IFLP   13074
INSTITUTO DE FISICA LA PLATA
Unidad Ejecutora - UE
artículos
Título:
Paramagnetism and clustering in Fe-doped TiO2 nanoparticles
Autor/es:
C. RODRÍGUEZ TORRES; S. J. STEWART; C. ADAN; A. F. CABRERA
Revista:
JOURNAL OF ALLOYS AND COMPOUNDS
Editorial:
ELSEVIER SCIENCE SA
Referencias:
Año: 2010 vol. 495 p. 485 - 487
ISSN:
0925-8388
Resumen:
The magnetic behavior of Fe-doped TiO2 anatase nanoparticles (2.8 and 5.4 at.%) was investigated throughout magnetizations versus applied field measurements between 2 and 300K temperatures. The experimental results were well-fitted by using the Brillouin function, giving rise to a moment per isolated Fe atom of about 5B. The thermal evolution of the number of magnetic ions shows that a decrease of ions in paramagnetic state occurs below 50K for the most diluted sample. However for the 5.4 at.% sample the fall even at room temperature is evident. These moments probably order antiferromagnetically via superexchange interactions. Taking into account the low concentration of dopant and the high fraction of interacting ions, a correlated substitution of Fe in cation sites of TiO2 structure needs to be considered ions in paramagnetic state occurs below 50K for the most diluted sample. However for the 5.4 at.% sample the fall even at room temperature is evident. These moments probably order antiferromagnetically via superexchange interactions. Taking into account the low concentration of dopant and the high fraction of interacting ions, a correlated substitution of Fe in cation sites of TiO2 structure needs to be considered throughout magnetizations versus applied field measurements between 2 and 300K temperatures. The experimental results were well-fitted by using the Brillouin function, giving rise to a moment per isolated Fe atom of about 5B. The thermal evolution of the number of magnetic ions shows that a decrease of ions in paramagnetic state occurs below 50K for the most diluted sample. However for the 5.4 at.% sample the fall even at room temperature is evident. These moments probably order antiferromagnetically via superexchange interactions. Taking into account the low concentration of dopant and the high fraction of interacting ions, a correlated substitution of Fe in cation sites of TiO2 structure needs to be considered ions in paramagnetic state occurs below 50K for the most diluted sample. However for the 5.4 at.% sample the fall even at room temperature is evident. These moments probably order antiferromagnetically via superexchange interactions. Taking into account the low concentration of dopant and the high fraction of interacting ions, a correlated substitution of Fe in cation sites of TiO2 structure needs to be considered 2 anatase nanoparticles (2.8 and 5.4 at.%) was investigated throughout magnetizations versus applied field measurements between 2 and 300K temperatures. The experimental results were well-fitted by using the Brillouin function, giving rise to a moment per isolated Fe atom of about 5B. The thermal evolution of the number of magnetic ions shows that a decrease of ions in paramagnetic state occurs below 50K for the most diluted sample. However for the 5.4 at.% sample the fall even at room temperature is evident. These moments probably order antiferromagnetically via superexchange interactions. Taking into account the low concentration of dopant and the high fraction of interacting ions, a correlated substitution of Fe in cation sites of TiO2 structure needs to be considered ions in paramagnetic state occurs below 50K for the most diluted sample. However for the 5.4 at.% sample the fall even at room temperature is evident. These moments probably order antiferromagnetically via superexchange interactions. Taking into account the low concentration of dopant and the high fraction of interacting ions, a correlated substitution of Fe in cation sites of TiO2 structure needs to be considered B. The thermal evolution of the number of magnetic ions shows that a decrease of ions in paramagnetic state occurs below 50K for the most diluted sample. However for the 5.4 at.% sample the fall even at room temperature is evident. These moments probably order antiferromagnetically via superexchange interactions. Taking into account the low concentration of dopant and the high fraction of interacting ions, a correlated substitution of Fe in cation sites of TiO2 structure needs to be considered2 structure needs to be considered