A black hole (BH) communicates information about its event area to an observer. This defines an information channel. We show that if the area is optimally encoded, the probability law on its square root follows approximate exponential decay, and the resulting entropy is precisely the Bekenstein–Hawking result including the important factor of 1/4. This result arises as well as the solution to: (a) maximum entropy subject to a fixed message length, or (b) minimum Fisher information subject to a normalization condition. A verifiable prediction is a randomly enlarged event area, implying a randomly enlarged irreducible mass value. These effects should be observable as an enhanced number of BH’s with large mass, resulting in an increased occurrence of gravitational lensing, and an enhanced ability to entrap relatively distant stellar objects.

A coarse-grained Wigner distribution p(W)(x,mu) obeying positivity derives out of information-theoretic considerations. Let p(x,mu) be the unknown joint probability density function (PDF) on position and momentum fluctuations x, mu for a particle in a pure state psi(x). Suppose that the phase part Psi(x,z) of its Fourier transform T-F[p(x,mu)]equivalent to parallel to G(x,z)parallel to exp[i Psi(x,z)] is constructed as a hologram. (Such a hologram is often used in heterodyne interferometry.) Consider a particle randomly illuminating this phase hologram. Let its two position coordinates be measured. Require that the measurements contain an extreme amount of Fisher information about true position, through variation of the phase function Psi(x,z). The extremum solution gives an output PDF p(x,mu) that is the convolution of the Wigner p(W)(x,mu) with an instrument function defining uncertainty in either position x or momentum mu. The convolution arises naturally out of the approach, and is one dimensional, in comparison with the ad hoc two-dimensional convolutions usually proposed for coarse graining purposes. The output obeys positivity, as required of a PDF, if the one-dimensional instrument function is sufficiently wide. The result holds for a large class of systems: those whose amplitudes psi(x) are the same at their boundaries [examples: states psi(x) with positive parity; with periodic boundary conditions; free particle trapped in a box].