Abstract
This paper reexamines the statistical quantum field theory of a free, minimally coupled, real scalar field Φ in a statically bounded, classical Friedmann cosmology, where the time-dependent scale factor Ω(t) tends to constant values Ω1 and Ω2 for t<t1 and t>t2. The principal objective is to investigate the intuition that ‘‘entropy’’ S correlates with average particle number 〈N〉, so that increases in 〈N〉 induced by parametric amplification manifest a one-to-one connection with increases in S. The definition of particle number Nk becomes unambiguous for t>t2 and t<t1, where the spacetime is static, the spatial modes ±k for early and late times being coupled by Bogoliubov coefficients αk and βk.