General Relativity: An Introduction for Physicists · Problem 16.12

Inflationary cosmology — Hobson, Efstathiou & Lasenby

Physics · stochastic-inflation-quantum-fluctuations

Problem

Consider an inflationary domain (or mini-universe in the context of Exercise 16.10) of initial radius H−1H^{-1}, in which the value of the scalar field ϕ≫1\phi \gg 1. In a time interval Δt=H−1\Delta t = H^{-1}, show that classically, in the slow-roll approximation, the value of ϕ\phi will change by Δϕ≈−2ϕ.\Delta\phi \approx -\frac{2}{\phi}. Assuming that the typical amplitude of quantum fluctuations in the scalar field is δϕ≈H/(2π)\delta\phi \approx H/(2\pi), show that δϕ≈12πV(ϕ)3.\delta\phi \approx \frac{1}{2\pi}\sqrt{\frac{V(\phi)}{3}}. Hence, for the case V(ϕ)=12m2ϕ2V(\phi) = \tfrac{1}{2}m^2\phi^2, show that the decrease in the value of the scalar field due to its classical motion is less than changes due to quantum fluctuations generated in the same time interval, provided that ϕ≫6m.\phi \gg \frac{6}{\sqrt{m}}. Assuming that the typical wavelength of the quantum fluctuation is δϕ\delta\phi is H−1H^{-1}, show that, after a time interval Δt=H−1\Delta t = H^{-1}, the original domain becomes effectively divided into e3∼20e^3 \sim 20 domains of radius H−1H^{-1}, each containing a roughly homogeneous scalar field ϕ+Δϕ+δϕ\phi + \Delta\phi + \delta\phi. Thus, on average, the volume of the universe containing a growing ϕ\phi-field increases by a factor ∼10\sim 10 after every time interval Δt=H−1\Delta t = H^{-1}. Note: This is the mechanism underlying stochastic inflation.

Related theory

Browse the problem library