Análisis ferromagnético de la configuración bosónica-fermiónica de espines (S_i^A = 3, S_j^B = 5/2)
En el presente trabajo se investiga el comportamiento térmico y magnético de un sistema ferromagnético bosónico-fermiónico de espines S_i^A = 3 y S_j^B = 5/2, alternados en una red cuadrada bipartita, mediante un modelo de Ising mixto, usando simulaciones Monte Carlo y condiciones de borde periódica...
- Autores:
-
Hernández Herazo, Richard Manuel
- Tipo de recurso:
- Trabajo de grado de pregrado
- Fecha de publicación:
- 2025
- Institución:
- Universidad de Córdoba
- Repositorio:
- Repositorio Institucional Unicórdoba
- Idioma:
- spa
- OAI Identifier:
- oai:repositorio.unicordoba.edu.co:ucordoba/9276
- Acceso en línea:
- https://repositorio.unicordoba.edu.co/handle/ucordoba/9276
https://repositorio.unicordoba.edu.co/
- Palabra clave:
- Ferromagneto
Modelo de Ising mixto
Transición discontinua
Superparamagnetismo
Ferromagnet
Mixed Ising model
Discontinuous transition
Superparamagnetism
- Rights
- openAccess
- License
- Copyright Universidad de Córdoba, 2025
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Análisis ferromagnético de la configuración bosónica-fermiónica de espines (S_i^A = 3, S_j^B = 5/2) |
| title |
Análisis ferromagnético de la configuración bosónica-fermiónica de espines (S_i^A = 3, S_j^B = 5/2) |
| spellingShingle |
Análisis ferromagnético de la configuración bosónica-fermiónica de espines (S_i^A = 3, S_j^B = 5/2) Ferromagneto Modelo de Ising mixto Transición discontinua Superparamagnetismo Ferromagnet Mixed Ising model Discontinuous transition Superparamagnetism |
| title_short |
Análisis ferromagnético de la configuración bosónica-fermiónica de espines (S_i^A = 3, S_j^B = 5/2) |
| title_full |
Análisis ferromagnético de la configuración bosónica-fermiónica de espines (S_i^A = 3, S_j^B = 5/2) |
| title_fullStr |
Análisis ferromagnético de la configuración bosónica-fermiónica de espines (S_i^A = 3, S_j^B = 5/2) |
| title_full_unstemmed |
Análisis ferromagnético de la configuración bosónica-fermiónica de espines (S_i^A = 3, S_j^B = 5/2) |
| title_sort |
Análisis ferromagnético de la configuración bosónica-fermiónica de espines (S_i^A = 3, S_j^B = 5/2) |
| dc.creator.fl_str_mv |
Hernández Herazo, Richard Manuel |
| dc.contributor.advisor.none.fl_str_mv |
Espriella Vélez, Nicolas Antonio de la Madera Yances, Julio Cesar |
| dc.contributor.author.none.fl_str_mv |
Hernández Herazo, Richard Manuel |
| dc.contributor.jury.none.fl_str_mv |
TORRES HOYOS, FRANCISCO JOSE Ortega Lopez, César |
| dc.subject.proposal.spa.fl_str_mv |
Ferromagneto Modelo de Ising mixto Transición discontinua Superparamagnetismo |
| topic |
Ferromagneto Modelo de Ising mixto Transición discontinua Superparamagnetismo Ferromagnet Mixed Ising model Discontinuous transition Superparamagnetism |
| dc.subject.keywords.eng.fl_str_mv |
Ferromagnet Mixed Ising model Discontinuous transition Superparamagnetism |
| description |
En el presente trabajo se investiga el comportamiento térmico y magnético de un sistema ferromagnético bosónico-fermiónico de espines S_i^A = 3 y S_j^B = 5/2, alternados en una red cuadrada bipartita, mediante un modelo de Ising mixto, usando simulaciones Monte Carlo y condiciones de borde periódicas. El Hamiltoniano del sistema contiene interacciones de intercambio a primeros y segundos vecinos, campos cristalinos y un campo magnético longitudinal. Se calculan las magnetizaciones totales y de las subredes, la energía y la