{"status":"ok","message-type":"work","message-version":"1.0.0","message":{"indexed":{"date-parts":[[2025,12,9]],"date-time":"2025-12-09T10:46:10Z","timestamp":1765277170174,"version":"3.46.0"},"reference-count":41,"publisher":"IOP Publishing","issue":"1","license":[{"start":{"date-parts":[[2025,12,9]],"date-time":"2025-12-09T00:00:00Z","timestamp":1765238400000},"content-version":"vor","delay-in-days":0,"URL":"https:\/\/creativecommons.org\/licenses\/by\/4.0\/"},{"start":{"date-parts":[[2025,12,9]],"date-time":"2025-12-09T00:00:00Z","timestamp":1765238400000},"content-version":"tdm","delay-in-days":0,"URL":"https:\/\/iopscience.iop.org\/info\/page\/text-and-data-mining"}],"content-domain":{"domain":["iopscience.iop.org"],"crossmark-restriction":false},"short-container-title":["2D Mater."],"published-print":{"date-parts":[[2026,3,1]]},"abstract":"<jats:title>Abstract<\/jats:title>\n                  <jats:p>\n                    Electron\u2013electron interactions in honeycomb lattices have attracted attention because of the intensive research on two-dimensional (2D) graphene. We investigated the finite-temperature electronic properties of honeycomb lattices using the single-band Hubbard model and the canonical partition function. The calculations were performed on a small cluster unit cell with\n                    <jats:italic>N<\/jats:italic>\n                    \u2009=\u20096 atoms. The half-filled band (one electron per) and hole-doped (one and two holes) honeycomb lattices were studied as a function of the intensity ratio between the on-site Coulomb repulsion (\n                    <jats:italic>U<\/jats:italic>\n                    ) and the nearest-neighbor electronic hopping (\n                    <jats:italic>t<\/jats:italic>\n                    ). The magnetization, magnetic susceptibility, spin\u2013spin correlation functions, spin-resolved specific heat, magneto-caloric effect (MCE), local magnetic moments, charge, and spin gaps were analyzed. In the half-filled band, the antiferromagnetic (AFM) insulator behavior developed as\n                    <jats:inline-formula>\n                      <jats:tex-math>\n                        \n                      <\/jats:tex-math>\n                      <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" overflow=\"scroll\">\n                        <mml:mrow>\n                          <mml:mi>U<\/mml:mi>\n                          <mml:mrow>\n                            <mml:mo>\/<\/mml:mo>\n                          <\/mml:mrow>\n                          <mml:mi>t<\/mml:mi>\n                        <\/mml:mrow>\n                      <\/mml:math>\n                    <\/jats:inline-formula>\n                    increased; the one-hole-doping case showed AFM order, presumably resonating valence bond states, and ferromagnetic (FM) insulator behavior as the\n                    <jats:inline-formula>\n                      <jats:tex-math>\n                        \n                      <\/jats:tex-math>\n                      <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" overflow=\"scroll\">\n                        <mml:mrow>\n                          <mml:mi>U<\/mml:mi>\n                          <mml:mrow>\n                            <mml:mo>\/<\/mml:mo>\n                          <\/mml:mrow>\n                          <mml:mi>t<\/mml:mi>\n                        <\/mml:mrow>\n                      <\/mml:math>\n                    <\/jats:inline-formula>\n                    strength increased. The entropy under external magnetic fields was calculated to determine the MCE. The magnetic field dependence of the total spin\n                    <jats:italic>S<\/jats:italic>\n                    was also analyzed. The honeycomb lattice with a half-filled band underwent a negative-positive MCE as the temperature increased. In contrast, the hole-doped systems exhibited a positive MCE, regardless of the\n                    <jats:inline-formula>\n                      <jats:tex-math>\n                        \n                      <\/jats:tex-math>\n                      <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" overflow=\"scroll\">\n                        <mml:mrow>\n                          <mml:mi>U<\/mml:mi>\n                          <mml:mrow>\n                            <mml:mo>\/<\/mml:mo>\n                          <\/mml:mrow>\n                          <mml:mi>t<\/mml:mi>\n                        <\/mml:mrow>\n                      <\/mml:math>\n                    <\/jats:inline-formula>\n                    strength. Our findings from a small cluster within the Hubbard model could help to further understand the electronic and magnetic properties of real 2D materials. However, it is important to note that the critical\n                    <jats:inline-formula>\n                      <jats:tex-math>\n                        \n                      <\/jats:tex-math>\n                      <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" overflow=\"scroll\">\n                        <mml:mrow>\n                          <mml:mi>U<\/mml:mi>\n                          <mml:mrow>\n                            <mml:mo>\/<\/mml:mo>\n                          <\/mml:mrow>\n                          <mml:mi>t<\/mml:mi>\n                        <\/mml:mrow>\n                      <\/mml:math>\n                    <\/jats:inline-formula>\n                    values for spin transitions and magnetic ordering could be size-dependent owing to the finite-size effects.\n                  <\/jats:p>","DOI":"10.1088\/2053-1583\/ae2594","type":"journal-article","created":{"date-parts":[[2025,11,28]],"date-time":"2025-11-28T22:48:17Z","timestamp":1764370097000},"page":"015016","update-policy":"https:\/\/doi.org\/10.1088\/crossmark-policy","source":"Crossref","is-referenced-by-count":0,"title":["Temperature and doping effects on the electronic and magnetic properties in two-dimensional graphene honeycomb lattices"],"prefix":"10.1088","volume":"13","author":[{"ORCID":"https:\/\/orcid.org\/0000-0003-4001-0038","authenticated-orcid":true,"given":"Florentino","family":"L\u00f3pez-Ur\u00edas","sequence":"first","affiliation":[],"role":[{"role":"author","vocabulary":"crossref"}]},{"ORCID":"https:\/\/orcid.org\/0000-0002-0855-3529","authenticated-orcid":false,"given":"Francisco","family":"S\u00e1nchez-Ochoa","sequence":"additional","affiliation":[],"role":[{"role":"author","vocabulary":"crossref"}]}],"member":"266","published-online":{"date-parts":[[2025,12,9]]},"reference":[{"key":"tdmae2594bib1","doi-asserted-by":"publisher","first-page":"109","DOI":"10.1103\/RevModPhys.81.109","type":"journal-article","article-title":"The electronic properties of graphene","volume":"81","author":"Castro Neto","year":"2009","journal-title":"Rev. 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Published by IOP Publishing Ltd","name":"copyright_information","label":"Copyright Information"},{"value":"2025-08-23","name":"date_received","label":"Date Received","group":{"name":"publication_dates","label":"Publication dates"}},{"value":"2025-11-28","name":"date_accepted","label":"Date Accepted","group":{"name":"publication_dates","label":"Publication dates"}},{"value":"2025-12-09","name":"date_epub","label":"Online publication date","group":{"name":"publication_dates","label":"Publication dates"}}]}}