scispace - formally typeset
Search or ask a question
Author

José Luis García-Muñoz

Bio: José Luis García-Muñoz is an academic researcher from Institute of Cost and Management Accountants of Bangladesh. The author has contributed to research in topics: Neutron diffraction & Magnetization. The author has an hindex of 37, co-authored 195 publications receiving 5410 citations. Previous affiliations of José Luis García-Muñoz include European Synchrotron Radiation Facility & Autonomous University of Barcelona.


Papers
More filters
Journal ArticleDOI
TL;DR: The amplitude $\ensuremath{\rho}(T,H)$ and temperature ${T}_{M}$ and CMR are found to be controlled by the radius of the lanthanide $({L}^{3+})$ which modifies the bending of the Mn-O-Mn bond.
Abstract: The amplitude $\ensuremath{\Delta}\ensuremath{\rho}(T,H)/\ensuremath{\rho}$ and temperature ${T}_{M}$, where the colossal magnetoresistance (CMR) response of ${L}_{1\ensuremath{-}x}{\mathrm{Ca}}_{x}{\mathrm{MnO}}_{3}$ manganites are maximum, are found to be controlled by the radius of the lanthanide $({L}^{3+})$ which modifies the bending of the Mn-O-Mn bond. Increasing the bond distortion lowers ${T}_{M}$ and enhances $\ensuremath{\Delta}\ensuremath{\rho}(T,H)/\ensuremath{\rho}$. Enhanced CMR arises from (1) a shift to lower temperatures of ${T}_{M}$, (2) a reduced mobility of the doping holes, and (3) an increase of the coupling between itinerant and localized electrons. The resistivity $\ensuremath{\rho}\left(H\right)$ follows an $\ensuremath{\approx}{\mathrm{BM}}^{2}\left(H\right)$ law and the parameter $B$ is also tuned by the Mn-O-Mn bond angle. The narrowing of the electronic bandwidth is the fundamental parameter controlling the observed CMR.

423 citations

Journal ArticleDOI
TL;DR: High-resolution neutron-powder-diffraction experiments have been performed to investigate the structural anomalies across the first-order M-I transition in the orthorhombic PrNiO 3 and Nd NiO 3 compounds.
Abstract: In the R${\mathrm{NiO}}_{3}$ series (R=La,Pr,Nd,Sm), the metal-insulator (M-I) transition temperature rises systematically as the size of the rare earth decreases and as the subsequent distortion from the ideal cubic perovskite increases. For R=La the system keeps its metallic character down to 1.5 K, while for R=Pr, Nd, and Sm electronic localization occurs at 135, 200, and 400 K, respectively. High-resolution neutron-powder-diffraction experiments have been performed to investigate the structural anomalies across the first-order M-I transition in the orthorhombic ${\mathrm{PrNiO}}_{3}$ and ${\mathrm{NdNiO}}_{3}$ compounds. The cell volume undergoes a subtle increase when the compounds become insulating, due to a slight increase of the Ni-O distances. This effect is accompanied by coupled tilts of ${\mathrm{NiO}}_{6}$ octahedra, which imply changes in the Ni-O-Ni angles (\ensuremath{\Delta}${\mathrm{\ensuremath{\Theta}}}_{\mathrm{O}\mathrm{\ensuremath{-}}\mathrm{Ni}\mathrm{\ensuremath{-}}\mathrm{O}}$\ensuremath{\approxeq}-0.5\ifmmode^\circ\else\textdegree\fi{}) governing the transfer integral between Ni ${\mathit{e}}_{\mathit{g}}$ and O 2p orbitals. These changes are sterically driven by the observed increase of the nickel-oxygen distances (\ensuremath{\Delta}${\mathit{d}}_{\mathrm{Ni}\mathrm{\ensuremath{-}}\mathrm{O}}$\ensuremath{\approxeq}+0.004 \AA{}) in the insulating (low-temperature) phase. The results of valence-bond calculations suggest the existence of ${\mathrm{Ni}}^{3+}$(${\mathit{d}}^{7}$) and ${\mathit{R}}^{3+}$ states for nickel and rare earth.

389 citations

Journal ArticleDOI
TL;DR: The first observation of changes in the crystal symmetry at the metal-insulator transition in perovskites was made in this article, where the authors reported the presence of two alternating NiO octahedra with expanded (Ni1) and contracted (Ni2) Ni-O bonds and a magnetic structure.
Abstract: Neutron and synchrotron diffraction data provide the first observation of changes in the crystal symmetry at the metal-insulator transition in $R{\mathrm{NiO}}_{3}$ perovskites. At high temperatures, ${\mathrm{YNiO}}_{3}$ is orthorhombic and metallic but below ${T}_{\mathrm{MI}}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}582\mathrm{K}$ it changes to a monoclinic insulator due to a charge disproportionation $(2{\mathrm{Ni}}^{3+}\ensuremath{\rightarrow}{\mathrm{Ni}}^{3+\ensuremath{\delta}}+{\mathrm{Ni}}^{3\ensuremath{-}\ensuremath{\delta}})$ that develops at the opening of the gap. We report the presence of two alternating ${\mathrm{NiO}}_{6}$ octahedra with expanded (Ni1) and contracted (Ni2) Ni-O bonds and a magnetic structure $[\mathbf{k}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}(1/2,0,1/2)]$ with unequal moments at Ni1 and Ni2 octahedra.