susceptibilidad magnética en función de la temperatura, para diferentes valores de las anisotropías (D_A, D_B), y el campo magnético externo (h). Los resultados muestran que el ferromagneto experimenta transiciones de fase continuas y discontinuas, en los intervalos -5 ≤ D_A < 4 y campo h < 0. Las transiciones discontinuas se destruyen cuando el sistema es sometido a campos positivos. En el análisis del comportamiento histérico del sistema en función de las anisotropías y acoplamientos de intercambio, se hallaron lazos simétricos y rectangulares, así como también fenómenos superparamagnéticos. |
| publishDate |
2025 |
| dc.date.accessioned.none.fl_str_mv |
2025-07-05T19:43:57Z |
| dc.date.available.none.fl_str_mv |
2025-07-05T19:43:57Z |
| dc.date.issued.none.fl_str_mv |
2025-07-03 |
| dc.type.none.fl_str_mv |
Trabajo de grado - Pregrado |
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info:eu-repo/semantics/bachelorThesis |
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http://purl.org/coar/resource_type/c_7a1f |
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info:eu-repo/semantics/acceptedVersion |
| dc.type.content.none.fl_str_mv |
Text |
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http://purl.org/coar/resource_type/c_7a1f |
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acceptedVersion |
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https://repositorio.unicordoba.edu.co/handle/ucordoba/9276 |
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Universidad de Córdoba |
| dc.identifier.reponame.none.fl_str_mv |
Repositorio Universidad de Córdoba |
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https://repositorio.unicordoba.edu.co/ |
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https://repositorio.unicordoba.edu.co/handle/ucordoba/9276 https://repositorio.unicordoba.edu.co/ |
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Universidad de Córdoba Repositorio Universidad de Córdoba |
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spa |
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spa |
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K. H. Buschow y F. R. de Boer. Physics of Magnetism and Magnetic Materials. Springer, 2003, pág. 19. M. Karimou y N. De La Espriella. “Critical phenomena in a two-dimensional ferrimagnetic system: Monte Carlo and Mean-Field Analysis”. En: Physica A: Statistical Mechanics and its Applications 531 (2019), pág. 121738. ISSN: 0378-4371. DOI: https://doi.org/10.1016/j.physa.2019.121738. Andrea Grimaldi et al. “Evaluating Spintronics-Compatible Implementations of Ising Machines”. En: Physical Review Applied 20 (2 ago. de 2023), pág. 024005. DOI: 10.1103/PhysRevApplied.20.024005. S. M. Yakout. “Spintronics: Future Technology for New Data Storage and Communication Devices”. En: Journal of Superconductivity and Novel Magnetism 33 (2020), págs. 2557–2580. DOI: 10.1007/s10948-020-05545-8. Abeer Mera, Q. Mahmood y Syed Awais Rouf. “Quantum ferromagnetism in transition metals doped II-VI semiconductors for spintronic applications: A merging technology”. En: Solid State Communications 352 (2022), pág. 114835. ISSN: 0038-1098. DOI: https://doi.org/10.1016/j.ssc.2022.114835. B. Deviren y M. Keskin. “Dynamic Phase Transitions and Compensation Temperatures in a Mixed Spin-3/2 and Spin-5/2 Ising System”. En: Journal of Statistical Physics 140 (2010), págs. 934–947. DOI: 10.1007/s10955-010-0025-6. Erhan Albayrak y A. Yigit. “The phase diagrams of the