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Salaheldeen M, Nafady A, Abu-Dief AM, Díaz Crespo R, Fernández-García MP, Andrés JP, López Antón R, Blanco JA, Álvarez-Alonso P. Enhancement of Exchange Bias and Perpendicular Magnetic Anisotropy in CoO/Co Multilayer Thin Films by Tuning the Alumina Template Nanohole Size. NANOMATERIALS 2022; 12:nano12152544. [PMID: 35893512 PMCID: PMC9332129 DOI: 10.3390/nano12152544] [Citation(s) in RCA: 3] [Impact Index Per Article: 1.5] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 06/15/2022] [Revised: 07/14/2022] [Accepted: 07/21/2022] [Indexed: 02/04/2023]
Abstract
The interest in magnetic nanostructures exhibiting perpendicular magnetic anisotropy and exchange bias (EB) effect has increased in recent years owing to their applications in a new generation of spintronic devices that combine several functionalities. We present a nanofabrication process used to induce a significant out-of-plane component of the magnetic easy axis and EB. In this study, 30 nm thick CoO/Co multilayers were deposited on nanostructured alumina templates with a broad range of pore diameters, 34 nm ≤ Dp ≤ 96 nm, maintaining the hexagonal lattice parameter at 107 nm. Increase of the exchange bias field (HEB) and the coercivity (HC) (12 times and 27 times, respectively) was observed in the nanostructured films compared to the non-patterned film. The marked dependence of HEB and HC with antidot hole diameters pinpoints an in-plane to out-of-plane changeover of the magnetic anisotropy at a nanohole diameter of ∼75 nm. Micromagnetic simulation shows the existence of antiferromagnetic layers that generate an exceptional magnetic configuration around the holes, named as antivortex-state. This configuration induces extra high-energy superdomain walls for edge-to-edge distance >27 nm and high-energy stripe magnetic domains below 27 nm, which could play an important role in the change of the magnetic easy axis towards the perpendicular direction.
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Affiliation(s)
- Mohamed Salaheldeen
- Physics Department, Faculty of Science, Sohag University, Sohag 82524, Egypt
- Departamento de Física, Universidad de Oviedo, C/Federico García Lorca 18, 33007 Oviedo, Spain; (R.D.C.); (M.P.F.-G.); (J.A.B.)
- Departamento de Física Aplicada, EIG, Universidad del País Vasco, UPV/EHU, 20018 San Sebastián, Spain
- Correspondence: (M.S.); (P.Á.-A.)
| | - Ayman Nafady
- Chemistry Department, College of Science, King Saud University, Riyadh 11451, Saudi Arabia;
| | - Ahmed M. Abu-Dief
- Chemistry Department, Faculty of Science, Sohag University, Sohag 82524, Egypt;
| | - Rosario Díaz Crespo
- Departamento de Física, Universidad de Oviedo, C/Federico García Lorca 18, 33007 Oviedo, Spain; (R.D.C.); (M.P.F.-G.); (J.A.B.)
| | - María Paz Fernández-García
- Departamento de Física, Universidad de Oviedo, C/Federico García Lorca 18, 33007 Oviedo, Spain; (R.D.C.); (M.P.F.-G.); (J.A.B.)
| | - Juan Pedro Andrés
- Instituto Regional de Investigación Científica Aplicada (IRICA), Universidad de Castilla-La Mancha, 13071 Ciudad Real, Spain; (J.P.A.); (R.L.A.)
- Departamento de Física Aplicada, Universidad de Castilla-La Mancha, 13071 Ciudad Real, Spain
| | - Ricardo López Antón
- Instituto Regional de Investigación Científica Aplicada (IRICA), Universidad de Castilla-La Mancha, 13071 Ciudad Real, Spain; (J.P.A.); (R.L.A.)
