The basic assumption of the induced gravity approach is that Einstein theor
y is an effective, low energy-form of a quantum theory of constituents. In
this approach the Bekenstein-Hawking entropy S-BH Of a black hole can be in
terpreted as a measure of the loss of information about constituents inside
the black hole horizon. To be more exact, S-BH is determined by quantum co
rrelations between "observable" and "non-observable" states with positive a
nd negative energy E, respectively. It is important that for non-minimally
coupled constituents E differs from the canonical Hamiltonian H. This expla
ins why previous definitions of the entanglement entropy in terms of H fail
ed to reproduce S-BH.