mixed spin-3/2 and spin-5/2 Ising system on the Bethe lattice”. En: physica status solidi (b) 244 (2007). Igor F. Lyuksyutov, Thomas Nattermann y Valery Pokrovsky. “Theory of the hysteresis loop in ferromagnets”. En: Physical Review B 59 (6 feb. de 1999), págs. 4260–4272. DOI: 10.1103/PhysRevB.59.4260. Mustafa Keskin y Mehmet Ertaş. “Dynamic magnetic hysteresis loop behaviors of a mixed spin (2, 5/2) Ising model on two interpenetrating square lattices”. En: Physica Scripta 95.5 (mar. de 2020), pág. 055805. DOI: 10.1088/1402-4896/ab783f. S. L. Driver et al. “Multiferroic (ferroelastic/ferromagnetic/ferrimagnetic) aspects of phase transitions in RCo2 Laves phases”. En: Journal of Physics: Condensed Matter 26.5 (ene. de 2014), pág. 056001. DOI: 10.1088/0953-8984/26/5/056001. R. Houenou et al. “The critical behaviors of a ferromagnetic–ferrimagnetic Ising ternary alloy with mixed spin-(1/2, 3/2, 5/2)”. En: The European Physical Journal Plus 136 (2021). D. Fouejio, P. Noudem y S. S. Zekeng. “Magnetic and thermodynamic properties of mixed spin-3/2 and spin-3 Ising ferrimagnets on a 2D triangular lattice: Monte Carlo study”. En: Chinese Journal of Physics (2024). Bo-chen Li y Wei Wang. “Exploration of dynamic phase transition of 3D Ising model with a new long-range interaction by using the Monte Carlo method”. En: Chinese Journal of Physics 90 (2024), págs. 15–30. ISSN: 0577-9073. DOI: https://doi.org/10.1016/j.cjph.2024.05.021. Zhaoxu Chen et al. “High-Tc Ferromagnetic Semiconductor in Thinned 3D Ising Ferromagnetic Metal Fe₃GaTe₂”. En: Nano Letters 24.3 (2024), págs. 993–1000. PMID: 38190333. DOI: 10.1021/acs.nanolett.3c04462. Yu Liu et al. “Three-dimensional Ising ferrimagnetism of Cr–Fe–Cr trimers in Fe Cr 2 Te 4”. En: Physical Review B 102 (ago. de 2020). DOI: 10.1103/PhysRevB.102.085158. Hadey K. Mohamad. “Spin compensation temperatures induced by longitudinal fields in a mixed spin-3/2 and spin-5/2 Ising ferrimagnet”. En: Journal of Magnetism and Magnetic Materials 323.1 (2011), págs. 61–66. ISSN: 0304-8853. DOI: https://doi.org/10.1016/j.jmmm.2010.08.030. Juan Adrian Reyes, N. De La Espriella y Gloria M. Buendía. “Effects of an external magnetic field on a mixed spin-3/2 and spin-5/2 Ising ferrimagnet: A Monte Carlo study”. En: physica status solidi (b) 252 (2015). “Critical and compensation behavior of a mixed spin-3/2 and spin-5/2 Ising ferrimagnetic system in a graphene layer”. En: Journal of Magnetism and Magnetic Materials 429 (2017), págs. 34–39. ISSN: 0304-8853. DOI: https://doi.org/10.1016/j.jmmm.2017.01.004. Nicolás De La Espriella, Mounirou Karimou y Gloria M. Buendía. “Mixed Spin (3/2, 7/2) Ising-Type Ferrimagnet: Monte Carlo–Mean Field Treatment”. En: physica status solidi (b) 258.4 (), pág. 2000536. DOI: https://doi.org/10.1002/pssb.202000536. K. H. Jürgen Buschow, Piet van Engen y R. Jongebreur. “Magneto-optical properties of metallic ferromagnetic materials”. En: Journal of Magnetism and Magnetic Materials 38 (1983), págs. 1–22. “Magnetic properties of mixed integer and half-integer spins in a Blume–Capel model: A Monte Carlo study”. En: Journal of Magnetism and Magnetic Materials 421 (2017), págs. 76–81. ISSN: 0304-8853. DOI: https://doi.org/10.1016/j.jmmm.2016.07.069. M. Bessimou y Rachid Masrour. “Magnetocaloric effect and magnetic properties of Dy2CoMnO6: Monte Carlo study”. En: Philosophical Magazine 103 (2022), págs. 56–66. “Mixed spin-3/2 and spin-2 Ising model on diamond-like decorated square: A Monte Carlo