- Departamento de Física Aplicada, Universidad de Castilla-La Mancha, 13071 Ciudad Real, Spain
| | - Jesús A. Blanco
- Departamento de Física, Universidad de Oviedo, C/Federico García Lorca 18, 33007 Oviedo, Spain; (R.D.C.); (M.P.F.-G.); (J.A.B.)
| | - Pablo Álvarez-Alonso
- Departamento de Física, Universidad de Oviedo, C/Federico García Lorca 18, 33007 Oviedo, Spain; (R.D.C.); (M.P.F.-G.); (J.A.B.)
- Instituto Universitario de Tecnología Industrial de Asturias, Universidad de Oviedo, 33203 Gijón, Spain
- Correspondence: (M.S.); (P.Á.-A.)
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Träger N, Gruszecki P, Lisiecki F, Groß F, Förster J, Weigand M, Głowiński H, Kuświk P, Dubowik J, Krawczyk M, Gräfe J. Demonstration of k-vector selective microscopy for nanoscale mapping of higher order spin wave modes. NANOSCALE 2020; 12:17238-17244. [PMID: 32558843 DOI: 10.1039/d0nr02132f] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/11/2023]
Abstract
As a potential route towards beyond CMOS computing magnonic waveguides show outstanding properties regarding fundamental wave physics and data transmission. Here, we use time resolved scanning transmission X-ray microscopy to directly observe spin waves in magnonic permalloy waveguides with nanoscale resolution. Additionally, we demonstrate an approach for k-vector selective imaging to deconvolute overlapping modes in real space measurements. Thereby, we observe efficient excitation of symmetric and antisymmetric modes. The profiles of higher order modes that arise from sub-micron confinement are precisely mapped out and compared to analytical models. Thus, we lay a basis for the design of multimode spin wave transmission systems and demonstrate a general technique for k-specific microscopy that can also be used beyond the field of magnonics.
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Affiliation(s)
- Nick Träger
- Max Planck Institute for Intelligent Systems, Stuttgart, Germany.
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Salaheldeen M, Vega V, Ibabe A, Jaafar M, Asenjo A, Fernandez A, Prida VM. Tailoring of Perpendicular Magnetic Anisotropy in Dy 13Fe 87 Thin Films with Hexagonal Antidot Lattice Nanostructure. NANOMATERIALS 2018; 8:nano8040227. [PMID: 29642476 PMCID: PMC5923557 DOI: 10.3390/nano8040227] [Citation(s) in RCA: 10] [Impact Index Per Article: 1.7] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 03/10/2018] [Revised: 03/31/2018] [Accepted: 04/05/2018] [Indexed: 11/16/2022]
Abstract
In this article, the magnetic properties of hexagonally ordered antidot arrays made of Dy13Fe87 alloy are studied and compared with corresponding ones of continuous thin films with the same compositions and thicknesses, varying between 20 nm and 50 nm. Both samples, the continuous thin films and antidot arrays, were prepared by high vacuum e-beam evaporation of the alloy on the top-surface of glass and hexagonally self-ordered nanoporous alumina templates, which serve as substrates, respectively. By using a highly sensitive magneto-optical Kerr effect (MOKE) and vibrating sample magnetometer (VSM) measurements an interesting phenomenon has been observed, consisting in the easy magnetization axis transfer from a purely in-plane (INP) magnetic anisotropy to out-of-plane (OOP) magnetization. For the 30 nm film thickness we have measured the volume hysteresis loops by VSM with the easy magnetization axis lying along the OOP direction. Using magnetic force microscopy measurements (MFM), there is strong evidence to suggest that the formation of magnetic domains with OOP magnetization occurs in this sample. This phenomenon can be of high interest for the development of novel magnetic and magneto-optic perpendicular recording patterned media based on template-assisted deposition techniques.
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Affiliation(s)
- Mohamed Salaheldeen
- Physics Department, Faculty of Science, Sohag University, 82524 Sohag, Egypt.
