F. H. Sánchez
National University of La Plata
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Featured researches published by F. H. Sánchez.
Physical Review B | 2005
S. Duhalde; M. F. Vignolo; F. Golmar; C. Chiliotte; C.E. Rodríguez Torres; L. A. Errico; A.F. Cabrera; M. Rentería; F. H. Sánchez; M. Weissmann
In recent years there has been an intense search for room temperature ferromagnetism in doped dilute semiconductors, which have many potentially applications in spintronics and optoelectronics. We report here the unexpected observation of significant room temperature ferromagnetism in a semiconductor doped with nonmagnetic impurities, Cu-doped TiO
Langmuir | 2016
D. F. Coral; Pedro Mendoza Zélis; Marzia Marciello; Maria del Puerto Morales; Aldo Craievich; F. H. Sánchez; Marcela B. Fernández van Raap
_2
Journal of Applied Physics | 2015
I. J. Bruvera; P. Mendoza Zélis; M. Pilar Calatayud; Gerardo F. Goya; F. H. Sánchez
thin films grown by Pulsed Laser Deposition. The magnetic moment, calculated from the magnetization curves, resulted surprisingly large, about 1.5
Journal of Physics D | 2013
P. Mendoza Zélis; G. A. Pasquevich; S J Stewart; M. B. Fernández van Raap; J. C. Aphesteguy; I. J. Bruvera; C Laborde; B Pianciola; Silvia E. Jacobo; F. H. Sánchez
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Journal of Applied Physics | 1987
Y. D. Zhang; J. I. Budnick; J. C. Ford; W. A. Hines; F. H. Sánchez; Ryusuke Hasegawa
per Cu atom. A large magnetic moment was also obtained from ab initio calculations using the supercell method for TiO
Applied Physics Letters | 2008
F. Golmar; A.M. Mudarra Navarro; C.E. Rodríguez Torres; F. H. Sánchez; F. D. Saccone; P. C. dos Santos Claro; Guillermo Benítez; Patricia L. Schilardi
_2
IEEE Transactions on Magnetics | 1987
J. I. Budnick; F. H. Sánchez; Y. Zhang; M. Choi; W. Hines; Z. Zhang; Shihui Ge; Ryusuke Hasegawa
with Cu impurities, but only if an oxygen vacancy in the nearest-neighbour shell of Cu was present. This result suggests that the role of oxygen vacancies is crucial for the appearance of ferromagnetism. The calculations also predict that Cu doping favours the formation of oxygen vacancies.
MRS Proceedings | 1985
F. H. Sánchez; F. Namavar; J. I. Budnick; A. Fasihudin; H. C. Hayden
Biomedical magnetic colloids commonly used in magnetic hyperthermia experiments often display a bidisperse structure, i.e., are composed of stable nanoclusters coexisting with well-dispersed nanoparticles. However, the influence of nanoclusters in the optimization of colloids for heat dissipation is usually excluded. In this work, bidisperse colloids are used to analyze the effect of nanoclustering and long-range magnetic dipolar interaction on the magnetic hyperthermia efficiency. Two kinds of colloids, composed of magnetite cores with mean sizes of around 10 and 18 nm, coated with oleic acid and dispersed in hexane, and coated with meso-2,3-dimercaptosuccinic acid and dispersed in water, were analyzed. Small-angle X-ray scattering was applied to thoroughly characterize nanoparticle structuring. We proved that the magnetic hyperthermia performances of nanoclusters and single nanoparticles are distinctive. Nanoclustering acts to reduce the specific heating efficiency whereas a peak against concentration appears for the well-dispersed component. Our experiments show that the heating efficiency of a magnetic colloid can increase or decrease when dipolar interactions increase and that the colloid concentration, i.e., dipolar interaction, can be used to improve magnetic hyperthermia. We have proven that the power dissipated by an ensemble of dispersed magnetic nanoparticles becomes a nonextensive property as a direct consequence of the long-range nature of dipolar interactions. This knowledge is a key point in selecting the correct dose that has to be injected to achieve the desired outcome in intracellular magnetic hyperthermia therapy.
Physics Letters A | 1981
A. F. Pasquevich; A. G. Bibiloni; Massolo Cp; F. H. Sánchez; A. López-García
In a magnetization vs. temperature (M vs. T) experiment, the blocking region of a magnetic nanoparticle (MNP) assembly is the interval of T values were the system begins to respond to an applied magnetic field H when heating the sample from the lower reachable temperature. The location of this region is determined by the anisotropy energy barrier depending on the applied field H, the volume V, the magnetic anisotropy constant K of the MNPs and the observing time of the technique. In the general case of a polysized sample, a representative blocking temperature value
Journal of Magnetism and Magnetic Materials | 1986
Y. D. Zhang; W. A. Hines; J. I. Budnick; M. Chao; F. H. Sánchez; Ryusuke Hasegawa
T_B