simulation”. En: Physica A: Statistical Mechanics and its Applications 539 (2020), pág. 122878. ISSN: 0378-4371. DOI: https://doi.org/10.1016/j.physa.2019.122878. “Compensation behavior for a mixed spin-3 and spin-7/2 Blume–Capel system with crystal field interaction”. En: Chinese Journal of Physics 88 (2024), págs. 879–887. ISSN: 0577-9073. DOI: https://doi.org/10.1016/j.cjph.2024.02.023. “Magnetic characteristics of a mixed spin-3 and spin-7/2 Blume–Capel system for square and simple cubic lattices”. En: Solid State Communications 338 (2021), pág. 114456. ISSN: 0038-1098. DOI: https://doi.org/10.1016/j.ssc.2021.114456. Nicola A. Spaldin. Magnetic Materials. 2a. Cambridge University Press, 2010. B. D. Cullity y C. D. Graham. Introduction to Magnetic Materials. 2a. John Wiley Sons, 2008. Y. Cao et al. “Overview and advances in a layered chiral helimagnet Cr1/3NbS2”. En: Materials Today Advances 7 (2020), pág. 100080. ISSN: 2590-0498. DOI: https://doi.org/10.1016/j.mtadv.2020.100080. Michael Shatruk y Judith K. Clark. “Magnetic materials”. En: Comprehensive Inorganic Chemistry III. Editado por Jan Reedijk y Kenneth R. Poeppelmeier. Vol. 4.08. Elsevier, 2023, págs. 236–261. ISBN: 9780128231531. Abdel-Mohsen Onsy Mohamed y Evan K. Paleologos. “Chapter 15 – Magnetic Properties of Soils”. En: Fundamentals of Geoenvironmental Engineering. Editado por Abdel-Mohsen Onsy Mohamed y Evan K. Paleologos. Butterworth-Heinemann, 2018, págs. 535–580. ISBN: 978-0-12-804830-6. DOI: https://doi.org/10.1016/B978-0-12-804830-6.00015-6. Alessia Berti, Claudio Giorgi y Elena Vuk. “Hysteresis and temperature-induced transitions in ferromagnetic materials”. En: Applied Mathematical Modelling 39.2 (2015), págs. 820–837. ISSN: 0307-904X. DOI: https://doi.org/10.1016/j.apm.2014.07.004. Matthias B. Jungfleisch, Wei Zhang y Axel Hoffmann. “Perspectives of antiferromagnetic spintronics”. En: Physics Letters A 382.13 (2018), págs. 865–871. ISSN: 0375-9601. DOI: https://doi.org/10.1016/j.physleta.2018.01.008. R. K. Kotnala y Jyoti Shah. “Chapter 4 – Ferrite Materials: Nano to Spintronics Regime”. En: editado por K. H. J. Buschow. Vol. 23. Handbook of Magnetic Materials. Elsevier, 2015, págs. 291–379. DOI: https://doi.org/10.1016/B978-0-444-63528-0.00004-8. Elena Bartolomé et al. “Chapter 1 – Magnetic Relaxation of Lanthanide-Based Molecular Magnets”. En: editado por Ekkes Brück. Vol. 26. Handbook of Magnetic Materials. Elsevier, 2017, págs. 1–289. DOI: https://doi.org/10.1016/bs.hmm.2017.09.002. Gayanath W. Fernando. “Chapter 4 – Magnetic Anisotropy in Transition Metal Systems”. En: Metallic Multilayers and their Applications. Editado por Gayanath W. Fernando. Vol. 4. Handbook of Metal Physics. Elsevier, 2008, págs. 89–110. DOI: https://doi.org/10.1016/S1570-002X(07)00004-3. Ananya Renuka Balakrishna. “Rethinking hysteresis in magnetic materials”. En: MRS communications 14.5 (ago. de 2024). doi: 10.1557/s43579-024-00624-6. Angélica L. Gelover-Santiago. Simulación del modelo de Ising con el m´etodo de Monte Carlo. 2a. Coordinaci´ on de Servicios Editoriales UNAM, 1990. D. P. Landau y K. Binder. A Guide to Monte Carlo Simulations in Statistical Physics. 4a. Cambridge University Press, 2014. T. Ostler et al. “Ultrafast heating as a sufficient stimulus for magnetization reversal in a ferrimagnet”. En: Nature Communications 3 (2012), pág. 666. DOI: 10.1038/ncomms1666. URL: https://doi.org/10.1038/ncomms1666. |
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Copyright Universidad de Córdoba, 2025 |
