A well-known argument in cosmology gives that the power spectrum (or structure function) P(k) of mass density fluctuations produced from a uniform initial state by physics which is causal (i.e. moves matter and momentum only up to a finite scale) has the behaviour P(k) k4 at small k. Noting the assumption of analyticity at k = 0 of P(k) in the standard derivation of this result, we introduce a class of solvable one-dimensional models which allows us to study the relation between the behaviour of P(k) at small k and the properties of the probability distribution f(l) for the spatial extent l of mass and momentum-conserving fluctuations. We find that the k4 behaviour is obtained in the case that the first six moments of f(l) are finite. Interestingly, the condition that the fluctuations be localised--taken to correspond to the convergence of the first two moments of f(l)--imposes only the weaker constraint P(k) kn with n anywhere in the range 0 < n <= 4. We interpret this result to suggest that the causality bound will be loosened in this way if quantum fluctuations are permitted.
Causality constraints on fluctuations in cosmology: A study with exactly solvable one-dimensional models
Andrea Gabrielli;
2004
Abstract
A well-known argument in cosmology gives that the power spectrum (or structure function) P(k) of mass density fluctuations produced from a uniform initial state by physics which is causal (i.e. moves matter and momentum only up to a finite scale) has the behaviour P(k) k4 at small k. Noting the assumption of analyticity at k = 0 of P(k) in the standard derivation of this result, we introduce a class of solvable one-dimensional models which allows us to study the relation between the behaviour of P(k) at small k and the properties of the probability distribution f(l) for the spatial extent l of mass and momentum-conserving fluctuations. We find that the k4 behaviour is obtained in the case that the first six moments of f(l) are finite. Interestingly, the condition that the fluctuations be localised--taken to correspond to the convergence of the first two moments of f(l)--imposes only the weaker constraint P(k) kn with n anywhere in the range 0 < n <= 4. We interpret this result to suggest that the causality bound will be loosened in this way if quantum fluctuations are permitted.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.