The gravitational interactions between the LMC and the Milky Way can give rise to dynamical perturbations in the MW halo, leading to a biased distribution of stellar density and other kinematic signals. These disequilibrium phenomena exhibit variations under different parameter combinations of the MW-LMC model. In this work, we run 50 high-resolution N-body simulations spanning different masses and halo shapes of the Milky Way and LMC and investigate how the LMC-induced perturbations evolve with these model parameters. We measure the magnitude of kinematic perturbations from the mean velocities of simulated halo stars and identify a discontinuity between the first-infall and second-passage scenarios of the LMC's orbital history. We demonstrate that, due to the short dynamical times of the Galactic inner halo, the reduced perturbation magnitude in the second-passage scenario is mainly a result of the LMC's second infall into the MW, which starts at a much lower velocity relative to the inner halo compared to the first-infall scenario. Using a subset of ~ 1200 RR Lyrae stars located in the outer halo (50 ≤ RGC < 100 kpc), which are selected from a larger sample of 135,873 RR Lyrae stars with precise distance estimates from Gaia, we find the mean latitudinal velocity (vb) in the heliocentric frame to be vb = 30.8 ± 4.0 km/s. The observation contradicts the second-passage scenario and supports the first-infall scenario with a massive LMC (~ 2.1 × 10¹¹ M_) at infall, an oblate MW halo with a virial mass M₂₀₀ < 1.4 × 10¹² M_ and a flattening parameter $q > 0.7$.
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Sheng et al. (2024) studied this question.
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