- Depto. Física, Universidad de Oviedo, C/Federico Garcia Lorca 18, 33007 Oviedo, Asturias, Spain.
| | - Victor Vega
- Depto. Física, Universidad de Oviedo, C/Federico Garcia Lorca 18, 33007 Oviedo, Asturias, Spain.
- Laboratorio Membranas Nanoporosas, Servicios Científico-Técnicos, Universidad de Oviedo, Campus El Cristo s/n, 33006 Oviedo, Asturias, Spain.
| | - Angel Ibabe
- Instituto de Ciencia de Materiales de Madrid, CSIC, Cantoblanco, 28049 Madrid, Spain.
| | - Miriam Jaafar
- Instituto de Ciencia de Materiales de Madrid, CSIC, Cantoblanco, 28049 Madrid, Spain.
| | - Agustina Asenjo
- Instituto de Ciencia de Materiales de Madrid, CSIC, Cantoblanco, 28049 Madrid, Spain.
| | - Agustin Fernandez
- Depto. Física, Universidad de Oviedo, C/Federico Garcia Lorca 18, 33007 Oviedo, Asturias, Spain.
| | - Victor M Prida
- Depto. Física, Universidad de Oviedo, C/Federico Garcia Lorca 18, 33007 Oviedo, Asturias, Spain.
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Schneider T, Langer M, Alekhina J, Kowalska E, Oelschlägel A, Semisalova A, Neudert A, Lenz K, Potzger K, Kostylev MP, Fassbender J, Adeyeye AO, Lindner J, Bali R. Programmability of Co-antidot lattices of optimized geometry. Sci Rep 2017; 7:41157. [PMID: 28145463 PMCID: PMC5286523 DOI: 10.1038/srep41157] [Citation(s) in RCA: 8] [Impact Index Per Article: 1.1] [Reference Citation Analysis] [Abstract] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 09/19/2016] [Accepted: 12/14/2016] [Indexed: 11/30/2022] Open
Abstract
Programmability of stable magnetization configurations in a magnetic device is a highly desirable feature for a variety of applications, such as in magneto-transport and spin-wave logic. Periodic systems such as antidot lattices may exhibit programmability; however, to achieve multiple stable magnetization configurations the lattice geometry must be optimized. We consider the magnetization states in Co-antidot lattices of ≈50 nm thickness and ≈150 nm inter-antidot distance. Micromagnetic simulations were applied to investigate the magnetization states around individual antidots during the reversal process. The reversal processes predicted by micromagnetics were confirmed by experimental observations. Magnetization reversal in these antidots occurs via field driven transition between 3 elementary magnetization states – termed G, C and Q. These magnetization states can be described by vectors, and the reversal process proceeds via step-wise linear operations on these vector states. Rules governing the co-existence of the three magnetization states were empirically observed. It is shown that in an n × n antidot lattice, a variety of field switchable combinations of G, C and Q can occur, indicating programmability of the antidot lattices.
