  A new thermalization scenario for heavy ion collisions is discussed. It is
based on the Hawking--Unruh effect: an observer moving with an acceleration $a$
experiences the influence of a thermal bath with an effective temperature $T =
a / 2\pi$, similar to the one present in the vicinity of a black hole horizon.
In the case of heavy ion collisions, the acceleration is caused by a pulse of
chromo--electric field $E \sim Q_s^2/g$ ($Q_s$ is the saturation scale, and $g$
is the strong coupling), the typical acceleration is $a \sim Q_s$, and the heat
bath temperature is $T \simeq Q_s / 2\pi \sim 200$ MeV. In nuclear collisions
at sufficiently high energies the effect can induce a rapid thermalization over
the time period of $\tau \sim \pi/Q_s $ accompanied by phase transitions. A
specific example of chiral symmetry restoration induced by the chromo--electric
field is considered; it is mathematically analogous to the phase transition
occurring in the vicinity of a black hole.
