  We put forward an attempt towards building a possible theoretical model to
understand the observer dependent thermalization of black hole horizon. The
near horizon Hamiltonian for a massless, chargeless particle is $xp$ type. This
is unstable in nature and so the horizon can induce instability in a system.
The particle in turn finds the horizon thermal when it interacts with it. We
explicitly show this in the Schrodinger as well as in Heisenberg pictures by
taking into account the time evolution of the system under this Hamiltonian.
Hence we postulate that existing instability near the horizon can be one of the
potential candidates for explaining the black hole thermalization.