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Affiliation(s)
- Tobias Schneider
- Helmholtz-Zentrum Dresden-Rossendorf, Institute of Ion Beam Physics and Materials Research, 01328 Dresden, Germany.,Technische Universität Chemnitz, Institute of Physics, 09107 Chemnitz, Germany
| | - Manuel Langer
- Helmholtz-Zentrum Dresden-Rossendorf, Institute of Ion Beam Physics and Materials Research, 01328 Dresden, Germany.,Technische Universität Dresden, Department of Physics, 01069 Dresden, Germany
| | - Julia Alekhina
- Helmholtz-Zentrum Dresden-Rossendorf, Institute of Ion Beam Physics and Materials Research, 01328 Dresden, Germany.,Lomonosov Moscow State University, Faculty of Physics, 119991 Moscow, Russia
| | - Ewa Kowalska
- Helmholtz-Zentrum Dresden-Rossendorf, Institute of Ion Beam Physics and Materials Research, 01328 Dresden, Germany.,Technische Universität Dresden, Department of Physics, 01069 Dresden, Germany
| | - Antje Oelschlägel
- Helmholtz-Zentrum Dresden-Rossendorf, Institute of Ion Beam Physics and Materials Research, 01328 Dresden, Germany.,Technische Universität Dresden, Department of Physics, 01069 Dresden, Germany
| | - Anna Semisalova
- Helmholtz-Zentrum Dresden-Rossendorf, Institute of Ion Beam Physics and Materials Research, 01328 Dresden, Germany.,Lomonosov Moscow State University, Faculty of Physics, 119991 Moscow, Russia
| | - Andreas Neudert
- Helmholtz-Zentrum Dresden-Rossendorf, Institute of Ion Beam Physics and Materials Research, 01328 Dresden, Germany
| | - Kilian Lenz
- Helmholtz-Zentrum Dresden-Rossendorf, Institute of Ion Beam Physics and Materials Research, 01328 Dresden, Germany
| | - Kay Potzger
- Helmholtz-Zentrum Dresden-Rossendorf, Institute of Ion Beam Physics and Materials Research, 01328 Dresden, Germany
| | - Mikhail P Kostylev
- University of Western Australia, School of Physics, 6009 Crawley, Australia
| | - Jürgen Fassbender
- Helmholtz-Zentrum Dresden-Rossendorf, Institute of Ion Beam Physics and Materials Research, 01328 Dresden, Germany.,Technische Universität Dresden, Department of Physics, 01069 Dresden, Germany
| | - Adekunle O Adeyeye
- National University of Singapore, Department of Electrical and Computer Engineering, 117576 Singapore
| | - Jürgen Lindner
- Helmholtz-Zentrum Dresden-Rossendorf, Institute of Ion Beam Physics and Materials Research, 01328 Dresden, Germany
| | - Rantej Bali
- Helmholtz-Zentrum Dresden-Rossendorf, Institute of Ion Beam Physics and Materials Research, 01328 Dresden, Germany
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Béron F, Kaidatzis A, Velo MF, Arzuza LCC, Palmero EM, Del Real RP, Niarchos D, Pirota KR, García-Martín JM. Nanometer Scale Hard/Soft Bilayer Magnetic Antidots. NANOSCALE RESEARCH LETTERS 2016; 11:86. [PMID: 26873261 PMCID: PMC4752520 DOI: 10.1186/s11671-016-1302-3] [Citation(s) in RCA: 3] [Impact Index Per Article: 0.4] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 11/03/2015] [Accepted: 01/31/2016] [Indexed: 06/01/2023]
Abstract
The effect of arrays of nanometer scale pores on the magnetic properties of thin films has been analyzed. Particularly, we investigated the influence of the out-of-plane magnetization component created by the nanopores on the in-plane magnetic behavior of patterned hard/soft magnetic thin films in antidot morphology. Its influence on the coupling in Co/Py bilayers of few tens of nanometer thick is compared for disordered and ordered antidots of 35-nm diameter. The combination of magneto-optical Kerr effect (MOKE) and first-order reversal curve (FORC) technique allows probing the effects of the induced perpendicular magnetization component on the bilayer magnetic behavior, while magnetic force microscopy (MFM) is used to image it. We found that ordered antidots yield a stronger out-of-plane component than disordered ones, influencing in a similar manner the hard layer global in-plane magnetic behavior if with a thin or without soft layer. However, its influence changes with a thicker soft layer, which may be an indication of a weaker coupling.
