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) proportional to k(4) 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(1) for the spatial extent I of mass and momentum-conserving fluctuations. We find that the k(4) 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) proportional to k(n) with n anywhere in the range 0 < n less than or equal to 4. We interpret this result to suggest that the causality bound will be loosened in this way if quantum fluctuations are permitted.
Gabrielli, A., Joyce, M., Marcos, B., Viot, P. (2004). Causality constraints on fluctuations in cosmology: A study with exactly solvable one-dimensional models. EUROPHYSICS LETTERS, 66(1), 1-7 [10.1209/epl/i2003-10150-y].
Causality constraints on fluctuations in cosmology: A study with exactly solvable one-dimensional models
Gabrielli A.
;
2004-01-01
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) proportional to k(4) 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(1) for the spatial extent I of mass and momentum-conserving fluctuations. We find that the k(4) 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) proportional to k(n) with n anywhere in the range 0 < n less than or equal to 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.