We study the quantum paraelectric-ferroelectric transition near a quantum critical point, emphasizing the role of temperature as a finite size effect in time. The influence of temperature near quantum criticality may thus be likened to a temporal Casimir effect. The resulting finite-size scaling approach yields $frac{1}{T^2}$ behavior of the paraelectric susceptibility ($chi$) and the scaling form $chi(omega,T) = frac{1}{omega^2} F(frac{omega}{T})$, recovering results previously found by more technical methods. We use a Gaussian theory to illustrate how these temperature-dependences emerge from a microscopic approach; we characterize the classical-quantum crossover in $chi$, and the resulting phase diagram is presented. We also show that coupling to an acoustic phonon at low temperatures ($T$) is relevant and influences the transition line, possibly resulting in a reentrant quantum ferroelectric phase. Observable consequences of our approach for measurements on specific paraelectric materials at low temperatures are discussed.
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