Cuprate d-wave superconductivity based on Non perturbative many body theory for spin fluctuation
Abstract
We employ the nonperturbative many-body spin GW method to compute the single-particle Green's function, and the covariance method to evaluate the two-body correlation functions, for the Hubbard model of superconductors. The method, benchmarked at strong coupling and low temperatures, allows simulations on lattices up to 64×64, thereby enabling access to the thermodynamic limit. We find the key transition temperatures---namely the Néel temperature and the superconducting critical temperature Tc---to be in quantitative agreement with experimental data. Above the d-wave superconducting dome, there exists a broad pseudogap region in which the normal-state excitations are suppressed. These results indicate our approach may offer a new route toward investigating strongly correlated systems, especially cuprate superconductors.
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BibTeX
@misc{gong2026cuprate,
title = {{Cuprate d-wave superconductivity based on Non perturbative many body theory for spin fluctuation}},
author = {Jianwei Gong and Junnian Xiong and Ruitao Xiao and Hui Li and Ziyu Li and Huaqing Huang and Dingping Li},
howpublished = {arXiv},
year = {2026},
month = aug,
doi = {10.48550/arxiv.2607.04168},
eprint = {2607.04168},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2607.04168},
note = {CC BY 4.0},
}
RIS
TY - UNPB
TI - Cuprate d-wave superconductivity based on Non perturbative many body theory for spin fluctuation
AU - Jianwei Gong
AU - Junnian Xiong
AU - Ruitao Xiao
AU - Hui Li
AU - Ziyu Li
AU - Huaqing Huang
AU - Dingping Li
PY - 2026
DA - 2026/08/31
PB - arXiv
DO - 10.48550/arxiv.2607.04168
UR - https://arxiv.org/abs/2607.04168
AB - We employ the nonperturbative many-body spin GW method to compute the single-particle Green's function, and the covariance method to evaluate the two-body correlation functions, for the Hubbard model of superconductors. The method, benchmarked at strong coupling and low temperatures, allows simulations on lattices up to 64×64, thereby enabling access to the thermodynamic limit. We find the key transition temperatures---namely the Néel temperature and the superconducting critical temperature T_c---to be in quantitative agreement with experimental data. Above the d-wave superconducting dome, there exists a broad pseudogap region in which the normal-state excitations are suppressed. These results indicate our approach may offer a new route toward investigating strongly correlated systems, especially cuprate superconductors.
ER -