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Atribución-NoComercial-SinDerivadas 4.0 Internacional (CC BY-NC-ND 4.0) |
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Copyright Universidad de Córdoba, 2025 https://creativecommons.org/licenses/by-nc-nd/4.0/ Atribución-NoComercial-SinDerivadas 4.0 Internacional (CC BY-NC-ND 4.0) http://purl.org/coar/access_right/c_abf2 |
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Universidad de Córdoba |
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Facultad de Ciencias Básicas |
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Montería, Córdoba, Colombia |
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Física |
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Espriella Vélez, Nicolas Antonio de la421da0b3-24ed-44f7-b0ed-42afa0f7d569600Madera Yances, Julio Cesar6f24508e-f17a-4044-9abb-abfe7896b25e600Hernández Herazo, Richard Manuelb9aeff46-0f0f-499d-9390-b203e54bf138-1TORRES HOYOS, FRANCISCO JOSEe0889e8d-f195-4246-86cc-21f3b9158352600Ortega Lopez, César326e5843-fd0b-4bad-9439-246a9ce34a5a6002025-07-05T19:43:57Z2025-07-05T19:43:57Z2025-07-03https://repositorio.unicordoba.edu.co/handle/ucordoba/9276Universidad de CórdobaRepositorio Universidad de Córdobahttps://repositorio.unicordoba.edu.co/En el presente trabajo se investiga el comportamiento térmico y magnético de un sistema ferromagnético bosónico-fermiónico de espines S_i^A = 3 y S_j^B = 5/2, alternados en una red cuadrada bipartita, mediante un modelo de Ising mixto, usando simulaciones Monte Carlo y condiciones de borde periódicas. El Hamiltoniano del sistema contiene interacciones de intercambio a primeros y segundos vecinos, campos cristalinos y un campo magnético longitudinal. Se calculan las magnetizaciones totales y de las subredes, la energía y la susceptibilidad magnética en función de la temperatura, para diferentes valores de las anisotropías (D_A, D_B), y el campo magnético externo (h). Los resultados muestran que el ferromagneto experimenta transiciones de fase continuas y discontinuas, en los intervalos -5 ≤ D_A < 4 y campo h < 0. Las transiciones discontinuas se destruyen cuando el sistema es sometido a campos positivos. En el análisis del comportamiento histérico del sistema en función de las anisotropías y acoplamientos de intercambio, se hallaron lazos simétricos y rectangulares, así como también fenómenos superparamagnéticos.1 Introducción2 Marco teórico2.0.1 Magnetización e inducción magnética2.0.2 Susceptibilidad y permeabilidad2.0.3 Materiales magnéticos2.0.4 Tipos de materiales magnéticos2.0.5 Interacciones magnéticas2.0.6 Energía de intercambio2.0.7 Transiciones de fase2.0.8 Modelo Ising2.0.9 Método Monte Carlo3 Resultados y análisis3.1 Modelo y Hamiltoniano de interacción3.2 Variables termodinámicas del sistema3.3 Efecto anisotrópico sobre el ferromagneto3.3.1 Influencia sobre la magnetización3.3.2 Influencia sobre la susceptibilidad magnética (χ_T)3.3.3 Influencia sobre la energía (E)3.3.4 Efectos sobre la temperatura3.4 Comportamiento histérico del ferromagneto3.4.1 Modelo J_AB – J_SA – D; T = 53.4.2 Modelo J_AB – J_SA – J_SB – D; T = 53.4.3 Modelo J_AB – J_SA – D_A – D_B; T = 53.4.4 Modelo J_AB – J_SA – D_A – D_B; T = 103.4.5 Modelo J_AB – D_A – D_B; T = 104 ConclusionesPregradoFísico(a)Trabajos de Investigación y/o Extensiónapplication/pdfspaUniversidad de CórdobaFacultad de Ciencias BásicasMontería, Córdoba, ColombiaFísicaCopyright Universidad