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Possible hidden phases in photo-doped Mott insulators
December 11, 2023 @ 09:45 - 10:15 CET
Y. Murakami1
1Center for Emergent Matter Science, RIKEN, Wako, Saitama 351-0198, Japan
Doping charge carriers into Mott insulators provides a pathway to produce intriguing emergent phenomena. In equilibrium systems, doping can be chemically controlled. On the other hand, photo-doping, where particles are excited across the Mott gap, provides an alternative way. Compared to chemical-doping, photo-doping creates a wider variety of charge carriers, which may lead to the emergence of fascinating nonequilibrium states. In particular, when the gap is large, the lifetime of photo-carriers is exponentially enhanced, leading to quasi-steady states after intraband cooling of photo-carriers.
In this talk, we explore possible hidden phases that arise as quasi-steady states of photodoped Mott insulators using the quasi-equilibrium approach [1]. Within this approach, we treat the photo-doped state as an equilibrium state of an effective model for a given photo-doping level. We apply the idea to the 1D extended Hubbard model. In the first part [1], we present our numerical results obtained with the infinite time-evolving block decimation. We show the emergence of the so-called η-pairing phase and the string charge-density-wave phase, and discuss their physical properties. In the second part [2], we reveal the analytical aspects of these photo-doped states. We show that the corresponding wave function in the large on-site interaction limit can be expressed as , which indicates the separation of spin, charge and η−spin degrees of freedoms. Here η−spin represents the type of the photo-carriers, i.e. doublons and holons. This state is analogous to the celebrated Ogata-Shiba state of the doped Hubbard model in equilibrium. The expression provides us useful insight into the properties of the photo-doped states. Our results demonstrate that the emergent degrees of freedom activated by photo-doping can lead to peculiar types of quantum states absent in equilibrium.