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Affiliation(s)
- Fanny Béron
- Instituto de Física Gleb Wataghin (IFGW), Universidade Estadual de Campinas (UNICAMP), Campinas, SP, 13083-859, Brazil.
| | - Andreas Kaidatzis
- Institute of Nanoscience and Nanotechnology, NCSR "Demokritos", Aghia Paraskevi, Attiki, Athens, 15310, Greece.
| | - Murilo F Velo
- Instituto de Física Gleb Wataghin (IFGW), Universidade Estadual de Campinas (UNICAMP), Campinas, SP, 13083-859, Brazil.
| | - Luis C C Arzuza
- Instituto de Física Gleb Wataghin (IFGW), Universidade Estadual de Campinas (UNICAMP), Campinas, SP, 13083-859, Brazil.
| | - Ester M Palmero
- Instituto de Ciencia de Materiales de Madrid (ICMM), Consejo Superior de Investigaciones Científicas (CSIC), Madrid, 28049, Spain.
| | - Rafael P Del Real
- Instituto de Ciencia de Materiales de Madrid (ICMM), Consejo Superior de Investigaciones Científicas (CSIC), Madrid, 28049, Spain.
| | - Dimitrios Niarchos
- Institute of Nanoscience and Nanotechnology, NCSR "Demokritos", Aghia Paraskevi, Attiki, Athens, 15310, Greece.
| | - Kleber R Pirota
- Instituto de Física Gleb Wataghin (IFGW), Universidade Estadual de Campinas (UNICAMP), Campinas, SP, 13083-859, Brazil.
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Wiedwald U, Gräfe J, Lebecki KM, Skripnik M, Haering F, Schütz G, Ziemann P, Goering E, Nowak U. Magnetic switching of nanoscale antidot lattices. BEILSTEIN JOURNAL OF NANOTECHNOLOGY 2016; 7:733-50. [PMID: 27335762 PMCID: PMC4901900 DOI: 10.3762/bjnano.7.65] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.1] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Received: 11/30/2015] [Accepted: 04/30/2016] [Indexed: 06/06/2023]
Abstract
We investigate the rich magnetic switching properties of nanoscale antidot lattices in the 200 nm regime. In-plane magnetized Fe, Co, and Permalloy (Py) as well as out-of-plane magnetized GdFe antidot films are prepared by a modified nanosphere lithography allowing for non-close packed voids in a magnetic film. We present a magnetometry protocol based on magneto-optical Kerr microscopy elucidating the switching modes using first-order reversal curves. The combination of various magnetometry and magnetic microscopy techniques as well as micromagnetic simulations delivers a thorough understanding of the switching modes. While part of the investigations has been published before, we summarize these results and add significant new insights in the magnetism of exchange-coupled antidot lattices.
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Affiliation(s)
- Ulf Wiedwald
- Institute of Solid State Physics, Ulm University, Albert-Einstein-Allee 11, 89069 Ulm, Germany
- Faculty of Physics and Center for Nanointegration Duisburg-Essen (CENIDE), University of Duisburg-Essen, Lotharstr. 1, 47057 Duisburg, Germany
| | - Joachim Gräfe
- Max-Planck-Institute for Intelligent Systems, Heisenbergstr. 3, 70569 Stuttgart, Germany
| | - Kristof M Lebecki
- Department of Physics, University of Konstanz, 78457 Konstanz, Germany
- IT4Innovations Centre, VSB Technical University of Ostrava, Czech Republic
| | - Maxim Skripnik
- Department of Physics, University of Konstanz, 78457 Konstanz, Germany
| | - Felix Haering
- Institute of Solid State Physics, Ulm University, Albert-Einstein-Allee 11, 89069 Ulm, Germany
| | - Gisela Schütz
- Max-Planck-Institute for Intelligent Systems, Heisenbergstr. 3, 70569 Stuttgart, Germany
| | - Paul Ziemann
- Institute of Solid State Physics, Ulm University, Albert-Einstein-Allee 11, 89069 Ulm, Germany
| | - Eberhard Goering
- Max-Planck-Institute for Intelligent Systems, Heisenbergstr. 3, 70569 Stuttgart, Germany
| | - Ulrich Nowak
- Department of Physics, University of Konstanz, 78457 Konstanz, Germany
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