I. Lucas
University of Zaragoza
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Featured researches published by I. Lucas.
Applied Physics Letters | 2013
R. Ramos; Takashi Kikkawa; Ken-ichi Uchida; Hiroto Adachi; I. Lucas; Myriam H. Aguirre; P. A. Algarabel; L. Morellon; Sadamichi Maekawa; Eiji Saitoh; M. R. Ibarra
We report the experimental observation of the spin Seebeck effect in magnetite thin films. The signal observed at temperatures above the Verwey transition is a contribution from both the anomalous Nernst (ANE) and spin Seebeck (SSE) effects. The contribution from the ANE of the Fe3O4 layer to the SSE is found to be negligible due to the resistivity difference between Fe3O4 and Pt layers. Below the Verwey transition, the SSE is free from the ANE of the ferromagnetic layer and it is also found to dominate over the ANE due to magnetic proximity effect on the Pt layer.
Physical Review B | 2015
R. Ramos; Takashi Kikkawa; Myriam H. Aguirre; I. Lucas; A. Anadón; Takafumi Oyake; Ken-ichi Uchida; Hiroto Adachi; Junichiro Shiomi; P. A. Algarabel; L. Morellon; Sadamichi Maekawa; Eiji Saitoh; M. R. Ibarra
Thermal spin pumping constitutes a novel mechanism for generation of spin currents; however their weak intensity constitutes a major roadblock for its usefulness. We report a phenomenon that produces a huge spin current in the central region of a multilayer system, resulting in a giant spin Seebeck effect in a structure formed by repetition of ferromagnet/metal bilayers. The result is a consequence of the interconversion of magnon and electron spin currents at the multiple interfaces. This work opens the possibility to design thin film heterostructures that may boost the application of thermal spin currents in spintronics.
Applied Physics Letters | 2015
S. Sangiao; J. M. De Teresa; L. Morellon; I. Lucas; M. C. Martinez-Velarte; M. Viret
We show here that using spin orbit coupling interactions at a metallic interface it is possible to control the sign of the spin to charge conversion in a spin pumping experiment. Using the intrinsic symmetry of the “Inverse Rashba Edelstein Effect” (IREE) in a Bi/Ag interface, the charge current changes sign when reversing the order of the Ag and Bi stacking. This confirms the IREE nature of the conversion of spin into charge in these interfaces and opens the way to tailoring the spin sensing voltage by an appropriate trilayer sequence.
APL Materials | 2016
R. Ramos; A. Anadón; I. Lucas; Ken-ichi Uchida; P. A. Algarabel; L. Morellon; Myriam H. Aguirre; Eiji Saitoh; M. R. Ibarra
We report a systematic study on the thermoelectric performance of spin Seebeck devices based on Fe3O4/Pt junction systems. We explore two types of device geometries: a spin Hall thermopile and spin Seebeck multilayer structures. The spin Hall thermopile increases the sensitivity of the spin Seebeck effect, while the increase in the sample internal resistance has a detrimental effect on the output power. We found that the spin Seebeck multilayers can overcome this limitation since the multilayers exhibit the enhancement of the thermoelectric voltage and the reduction of the internal resistance simultaneously, therefore resulting in significant power enhancement. This result demonstrates that the multilayer structures are useful for improving the thermoelectric performance of the spin Seebeck effect.
Nano Letters | 2015
Lorena Marín; Luis A. Rodríguez; C. Magen; E. Snoeck; Rémi Arras; I. Lucas; L. Morellon; P. A. Algarabel; José María de Teresa; M. Ricardo Ibarra
Epitaxial strain alters the physical properties of thin films grown on single crystal substrates. Thin film oxides are particularly apt for strain engineering new functionalities in ferroic materials. In the case of La(2/3)Ca(1/3)MnO(3) (LCMO) thin films, here we show the first experimental images obtained by electron holography demonstrating that epitaxial strain induces the segregation of a flat and uniform nonferromagnetic layer with antiferromagnetic (AFM) character at the top surface of a ferromagnetic (FM) layer, the whole film being chemical and structurally homogeneous at room temperature. For different substrates and growth conditions the tetragonality of LCMO at room temperature, defined as τ = |c - a|/a, is the driving force for a phase coexistence above an approximate critical value of τC ≈ 0.024. Theoretical calculations prove that the increased tetragonality changes the energy balance of the FM and AFM ground states in strained LCMO, enabling the formation of magnetically inhomogeneous states. This work gives the key evidence that opens a new route to synthesize strain-induced exchanged-biased FM-AFM bilayers in single thin films, which could serve as building blocks of future spintronic devices.
