Magnetic Force Microscopy of Superparamagnetic Nanoparticles
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Magnetism, Magnetic Properties, Magnetochemistry
Magnetism, Magnetic Properties, Magnetochemistry 1 Magnetism All matter is electronic Positive/negative charges - bound by Coulombic forces Result of electric field E between charges, electric dipole Electric and magnetic fields = the electromagnetic interaction (Oersted, Maxwell) Electric field = electric +/ charges, electric dipole Magnetic field ??No source?? No magnetic charges, N-S No magnetic monopole Magnetic field = motion of electric charges (electric current, atomic motions) Magnetic dipole – magnetic moment = i A [A m2] 2 Electromagnetic Fields 3 Magnetism Magnetic field = motion of electric charges • Macro - electric current • Micro - spin + orbital momentum Ampère 1822 Poisson model Magnetic dipole – magnetic (dipole) moment [A m2] i A 4 Ampere model Magnetism Microscopic explanation of source of magnetism = Fundamental quantum magnets Unpaired electrons = spins (Bohr 1913) Atomic building blocks (protons, neutrons and electrons = fermions) possess an intrinsic magnetic moment Relativistic quantum theory (P. Dirac 1928) SPIN (quantum property ~ rotation of charged particles) Spin (½ for all fermions) gives rise to a magnetic moment 5 Atomic Motions of Electric Charges The origins for the magnetic moment of a free atom Motions of Electric Charges: 1) The spins of the electrons S. Unpaired spins give a paramagnetic contribution. Paired spins give a diamagnetic contribution. 2) The orbital angular momentum L of the electrons about the nucleus, degenerate orbitals, paramagnetic contribution. The change in the orbital moment -
Two-Dimensional Field-Sensing Map and Magnetic Anisotropy Dispersion
PHYSICAL REVIEW B 83, 144416 (2011) Two-dimensional field-sensing map and magnetic anisotropy dispersion in magnetic tunnel junction arrays Wenzhe Zhang* and Gang Xiao† Department of Physics, Brown University, Providence, Rhode Island 02912, USA Matthew J. Carter Micro Magnetics, Inc., 617 Airport Road, Fall River, Massachusetts 02720, USA (Received 22 July 2010; revised manuscript received 24 January 2011; published 22 April 2011) Due to the inherent disorder in local structures, anisotropy dispersion exists in almost all systems that consist of multiple magnetic tunnel junctions (MTJs). Aided by micromagnetic simulations based on the Stoner-Wohlfarth (S-W) model, we used a two-dimensional field-sensing map to study the effect of anisotropy dispersion in MTJ arrays. First, we recorded the field sensitivity value of an MTJ array as a function of the easy- and hard-axis bias fields, and then extracted the anisotropy dispersion in the array by comparing the experimental sensitivity map to the simulated map. Through a mean-square-error-based image processing technique, we found the best match for our experimental data, and assigned a pair of dispersion numbers (anisotropy angle and anisotropy constant) to the array. By varying each of the parameters one at a time, we were able to discover the dependence of field sensitivity on magnetoresistance ratio, coercivity, and magnetic anisotropy dispersion. The effects from possible edge domains are also discussed to account for a correction term in our analysis of anisotropy angle distribution using the S-W model. We believe this model is a useful tool for monitoring the formation and evolution of anisotropy dispersion in MTJ systems, and can facilitate better design of MTJ-based devices. -
Tailored Magnetic Properties of Exchange-Spring and Ultra Hard Nanomagnets
