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We focus on the Sierpinski triangle with Hausdorff dimension <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mn>1.58<\/mml:mn><\/mml:math> and consider several generations. In the tight-binding limit, we find compact localised states, which are also explained in terms of symmetry and linked to the formation of a ferrimagnetic phase at weak interaction. Simulations at half-filling revealed the persistence of this type of magnetic order for every value of interaction strength and a Mott transition for U\/t <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mo>&amp;#x223C;<\/mml:mo><\/mml:math> 4.5. In addition, we found a remarkable dependence on the Hausdorff dimension regarding <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mi>i<\/mml:mi><mml:mo stretchy=\"false\">)<\/mml:mo><\/mml:math> the number of compact localised states in different generations, <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mi>i<\/mml:mi><mml:mi>i<\/mml:mi><mml:mo stretchy=\"false\">)<\/mml:mo><\/mml:math> the scaling of the total many-body ground-state energy in the tight-binding limit, and <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\"><mml:mi>i<\/mml:mi><mml:mi>i<\/mml:mi><mml:mi>i<\/mml:mi><mml:mo stretchy=\"false\">)<\/mml:mo><\/mml:math> the density of the states at the corners of the lattice for specific values of electronic filling. Moreover, in the presence of an intrinsic spin-orbit coupling, the zero-energy compact localized states become entangled and give rise to inner and outer corner modes.<\/jats:p>","DOI":"10.22331\/q-2024-09-11-1469","type":"journal-article","created":{"date-parts":[[2024,9,11]],"date-time":"2024-09-11T14:10:15Z","timestamp":1726063815000},"page":"1469","update-policy":"https:\/\/doi.org\/10.22331\/q-crossmark-policy-page","source":"Crossref","is-referenced-by-count":4,"title":["The Fractal-Lattice Hubbard Model"],"prefix":"10.22331","volume":"8","author":[{"ORCID":"https:\/\/orcid.org\/0009-0000-2632-6306","authenticated-orcid":false,"given":"Monica","family":"Conte","sequence":"first","affiliation":[{"name":"Institute for Theoretical Physics, Utrecht University, Princetonplein 5, 3584CC Utrecht, The Netherlands,"}]},{"ORCID":"https:\/\/orcid.org\/0000-0001-8236-9052","authenticated-orcid":false,"given":"Vinicius","family":"Zampronio","sequence":"additional","affiliation":[{"name":"Departamento de F\u00edsica Te\u00f3rica e Experimental - UFRN, Av. Sen. Salgado Filho 3000, 59078-970, Natal - RN, Brazil,"},{"name":"Institute for Theoretical Physics, Utrecht University, Princetonplein 5, 3584CC Utrecht, The Netherlands,"}]},{"ORCID":"https:\/\/orcid.org\/0000-0001-7784-8104","authenticated-orcid":false,"given":"Malte","family":"R\u00f6ntgen","sequence":"additional","affiliation":[{"name":"Laboratoire d\u2019Acoustique de l\u2019Universit\u00e9 du Mans, Unite Mixte de Recherche 6613, Centre National de la Recherche Scientifique, Avenue O. Messiaen, F-72085 Le Mans Cedex 9, France"}]},{"ORCID":"https:\/\/orcid.org\/0000-0002-4190-3893","authenticated-orcid":false,"given":"Cristiane Morais","family":"Smith","sequence":"additional","affiliation":[{"name":"Institute for Theoretical Physics, Utrecht University, Princetonplein 5, 3584CC Utrecht, The Netherlands,"}]}],"member":"9598","published-online":{"date-parts":[[2024,9,11]]},"reference":[{"key":"0","doi-asserted-by":"publisher","unstructured":"Daniel P. Arovas, Erez Berg, Steven A. 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