Determination of the blocking temperature of magnetic nanoparticles : The good, the bad, and the ugly
- Autores
- Bruvera, Ignacio Javier; Mendoza Zélis, Pedro; Calatayud, M. Pilar; Goya, Gerardo Fabián; Sánchez, Francisco Homero
- Año de publicación
- 2015
- Idioma
- inglés
- Tipo de recurso
- artículo
- Estado
- versión publicada
- Descripción
- A numerically solved two-level Stoner-Wohlfarth model with thermal agitation is used to simulate Zero Field Cooling (ZFC)–Field Cooling (FC) curves of monosize and polysize samples and to determine the best method for obtaining a representative blocking temperature TB value of polysize samples. The results confirm a technique based on the T derivative of the difference between ZFC and FC curves proposed by Micha et al. (the good) and demonstrate its relation with two alternative methods: the ZFC maximum (the bad) and the inflection point (the ugly). The derivative method is then applied to experimental data, obtaining the TB distribution of a polysize Fe3O4 nanoparticle sample suspended in hexane with an excellent agreement with TEM characterization.
Instituto de Física La Plata - Materia
-
Ciencias Exactas
Física
Stoner-Wohlfarth model
Magnetic nanoparticles - Nivel de accesibilidad
- acceso abierto
- Condiciones de uso
- http://creativecommons.org/licenses/by/4.0/
- Repositorio
.jpg)
- Institución
- Universidad Nacional de La Plata
- OAI Identificador
- oai:sedici.unlp.edu.ar:10915/124066
Ver los metadatos del registro completo
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Determination of the blocking temperature of magnetic nanoparticles : The good, the bad, and the uglyBruvera, Ignacio JavierMendoza Zélis, PedroCalatayud, M. PilarGoya, Gerardo FabiánSánchez, Francisco HomeroCiencias ExactasFísicaStoner-Wohlfarth modelMagnetic nanoparticlesA numerically solved two-level Stoner-Wohlfarth model with thermal agitation is used to simulate Zero Field Cooling (ZFC)–Field Cooling (FC) curves of monosize and polysize samples and to determine the best method for obtaining a representative blocking temperature T<sub>B</sub> value of polysize samples. The results confirm a technique based on the T derivative of the difference between ZFC and FC curves proposed by Micha et al. (the good) and demonstrate its relation with two alternative methods: the ZFC maximum (the bad) and the inflection point (the ugly). The derivative method is then applied to experimental data, obtaining the T<sub>B</sub> distribution of a polysize Fe<sub>3</sub>O<sub>4</sub> nanoparticle sample suspended in hexane with an excellent agreement with TEM characterization.Instituto de Física La Plata2015-11-14info:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersionArticulohttp://purl.org/coar/resource_type/c_6501info:ar-repo/semantics/articuloapplication/pdfhttp://sedici.unlp.edu.ar/handle/10915/124066enginfo:eu-repo/semantics/altIdentifier/issn/0021-8979info:eu-repo/semantics/altIdentifier/issn/1089-7550info:eu-repo/semantics/altIdentifier/doi/10.1063/1.4935484info:eu-repo/semantics/openAccesshttp://creativecommons.org/licenses/by/4.0/Creative Commons Attribution 4.0 International (CC BY 4.0)reponame:SEDICI (UNLP)instname:Universidad Nacional de La Platainstacron:UNLP2025-11-12T10:53:48Zoai:sedici.unlp.edu.ar:10915/124066Institucionalhttp://sedici.unlp.edu.ar/Universidad públicaNo correspondehttp://sedici.unlp.edu.ar/oai/snrdalira@sedici.unlp.edu.arArgentinaNo correspondeNo correspondeNo correspondeopendoar:13292025-11-12 10:53:48.511SEDICI (UNLP) - Universidad Nacional de La Platafalse |
| dc.title.none.fl_str_mv |
Determination of the blocking temperature of magnetic nanoparticles : The good, the bad, and the ugly |
| title |
Determination of the blocking temperature of magnetic nanoparticles : The good, the bad, and the ugly |
| spellingShingle |
Determination of the blocking temperature of magnetic nanoparticles : The good, the bad, and the ugly Bruvera, Ignacio Javier Ciencias Exactas Física Stoner-Wohlfarth model Magnetic nanoparticles |