Journal of Applied Physics | 2007
D. Ciudad; J. L. Prieto; I. Lucas; C. Aroca; P. Sánchez
In this study, we report a method to optimize the coercivity keeping the magnetostriction value constant in electrodeposited CoP multilayers for their applications in magnetoelastic magnetic sensors. We have deposited multilayers of two different compositions of CoP (Co0.74P0.26 and Co0.83P0.17) and studied the influence of the thickness of the different layers, keeping the total thickness constant. The results show a saturation magnetostriction in between the values of the magnetostriction of the two materials and independent of the thickness of the layers. However, the reduction of the thickness of the layers is accompanied with a clear reduction of the coercive field to values as low as 0.5Oe and with a large increase of the permeability. This result shows, in the same material, an appreciable value of magnetostriction combined with low coercivity. Additionally we have found a controllable influence of the hydrogen flow on the direction of anisotropy which, in combination with other results, allows us ...
arXiv: Materials Science | 2017
Tom Seifert; Ulrike Martens; S. Günther; M. A. W. Schoen; F. Radu; X. Z. Chen; I. Lucas; R. Ramos; Myriam H. Aguirre; P. A. Algarabel; A. Anadón; H. Körner; Jakob Walowski; C. H. Back; M. R. Ibarra; L. Morellon; Eiji Saitoh; Martin Wolf; Can-Li Song; Ken-ichi Uchida; Markus Münzenberg; I. Radu; Tobias Kampfrath
Terahertz emission spectroscopy (TES) of ultrathin multilayers of magnetic and heavy metals has recently attracted much interest. This method not only provides fundamental insights into photoinduced spin transport and spin–orbit interaction at highest frequencies, but has also paved the way for applications such as efficient and ultrabroadband emitters of terahertz (THz) electromagnetic radiation. So far, predominantly standard ferromagnetic materials have been exploited. Here, by introducing a suitable figure of merit, we systematically compare the strength of THz emission from X/Pt bilayers with X being a complex ferro-, ferri- and antiferromagnetic metal, that is, dysprosium cobalt (DyCo5), gadolinium iron (Gd24Fe76), magnetite (Fe3O4) and iron rhodium (FeRh). We find that the performance in terms of spin-current generation not only depends on the spin polarization of the magnet’s conduction electrons, but also on the specific interface conditions, thereby suggesting TES to be a highly interface-sensitive technique. In general, our results are relevant for all applications that rely on the optical generation of ultrafast spin currents in spintronic metallic multilayers.
Applied Physics Letters | 2016
A. Anadón; R. Ramos; I. Lucas; P. A. Algarabel; L. Morellon; M. R. Ibarra; Myriam H. Aguirre
The dependence of Spin Seebeck effect (SSE) with the thickness of the magnetic materials is studied by means of incoherent thermal excitation. The SSE voltage signal in Fe3O4/Pt bilayer structure increases with the magnetic material thickness up to 100 nm, approximately, showing signs of saturation for larger thickness. This dependence is well described in terms of a spin current pumped in the platinum film by the magnon accumulation in the magnetic material. The spin current is generated by a gradient of temperature in the system and detected by the Pt top contact by means of inverse spin Hall effect. Calculations in the frame of the linear response theory adjust with a high degree of accuracy the experimental data, giving a thermal length scale of the magnon accumulation (Λ) of 17 ± 3 nm at 300 K and Λ = 40 ± 10 nm at 70 K.
ACS Applied Materials & Interfaces | 2014
I. Lucas; José Manuel Vila-Fungueiriño; Pilar Jiménez-Cavero; Beatriz Rivas-Murias; C. Magen; L. Morellon; F. Rivadulla
We report magnetic and electronic transport measurements across epitaxial bilayers of ferromagnetic insulator LaCoO3 and half-metallic ferromagnet La2/3Sr1/3MnO3 (LCO/LSMO: 3.5 nm/20 nm) fabricated by a chemical solution method. The I-V curves at room temperature and 4K measured with conducting atomic force microscopy (CAFM) on well-defined patterned areas exhibit the typical features of a tunneling process. The curves have been fitted to the Simmons model to determine the height (φ) and width (s) of the insulating LCO barrier. The results yield φ = 0.40 ± 0.05 eV (0.50 ± 0.01 eV) at room temperature (4K) and s = 3 nm, in good agreement with the structural analysis. Our results demonstrate that this chemical method is able to produce epitaxial heterostructures with the quality required for this type of fundamental studies and applications.
Nano Letters | 2016
Beatriz Rivas-Murias; I. Lucas; Pilar Jiménez-Cavero; C. Magen; L. Morellon; F. Rivadulla
We report the effect of interface symmetry-mismatch on the magnetic properties of LaCoO3 (LCO) thin films. Growing epitaxial LCO under tensile strain on top of cubic SrTiO3 (STO) produces a contraction along the c axis and a characteristic ferromagnetic response. However, we report here that ferromagnetism in LCO is completely suppressed when grown on top of a buffer layer of rhombohedral La2/3Sr1/3MnO3 (LSMO), in spite of identical in-plane and out-of-plane lattice deformation. This confirms that it is the lattice symmetry mismatch and not just the total strain, which determines the magnetism of LCO. On the basis of this control over the magnetic properties of LCO, we designed a multilayered structure to achieve independent rotation of the magnetization in ferromagnetic insulating LCO and half-metallic ferromagnet LSMO. This is an important step forward for the design of spin-filtering tunnel barriers based on LCO.