Abstract. This paper analyses wave propagation in a one-dimensional random medium with long-range correlations. The asymptotic regime where the fluctuations of the medium parameters are small and the propagation distance is large is studied. In this regime pulse propagation is characterized by a random time shift described in terms of a fractional Brownian motion and a deterministic spreading described by a pseudo-differential operator. This operator is characterized by a frequency-dependent attenuation that obeys a power law with an exponent ranging from 1 to 2 that is related to the power decay rate of the autocorrelation function of the fluctuations of the medium parameters. This frequency-dependent attenuation is associated with a frequency-dependent phase, which ensures causality of the filter that realizes the approximation. A discussion is provided showing that the mean-field theory cannot capture the correct attenuation rate, this is because it also averages the random time delay. Numerical results are given to illustrate the accuracy of the asymptotic theory.Key words. wave propagation, random media, long-range processes.1. Introduction. Wave propagation in multiscale and rough media, with longrange fluctuations, has recently attracted a lot of attention, as more and more data collected in real environments confirm that this situation can be encountered in many different contexts, such as in geophysics [11] or in laser beam propagation through the atmosphere [13,16,25]. Recently it has been shown that the main effect of such fluctuations of the medium parameters is a random time shift for the wave front, that obeys a Gaussian statistics described in terms of a fractional Brownian motion [22]. Here we observe the wave front along its random characteristics and we show that the wave front also experiences a deterministic shape modification, that can be described in terms of a pseudo-differential operator that depends on the power decay rate of the autocorrelation function of the fluctuations of the medium parameters. These results extend to general long-range media the ones derived in the context of a discrete Goupillaud medium in [26].The effective pseudo-differential operator obtained in this paper gives rise to a frequency-dependent attenuation that obeys a power law with an exponent ranging from 1 to 2. This exponent will be shown to be related to the exponent of the power decay rate of the autocorrelation function of the fluctuations of the medium parameters. Frequency-dependent attenuation has been observed in a wide range of applications in acoustics [4,29], and also in other domains, such as seismic wave propagation [7,8]. Experimental observations show that the attenuation of plane acoustic waves has a frequency dependence of the form E = E 0 exp(−γ(ω)z), where E denote the amplitude of an acoustic variable such as velocity or pressure and ω is the frequency. The damping coefficient has been seen to obey the empirical power law γ(ω) = γ 0 |ω| γ1 where γ 0 ∈ (0, ∞) and γ 1 ∈ (0, 2) are parameters ...