de Córdoba, 2025https://creativecommons.org/licenses/by-nc-nd/4.0/Atribución-NoComercial-SinDerivadas 4.0 Internacional (CC BY-NC-ND 4.0)info:eu-repo/semantics/openAccesshttp://purl.org/coar/access_right/c_abf2Análisis ferromagnético de la configuración bosónica-fermiónica de espines (S_i^A = 3, S_j^B = 5/2)Trabajo de grado - Pregradoinfo:eu-repo/semantics/bachelorThesishttp://purl.org/coar/resource_type/c_7a1finfo:eu-repo/semantics/acceptedVersionTextK. H. Buschow y F. R. de Boer. Physics of Magnetism and Magnetic Materials. Springer, 2003, pág. 19.M. Karimou y N. De La Espriella. “Critical phenomena in a two-dimensional ferrimagnetic system: Monte Carlo and Mean-Field Analysis”. En: Physica A: Statistical Mechanics and its Applications 531 (2019), pág. 121738. ISSN: 0378-4371. DOI: https://doi.org/10.1016/j.physa.2019.121738.Andrea Grimaldi et al. “Evaluating Spintronics-Compatible Implementations of Ising Machines”. En: Physical Review Applied 20 (2 ago. de 2023), pág. 024005. DOI: 10.1103/PhysRevApplied.20.024005.S. M. Yakout. “Spintronics: Future Technology for New Data Storage and Communication Devices”. En: Journal of Superconductivity and Novel Magnetism 33 (2020), págs. 2557–2580. DOI: 10.1007/s10948-020-05545-8.Abeer Mera, Q. Mahmood y Syed Awais Rouf. “Quantum ferromagnetism in transition metals doped II-VI semiconductors for spintronic applications: A merging technology”. En: Solid State Communications 352 (2022), pág. 114835. ISSN: 0038-1098. DOI: https://doi.org/10.1016/j.ssc.2022.114835.B. Deviren y M. Keskin. “Dynamic Phase Transitions and Compensation Temperatures in a Mixed Spin-3/2 and Spin-5/2 Ising System”. En: Journal of Statistical Physics 140 (2010), págs. 934–947. DOI: 10.1007/s10955-010-0025-6.Erhan Albayrak y A. Yigit. “The phase diagrams of the mixed spin-3/2 and spin-5/2 Ising system on the Bethe lattice”. En: physica status solidi (b) 244 (2007).Igor F. Lyuksyutov, Thomas Nattermann y Valery Pokrovsky. “Theory of the hysteresis loop in ferromagnets”. En: Physical Review B 59 (6 feb. de 1999), págs. 4260–4272. DOI: 10.1103/PhysRevB.59.4260.Mustafa Keskin y Mehmet Ertaş. “Dynamic magnetic hysteresis loop behaviors of a mixed spin (2, 5/2) Ising model on two interpenetrating square lattices”. En: Physica Scripta 95.5 (mar. de 2020), pág. 055805. DOI: 10.1088/1402-4896/ab783f.S. L. 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URL: https://doi.org/10.1038/ncomms1666.FerromagnetoModelo de Ising mixtoTransición discontinuaSuperparamagnetismoFerromagnetMixed Ising modelDiscontinuous transitionSuperparamagnetismPublicationORIGINALHernándezHerazoRichardManuel.pdfHernándezHerazoRichardManuel.pdfapplication/pdf2428391https://repositorio.unicordoba.edu.co/bitstreams/35da2a8b-2af3-4389-96c4-9e76aa4e2270/download7ee99d6e466b44965ace39c1e31c2ad4MD51Formato de autorización.pdfFormato de autorización.pdfapplication/pdf751045https://repositorio.unicordoba.edu.co/bitstreams/25c3df5f-7db7-4d2e-905c-2cb960a79d7f/download1e6392336518e1b8e3a05c9476a85897MD53LICENSElicense.txtlicense.txttext/plain; charset=utf-815543https://repositorio.unicordoba.edu.co/bitstreams/f23fccef-8c99-4949-a32b-186028036ff9/download73a5432e0b76442b22b026844140d683MD52TEXTHernándezHerazoRichardManuel.pdf.txtHernándezHerazoRichardManuel.pdf.txtExtracted 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Córdoba, 2025open.accesshttps://repositorio.unicordoba.edu.coRepositorio Universidad de 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