an equilibrium tracer, we infer the outer RC and constrain M31’s mass distribution for different velocity anisotropies β and dark matter halo profiles. The Navarro–Frenk–White (NFW) and Dekel–Zhao (DZ) models yield broadly consistent total masses ranging from 1.1 2 − 0.10 + 0.11 × 1 0 12 M ⊙ to 1.6 3 − 0.17 + 0.21 × 1 0 12 M ⊙ for β = 0.3–0.7. In contrast, the Einasto profile favors substantially lower masses of 0.4 1 − 0.06 + 0.09 to 0.8 6 − 0.16 + 0.21 × 1 0 12 M ⊙ , highlighting significant dependence on the adopted halo profile, although Einasto solutions are more in tension with independent mass estimates based on M31 satellite galaxies than the NFW and DZ models at fixed β . Overall, our analysis provides a comprehensive measurement of M31’s mass distribution under the assumption of dynamical equilibrium, while also quantifying the systematic uncertainties associated with halo velocity anisotropy and the choice of dark matter density profile.
SN - 0004-637X
SN - 1538-4357
ER -