Enhanced pair correlation functions in the two-dimensional Hubbard model

In this study we have computed the pair correlation functions in the two-dimensional Hubbard model using a quantum Monte Carlo method. We employ a new diagonalization algorithm in the quantum Monte Carlo method which is free from the negative sign problem. We show that the d-wave pairing correlation...

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Main Author: Takashi Yanagisawa
Format: Article
Language:English
Published: IOP Publishing 2013-01-01
Series:New Journal of Physics
Online Access:https://doi.org/10.1088/1367-2630/15/3/033012
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author Takashi Yanagisawa
author_facet Takashi Yanagisawa
author_sort Takashi Yanagisawa
collection DOAJ
description In this study we have computed the pair correlation functions in the two-dimensional Hubbard model using a quantum Monte Carlo method. We employ a new diagonalization algorithm in the quantum Monte Carlo method which is free from the negative sign problem. We show that the d-wave pairing correlation function is indeed enhanced slightly for the positive on-site Coulomb interaction U when doping away from the half-filling. When the system size becomes large, the pair correlation function P _d increases for U  > 0 compared to the non-interacting case, while P _d is suppressed for U  > 0 when the system size is small. The enhancement ratio P _d [ U ]/ P _d [ U  = 0] will give a criterion on the existence of superconductivity. The ratio P _d [ U ]/ P _d [ U  = 0] increases almost linearly ∝ L when the system size L  ×  L is increased. This increase is a good indication of the existence of a superconducting phase in the two-dimensional Hubbard model. There is, however, no enhancement of pair correlation functions in the half-filled case, which indicates the absence of superconductivity without hole doping.
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spelling doaj.art-249176697224404ba4599b50d8ea59912023-08-08T11:05:16ZengIOP PublishingNew Journal of Physics1367-26302013-01-0115303301210.1088/1367-2630/15/3/033012Enhanced pair correlation functions in the two-dimensional Hubbard modelTakashi Yanagisawa0Electronics and Photonics Research Institute , National Institute of Advanced Industrial Science and Technology (AIST), Central 2, 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568, JapanIn this study we have computed the pair correlation functions in the two-dimensional Hubbard model using a quantum Monte Carlo method. We employ a new diagonalization algorithm in the quantum Monte Carlo method which is free from the negative sign problem. We show that the d-wave pairing correlation function is indeed enhanced slightly for the positive on-site Coulomb interaction U when doping away from the half-filling. When the system size becomes large, the pair correlation function P _d increases for U  > 0 compared to the non-interacting case, while P _d is suppressed for U  > 0 when the system size is small. The enhancement ratio P _d [ U ]/ P _d [ U  = 0] will give a criterion on the existence of superconductivity. The ratio P _d [ U ]/ P _d [ U  = 0] increases almost linearly ∝ L when the system size L  ×  L is increased. This increase is a good indication of the existence of a superconducting phase in the two-dimensional Hubbard model. There is, however, no enhancement of pair correlation functions in the half-filled case, which indicates the absence of superconductivity without hole doping.https://doi.org/10.1088/1367-2630/15/3/033012
spellingShingle Takashi Yanagisawa
Enhanced pair correlation functions in the two-dimensional Hubbard model
New Journal of Physics
title Enhanced pair correlation functions in the two-dimensional Hubbard model
title_full Enhanced pair correlation functions in the two-dimensional Hubbard model
title_fullStr Enhanced pair correlation functions in the two-dimensional Hubbard model
title_full_unstemmed Enhanced pair correlation functions in the two-dimensional Hubbard model
title_short Enhanced pair correlation functions in the two-dimensional Hubbard model
title_sort enhanced pair correlation functions in the two dimensional hubbard model
url https://doi.org/10.1088/1367-2630/15/3/033012
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