| title_short |
Determination of the blocking temperature of magnetic nanoparticles : The good, the bad, and the ugly |
| title_full |
Determination of the blocking temperature of magnetic nanoparticles : The good, the bad, and the ugly |
| title_fullStr |
Determination of the blocking temperature of magnetic nanoparticles : The good, the bad, and the ugly |
| title_full_unstemmed |
Determination of the blocking temperature of magnetic nanoparticles : The good, the bad, and the ugly |
| title_sort |
Determination of the blocking temperature of magnetic nanoparticles : The good, the bad, and the ugly |
| dc.creator.none.fl_str_mv |
Bruvera, Ignacio Javier Mendoza Zélis, Pedro Calatayud, M. Pilar Goya, Gerardo Fabián Sánchez, Francisco Homero |
| author |
Bruvera, Ignacio Javier |
| author_facet |
Bruvera, Ignacio Javier Mendoza Zélis, Pedro Calatayud, M. Pilar Goya, Gerardo Fabián Sánchez, Francisco Homero |
| author_role |
author |
| author2 |
Mendoza Zélis, Pedro Calatayud, M. Pilar Goya, Gerardo Fabián Sánchez, Francisco Homero |
| author2_role |
author author author author |
| dc.subject.none.fl_str_mv |
Ciencias Exactas Física Stoner-Wohlfarth model Magnetic nanoparticles |
| topic |
Ciencias Exactas Física Stoner-Wohlfarth model Magnetic nanoparticles |
| dc.description.none.fl_txt_mv |
A numerically solved two-level Stoner-Wohlfarth model with thermal agitation is used to simulate Zero Field Cooling (ZFC)–Field Cooling (FC) curves of monosize and polysize samples and to determine the best method for obtaining a representative blocking temperature T<sub>B</sub> value of polysize samples. The results confirm a technique based on the T derivative of the difference between ZFC and FC curves proposed by Micha et al. (the good) and demonstrate its relation with two alternative methods: the ZFC maximum (the bad) and the inflection point (the ugly). The derivative method is then applied to experimental data, obtaining the T<sub>B</sub> distribution of a polysize Fe<sub>3</sub>O<sub>4</sub> nanoparticle sample suspended in hexane with an excellent agreement with TEM characterization. Instituto de Física La Plata |
| description |
A numerically solved two-level Stoner-Wohlfarth model with thermal agitation is used to simulate Zero Field Cooling (ZFC)–Field Cooling (FC) curves of monosize and polysize samples and to determine the best method for obtaining a representative blocking temperature T<sub>B</sub> value of polysize samples. The results confirm a technique based on the T derivative of the difference between ZFC and FC curves proposed by Micha et al. (the good) and demonstrate its relation with two alternative methods: the ZFC maximum (the bad) and the inflection point (the ugly). The derivative method is then applied to experimental data, obtaining the T<sub>B</sub> distribution of a polysize Fe<sub>3</sub>O<sub>4</sub> nanoparticle sample suspended in hexane with an excellent agreement with TEM characterization. |
| publishDate |
2015 |
| dc.date.none.fl_str_mv |
2015-11-14 |
| dc.type.none.fl_str_mv |
info:eu-repo/semantics/article info:eu-repo/semantics/publishedVersion Articulo http://purl.org/coar/resource_type/c_6501 info:ar-repo/semantics/articulo |
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article |
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publishedVersion |
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http://sedici.unlp.edu.ar/handle/10915/124066 |
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| dc.language.none.fl_str_mv |
eng |
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eng |
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info:eu-repo/semantics/altIdentifier/issn/0021-8979 info:eu-repo/semantics/altIdentifier/issn/1089-7550 info:eu-repo/semantics/altIdentifier/doi/10.1063/1.4935484 |
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