Dc. Brody et Lp. Hughston, STATISTICAL GEOMETRY IN QUANTUM-MECHANICS, Proceedings - Royal Society. Mathematical, physical and engineering sciences, 454(1977), 1998, pp. 2445-2475
Citations number
55
Categorie Soggetti
Multidisciplinary Sciences
Journal title
Proceedings - Royal Society. Mathematical, physical and engineering sciences
A statistical model M is a family of probability distributions, charac
terized by a set of continuous parameters known as the parameter space
. This possesses natural geometrical properties induced by the embeddi
ng of the family of probability distributions into the space of all sq
uare-integrable functions. More precisely, by consideration of the squ
are-root density function we can regard M as a submanifold of the unit
sphere S in a real Hilbert space H. Therefore, H embodies the 'state
space' of the probability distributions, and the geometry of the given
statistical model, can be described in terms of the embedding of M in
S. The geometry in question is characterized by a natural Riemannian
metric (the Fisher-Rao metric), thus allowing us to formulate the prin
ciples of classical statistical inference in a natural geometric setti
ng. In particular, we focus attention on variance lower bounds for sta
tistical estimation, and establish generalizations of the classical Cr
amer-Rao and Bhattacharyya inequalities, described in terms of the geo
metry of the underlying real Hilbert space. As a comprehensive illustr
ation of the utility of the geometric framework, the statistical model
M is then specialized to the case of a submanifold of the state space
of a quantum mechanical system. This is pursued by introducing a comp
atible, complex structure on the underlying real Hilbert space, which
allows the operations of ordinary quantum mechanics to be reinterprete
d in the language of real Hilbert-space geometry. The application of g
eneralized variance bounds in the case of quantum statistical estimati
on leads to a set of higher-order corrections to the Heisenberg uncert
ainty relations for canonically conjugate observables.