Max-Planck-Institute für Intelligente Systeme Stuttgart Tailored Magnetic Properties of Exchange-Spring and Ultra Hard Nanomagnets Kwanghyo Son Dissertation An der Universität Stuttgart 2017 Tailored Magnetic Properties of Exchange-Spring and Ultra Hard Nanomagnets Von der Fakultät Mathematik und Physik der Universität Stuttgart zur Erlangung der Würde eines Doktors der Naturwissenschaften (Dr. rer. nat.) genehmigte Abhandlung Vorgelegt von Kwanghyo Son aus Seoul, SüdKorea Hauptberichter: Prof. Dr. Gisela Schütz Mitberichter: Prof. Dr. Sebastian Loth Tag der mündlichen Prüfung: 04. Oktober 2017 Max‐Planck‐Institut für Intelligente Systeme, Stuttgart 2017 II III Contents Contents ..................................................................................................................................... 1 Chapter 1 ................................................................................................................................... 1 General Introduction ......................................................................................................... 1 Structure of the thesis ....................................................................................................... 3 Chapter 2 ................................................................................................................................... 5 Basic of Magnetism .......................................................................................................... 5 2.1 The Origin of Magnetism ....................................................................................... -
Understanding the Origin of Magnetocrystalline Anisotropy in Pure and Fe/Si Substituted Smco5
Understanding the origin of magnetocrystalline anisotropy in pure and Fe/Si substituted SmCo5 *Rajiv K. Chouhan1,2,3, A. K. Pathak3, and D. Paudyal3 1CNR-NANO Istituto Nanoscienze, Centro S3, I-41125 Modena, Italy 2Harish-Chandra Research Institute, HBNI, Jhunsi, Allahabad 211019, India 3The Ames Laboratory, U.S. Department of Energy, Iowa State University, Ames, IA 50011–3020, USA We report magnetocrystalline anisotropy of pure and Fe/Si substituted SmCo5. The calculations were performed using the advanced density functional theory (DFT) including onsite electron-electron correlation and spin orbit coupling. Si substitution substantially reduces both uniaxial magnetic anisotropy and magnetic moment. Fe substitution with the selective site, on the other hand, enhances the magnetic moment with limited chemical stability. The magnetic hardness of SmCo5 is governed by Sm 4f localized orbital contributions, which get flatten and split with the substitution of Co (2c) with Si/Fe atoms, except the Fe substitution at 3g site. It is also confirmed that Si substitutions favor the thermodynamic stability on the contrary to diminishing the magnetic and anisotropic effect in SmCo5 at either site. INTRODUCTION Search for high-performance permanent magnets is always being a challenging task for modern technological applications as they are key driving components for propulsion motors, wind turbines and several other direct or indirect market consumer products. Curie temperature Tc, magnetic anisotropy, and saturation magnetization Ms, of the materials, are some basic fundamental properties used to classify the permanent magnets. At Curie temperature a material loses its ferromagnetic properties, hence higher the Tc, better is the magnets to be used under extreme conditions. -
Superparamagnetism and Magnetic Properties of Ni Nanoparticles Embedded in Sio2
PHYSICAL REVIEW B 66, 104406 ͑2002͒ Superparamagnetism and magnetic properties of Ni nanoparticles embedded in SiO2 F. C. Fonseca, G. F. Goya, and R. F. Jardim* Instituto de Fı´sica, Universidade de Sa˜o Paulo, CP 66318, 05315-970, Sa˜o Paulo, SP, Brazil R. Muccillo Centro Multidisciplinar de Desenvolvimento de Materiais Ceraˆmicos CMDMC, CCTM-Instituto de Pesquisas Energe´ticas e Nucleares, CP 11049, 05422-970, Sa˜o Paulo, SP, Brazil N. L. V. Carren˜o, E. Longo, and E. R. Leite Centro Multidisciplinar de Desenvolvimento de Materiais Ceraˆmicos CMDMC, Departamento de Quı´mica, Universidade Federal de Sa˜o Carlos, CP 676, 13560-905, Sa˜o Carlos, SP, Brazil ͑Received 4 March 2002; published 6 September 2002͒ We have performed a detailed characterization of the magnetic properties of Ni nanoparticles embedded in a SiO2 amorphous matrix. A modified sol-gel method was employed which resulted in Ni particles with ϳ Ϸ average radius 3 nm, as inferred by TEM analysis. Above the blocking temperature TB 20 K for the most diluted sample, magnetization data show the expected scaling of the M/M S vs H/T curves for superparamag- netic particles. The hysteresis loops were found to be symmetric about zero field axis with no shift via Ͻ exchange bias, suggesting that Ni particles are free from an oxide layer. For T TB the magnetic behavior of these Ni nanoparticles is in excellent agreement with the predictions of randomly oriented and noninteracting magnetic particles, as suggested by the temperature dependence of the coercivity field that obeys the relation ϭ Ϫ 1/2 ϳ HC(T) HC0͓1 (T/TB) ͔ below TB with HC0 780 Oe. -
