We investigate the dynamics of correlation propagation in the one-dimensional Fermi-Hubbard model with SU() symmetry when the repulsive-interaction strength is quenched from a large value, at which the ground state is a Mott-insulator with filling, to an intermediate value. From approximate analytical insights based on a simple model that captures the essential physics of the doublon excitations, we show that entanglement in the initial state leads to collective enhancement of the propagation velocity when , becoming equal to the velocity of the Bose-Hubbard model in the large- limit. These results are supported by numerical calculations of the density-density correlation in the quench dynamics for and .

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