300 citations

Journal ArticleDOI
TL;DR: In this article, a comparative study of the influence of the rare earth size on the structural parameters of R2BaCuO5 compounds with R = rare earth atom from Sm to Lu have been studied by neutron and X-ray powder diffraction.

264 citations

Journal ArticleDOI
TL;DR: Two-dimensional mapping is made possible by an adapted method for fast acquisition of electron energy-loss spectra and is supported by simulations, which help to explain the less intuitive features.
Abstract: The simultaneous measurement of structural and chemical information at the atomic scale provides fundamental insights into the connection between form and function in materials science and nanotechnology. We demonstrate structural and chemical mapping in ${\mathrm{Bi}}_{0.5}{\mathrm{Sr}}_{0.5}{\mathrm{MnO}}_{3}$ using an aberration-corrected scanning transmission electron microscope. Two-dimensional mapping is made possible by an adapted method for fast acquisition of electron energy-loss spectra. The experimental data are supported by simulations, which help to explain the less intuitive features.

231 citations


Cited by
More filters
Journal ArticleDOI
TL;DR: It is found that even a weak magnetoelectric interaction can lead to spectacular cross-coupling effects when it induces electric polarization in a magnetically ordered state.
Abstract: Magnetism and ferroelectricity are essential to many forms of current technology, and the quest for multiferroic materials, where these two phenomena are intimately coupled, is of great technological and fundamental importance. Ferroelectricity and magnetism tend to be mutually exclusive and interact weakly with each other when they coexist. The exciting new development is the discovery that even a weak magnetoelectric interaction can lead to spectacular cross-coupling effects when it induces electric polarization in a magnetically ordered state. Such magnetic ferroelectricity, showing an unprecedented sensitivity to ap plied magnetic fields, occurs in 'frustrated magnets' with competing interactions between spins and complex magnetic orders. We summarize key experimental findings and the current theoretical understanding of these phenomena, which have great potential for tuneable multifunctional devices.

3,683 citations

Journal ArticleDOI
TL;DR: In this paper, a large variety of experiments reviewed in detail here contain results compatible with the theoretical predictions, including phase diagrams of manganite models, the stabilization of the charge/orbital/spin ordered half-doped correlated electronics (CE)-states, the importance of the naively small Heisenberg coupling among localized spins, the setup of accurate mean-field approximations, and the existence of a new temperature scale T∗ where clusters start forming above the Curie temperature, the presence of stripes in the system, and many others.

2,927 citations

01 Jan 2011

2,117 citations

Journal ArticleDOI
TL;DR: The phenomenology of exchange bias and related effects in nanostructures is reviewed in this paper, where the main applications of exchange biased nanostructure are summarized and the implications of the nanometer dimensions on some of the existing exchange bias theories are briefly discussed.

1,721 citations

Journal ArticleDOI
10 Jun 1999-Nature
TL;DR: In this article, it was shown that the magnetoresistive response increases dramatically when the Curie temperature (T C) is reduced, and that the massive magnetoresistance in low-T C systems can be explained by percolative transport through the ferromagnetic domains; this depends sensitively on the relative spin orientation of adjacent magnetoric domains which can be controlled by applied magnetic fields.
Abstract: Colossal magnetoresistance1—an unusually large change of resistivity observed in certain materials following application of magnetic field—has been extensively researched in ferromagnetic perovskite manganites. But it remains unclear why the magnetoresistive response increases dramatically when the Curie temperature (T C) is reduced. In these materials, T C varies sensitively with changing chemical pressure; this can be achieved by introducing trivalent rare-earth ions of differing size into the perovskite structure2,3,4, without affecting the valency of the Mn ions. The chemical pressure modifies local structural parameters such as the Mn–O bond distance and Mn–O–Mn bond angle, which directly influence the case of electron hopping between Mn ions (that is, the electronic bandwidth). But these effects cannot satisfactorily explain the dependence of magnetoresistance on T C. Here we demonstrate, using electron microscopy data, that the prototypical (La,Pr,Ca)MnO3 system is electronically phase-separated into a sub-micrometre-scale mixture of insulating regions (with a particular type of charge-ordering) and metallic, ferromagnetic domains. We find that the colossal magnetoresistive effect in low-T C systems can be explained by percolative transport through the ferromagnetic domains; this depends sensitively on the relative spin orientation of adjacent ferromagnetic domains which can be controlled by applied magnetic fields.

1,417 citations