ID: cond-mat/0409002

Momentum space anisotropy in doped Mott insulators

September 1, 2004

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Pseudogap in Doped Mott Insulators is the Near-neighbour Analogue of the Mott Gap

September 5, 2002

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Tudor D. Stanescu, Philip Phillips
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We show that the strong coupling physics inherent to the insulating Mott state in 2D leads to a jump in the chemical potential upon doping and the emergence of a pseudogap in the single particle spectrum below a characteristic temperature. The pseudogap arises because any singly-occupied site not immediately neighbouring a hole experiences a maximum energy barrier for transport equal to $t^2/U$, where $t$ is the nearest-neighbour hopping integral and $U$ the on-site repulsion...

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Strong particle-hole asymmetry of charge instabilities in doped Mott insulators

January 25, 2014

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Matias Bejas, Andres Greco, Hiroyuki Yamase
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We study possible charge instabilities in doped Mott insulators by employing the two-dimensional t-J model with a positive value of the next nearest-neighbor hopping integral t' on a square lattice, which is applicable to electron-doped cuprates. Although the d-wave charge density wave (flux phase) and d-wave Pomeranchuk instability (nematic order) are dominant instabilities for a negative t' that corresponds to hole-doped cuprates, we find that those instabilities are strong...

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Antiferromagnetism and d-wave superconductivity in (doped) Mott insulators: A wave function approach

April 17, 2003

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Z. Y. Weng, Y. Zhou, V. N. Muthukumar
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We propose a class of wave functions that provide a unified description of antiferromagnetism and d-wave superconductivity in (doped) Mott insulators. The wave function has a Jastrow form and prohibits double occupancies. In the absence of holes, the wave function describes antiferromagnetism accurately. Off diagonal long range order develops at finite doping and the superconducting order parameter has d-wave symmetry. We also show how nodal quasiparticles and neutral spin ex...

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Asymmetry of the electron spectrum in hole-doped and electron-doped cuprates

September 20, 2005

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Huaiming Guo, Shiping Feng
Superconductivity
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Within the t-t'-J model, the asymmetry of the electron spectrum and quasiparticle dispersion in hole-doped and electron-doped cuprates is discussed. It is shown that the quasiparticle dispersions of both hole-doped and electron-doped cuprates exhibit the flat band around the (\pi,0) point below the Fermi energy. The lowest energy states are located at the (\pi/2,\pi/2) point for the hole doping, while they appear at the (\pi,0) point in the electron-doped case due to the elec...

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Doping dependence of charge dynamics in electron-doped cuprates

April 20, 2004

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Tianxing Ma, Huaiming Guo, Shiping Feng
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Within the t-t'-J model, the doping dependence of charge dynamics in electron-doped cuprates is studied. The conductivity spectrum shows a pseudogap structure with a low-energy peak appearing at $\omega\sim 0$ and an rather sharp midinfrared peak appearing around $\omega\sim 0.3\mid t\mid$, and the resistivity exhibits a crossover from the high temperature metallic-like to low temperature insulating-like behavior in the relatively low doped regime, and a metallic-like behavio...

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Spin Liquid State around a Doped Hole in Insulating Cuprates

April 16, 1999

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T. Tohyama, Y. Shibata, S. Maekawa, Z. -X. Shen, ... , Miller L. L.
Strongly Correlated Electron...
Superconductivity

The numerically exact diagonalization study on small clusters of the t-J model with the second- and third- neighbor hopping terms shows that a novel spin liquid state is realized around a doped hole with momentum k=(pi,0) and energy \sim 2J compared with that with (pi/2,pi/2) in insulating cuprates, where the spin and charge degrees of freedom are approximately decoupled. Our finding implies that the excitations in the insulating cuprates are mapped onto the the d-wave resona...

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Ab initio description of magnetic polarons in a Mott insulator

December 18, 2019

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Emil Blomquist, Johan Carlström
Strongly Correlated Electron...
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Polarons are among the most elementary quasiparticles of interacting quantum matter, consisting of a charge carrier dressed by an excited background. In Mott insulators, they take the form of a dopant surrounded by a distorted spin-background and are expected to dictate effective mass, transport properties and interactions between carriers. Despite the fundamental importance of polarons for the electronic structure of strongly correlated systems, access to their internal stru...

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Bosonic resonating valence bond wave function for doped Mott insulators

February 25, 2005

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Z. Y. Weng, Y. Zhou, V. N. Muthukumar
Strongly Correlated Electron...
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We propose a new class of ground states for doped Mott insulators in the electron second-quantization representation. They are obtained from a bosonic resonating valence bond (RVB) theory of the t-J model. At half filling, the ground state describes spin correlations of the S=1/2 Heisenberg model very accurately. Its spin degrees of freedom are characterized by RVB pairing of spins, the size of which decreases continuously as holes are doped into the system. Charge degrees of...

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Variational wave function for an anisotropic single-hole-doped $t$-$J$ ladder

September 3, 2015

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Qing-Rui Wang, Zheng Zhu, ... , Weng Zheng-Yu
Strongly Correlated Electron...
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Based on three general guiding principles, i.e., no double occupancy constraint, accurate description of antiferromagnetism at half-filling, and the precise sign structure of the $t$-$J$ model, a new ground state wave function has been constructed recently [Weng, New J. Phys. 13, 103039 (2011)]. In this paper, we specifically study such kind of variational ground state for the one-hole-doped anisotropic two-leg $t$-$J$ ladder using variational Monte Carlo (VMC) method. The re...

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Doping dependent quasiparticle band structure in cuprate superconductors

November 5, 1996

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R. Eder, Y. Ohta, G. A. Sawatzky
Superconductivity

We present an exact diagonalization study of the single particle spectral function in the so-called t-t'-t''-J model in 2D. As a key result, we find that unlike the `pure' t-J model, hole doping leads to a major reconstruction of the quasiparticle band structure near (pi,0): whereas for the undoped system the quasiparticle states near (pi,0) are deep below the top of the band at (pi/2,pi/2), hole doping shifts these states up to E_F, resulting in extended flat band regions cl...

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