In this paper we focus on understanding the physical processes that lead to stable or unstable ionization fronts (I-fronts) observed in simulations of moving black holes (BHs). The front instability may trigger bursts of gas accretion, rendering the BH significantly more luminous than at steady-state. We perform a series of idealized three dimensional radiation hydrodynamics simulations resolving the I-fronts around BHs of mass and velocity accreting from a medium of density . The I-front, with radius , transitions from D-type to R-type as the BH velocity becomes larger than a critical value $v_\sim 40,\Delta R_v_\inftyv_$. We find that both D-type and R-type fronts can be unstable given the following two conditions: i) for D-type fronts the shell thickness must be $\Delta R_/R_<0.05v_\infty \gtrsim 20,$.), while no similar restriction holds for R-type fronts; ii) the temperature jump across the I-front must be . This second condition is satisfied if or if . Due to X-ray pre-heating typically , unless the D-type shell is optically thick to X-rays, which also happens when is greater than a metallicity-dependent critical value. We thus conclude that I-fronts around BHs are unstable only for relatively massive BHs moving trough very dense molecular clouds. We briefly discuss the observational consequences of the X-ray luminosity bursts likely associated with this instability.

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