Abstract

Motivated by the recent progress in time-resolved nonequilibrium spectroscopy in condensed matter, we study an optically excited one-dimensional ionic Hubbard model by exact diagonalization. The model is relevant to organic crystals, transition metal oxides, or ultracold atoms in optical lattices. We implement numerical pump-probe measurements to calculate time-dependent conductivity and single-particle spectral functions. In general, short optical excitation induces a metallic behavior imprinted as a Drude peak in conductivity or an in-gap density of states. In a Mott insulator, we find that the induced Drude peak oscillates at the pump frequency and its second harmonic. The former comes from the oscillation of currents, and the latter from the interference of single- and three-photon excited states. In a band insulator, the Drude peak oscillates only at the pump frequency, and quantities such as the double occupancy do not oscillate. The absence of the second harmonic oscillation is due to the degeneracy of multi-photon excited states. The in-gap density of states in both insulators correlates with the Drude weight and the energy absorption for weak pumping. Strong pumping leads to saturation of the in-gap density of states and to suppression of the Drude weight in the Mott regime. We have also checked that the above features are robust for insulators in the intermediate parameter range. Our study demonstrates the distinct natures of the multi-photon excited states in two different insulators.

Highlights

  • Nonequilibrium properties of strongly correlated electron systems have been an intense research topic for many decades [1, 2, 3, 4, 5, 6, 7]

  • In a Mott insulator, we find that the induced Drude peak oscillates at the pump frequency and its second harmonic

  • We find that the Drude peak oscillates at the pump frequency ωp = 6.1, which comes from the current oscillation

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Summary

Introduction

Nonequilibrium properties of strongly correlated electron systems have been an intense research topic for many decades [1, 2, 3, 4, 5, 6, 7]. Resultant states after optical excitation are far away from equilibrium, and various time-dependent spectroscopic measurements are employed to analyze the transient states, e.g., time-domain THz spectroscopy [14], time-resolved photoemission spectroscopy [15, 16], or time-dependent X-ray diffraction [17, 18]. They have been applied to systems such as high-Tc superconductors [10], manganites [8], or organic compounds [9], and have discovered intriguing phenomena. DMRG gives very accurate results for one-dimensional systems, and extensions to higher-dimensions are possible [40]

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