Given IMBH mass and stellar cusp, compute expected proper-motion wander and compare against Gaia DR4 and Roman Space Telescope astrometric floors.
Using current σ_★ and D from sliders. Mass fixed at each scenario value.
Merritt (2001) showed that an IMBH embedded in a stellar cusp will reach equipartition with the surrounding stars. By kinetic energy equipartition: M_BH × ⟨v_BH²⟩ = ⟨m_★⟩ × σ_★² (one-dimensional, each component). This gives:
v_BH_rms = σ_★ × √(⟨m_★⟩ / M_BH)
The transverse (sky-plane) velocity component is v_t = v_BH_rms (one dimension). Proper motion in µas/yr uses the conversion: μ[µas/yr] = v_t[km/s] / (4.74 × D[kpc]) × 1000.
Gaia DR4: single-epoch proper motion floor ~15 µas/yr for bright stars; systematic photocenter ~30 µas over 5-year baseline. Detectable if μ > 15 µas/yr, marginal 5–15, undetectable <5.
Roman Space Telescope: projected narrow-field astrometry ~1 µas/yr. Detectable if μ > 1 µas/yr, marginal 0.3–1.
ngEHT/VLBI: ~10 µas absolute astrometry floor for the brightest compact sources.
Merritt 2001 (AJ 121:2385) — Brownian motion of massive black holes in stellar cusps. Häberle et al. 2024 (Nature 631:285) — IMBH mass ≥ 8,200 M☉ from fast-star kinematics. Bañares-Hernández et al. 2025 (A&A 693:A104) — IMBH mass upper bound ≤ 6,000 M☉ from proper motions. Gaia Collaboration 2022 (A&A 616:A1) — Gaia astrometry performance.