Erratum: Propagation of Second sound in a superfluid Fermi gas in the unitary limit [Phys. Rev. A 80, 043613 (2009)] Emiko Arahata and Tetsuro NikuniWe made some errors in Sec. IV. The correct interaction parameter is g B n B /k B T c = 0.807. The sound velocities plotted in Fig. 7 are normalized by the "Fermi velocity" defined in terms of the density and mass of bosons, i.e. v f = (6π 2 n B ) 1/3 /2M . Due to mishandling of raw data, the values given in Fig. 8 did not correspond to our calculated results. The corrected version of the figure is given as Fig. 0 below. The qualitative behaviors of W 1 and W 2 in the BEC limit are quite different from those in the unitary limit, i.e. W 2 > W 1 in most temperatures (T > 0.4T c ). This change does not affect any other result nor the conclusion of the paper. FIG. 0: W1/(W1 + W2) and W2/(W1 + W2) as a function of temperature.We study sound propagation in a uniform superfluid gas of Fermi atoms in the unitary limit.The existence of normal and superfluid components leads to appearance of two sound modes in the collisional regime, referred to as first and second sound. The second sound is of particular interest as it is a clear signal of a superfluid component. Using Landau's two-fluid hydrodynamic theory, we calculate hydrodynamic sound velocities and these weights in the density response function. The latter is used to calculate the response to a sudden modification of the external potential generating pulse propagation. The amplitude of a pulse which is proportional to the weight in the response function, is calculated the basis of the approach of Nozières and Schmitt-Rink (NSR) for the BCS-BEC crossover. We show that, in a superfluid Fermi gas at unitarity, the second sound pulse is excited with an appreciate amplitude by density perturbations.