Magnetic Anisotropy and Exchange in (001) Textured Fept-Based Nanostructures
University of Nebraska - Lincoln DigitalCommons@University of Nebraska - Lincoln Theses, Dissertations, and Student Research: Department of Physics and Astronomy Physics and Astronomy, Department of 12-2013 Magnetic Anisotropy and Exchange in (001) Textured FePt-based Nanostructures Tom George University of Nebraska-Lincoln, [email protected] Follow this and additional works at: https://digitalcommons.unl.edu/physicsdiss Part of the Condensed Matter Physics Commons George, Tom, "Magnetic Anisotropy and Exchange in (001) Textured FePt-based Nanostructures" (2013). Theses, Dissertations, and Student Research: Department of Physics and Astronomy. 31. https://digitalcommons.unl.edu/physicsdiss/31 This Article is brought to you for free and open access by the Physics and Astronomy, Department of at DigitalCommons@University of Nebraska - Lincoln. It has been accepted for inclusion in Theses, Dissertations, and Student Research: Department of Physics and Astronomy by an authorized administrator of DigitalCommons@University of Nebraska - Lincoln. MAGNETIC ANISOTROPY AND EXCHANGE IN (001) TEXTURED FePt-BASED NANOSTRUCTURES by Tom Ainsley George A DISSERTATION Presented to the Faculty of The Graduate College at the University of Nebraska In Partial Fulfillment of Requirements For the Degree of Doctor of Philosophy Major: Physics and Astronomy Under the Supervision of Professor David J. Sellmyer Lincoln, Nebraska December, 2013 MAGNETIC ANISOTROPY AND EXCHANGE IN (001) TEXTURED FePt-BASED NANOSTRUCTURES Tom Ainsley George, Ph.D. University of Nebraska, 2013 Adviser: David J. Sellmyer Hard-magnetic L10 phase FePt has been demonstrated as a promising candidate for future nanomagnetic applications, especially magnetic recording at areal densities approaching 10 Tb/in2. Realization of FePt’s potential in recording media requires control of grain size and intergranular exchange interactions in films with high degrees of L10 order and (001) crystalline texture, including high perpendicular magnetic anisotropy. -
Magnetic Dynamics of Single Domain Ni Nanoparticles
J. Appl. Phys. 93, 6531 (2003); doi:10.1063/1.1540032 (3 pages) AF-13 Magnetic dynamics of single domain Ni nanoparticles G. F. Goya, F.C. Fonseca, and R. F. Jardim Instituto de Física, Universidade de São Paulo, CP 66318, 05315-970, São Paulo, Brazil R. Muccillo Centro Multidisciplinar de Desenvolvimento de Materiais Cerâmicos CMDMC, CCTM-Instituto de Pesquisas Energéticas e Nucleares CP 11049, 05422-970, São Paulo, SP, Brazil N. L. V. Carreño, E. Longo, and E.R. Leite Centro Multidisciplinar de Desenvolvimento de Materiais Cerâmicos CMDMC, Departamento de Química, Universidade Federal de São Carlos CP 676, 13560-905, São Carlos, SP, Brazil The dynamic magnetic properties of Ni nanoparticles diluted in an amorphous SiO2 matrix prepared from a modified sol-ge l me thod have been studied by the frequency f dependence of the ac magnetic susceptibility χ(T). For samples with similar average radii ~ 3-4 nm, an increase of the blocking temperature from TB ~ 20 to ~ 40 K was observed for Ni concentrations of ~ 1.5 and 5 wt.%, respectively, assigned to the effects of dipolar interactions. Both the in-phase χ’(T) and the out-of- phase χ’’(T) maxima follow the predictions of the thermally activated Néel-Arrhenius model. The effective magnetic anisotropy constant Keff inferred from χ’’(T) versus f data for the 1.5 wt.% Ni sample is close to the value of the magnetocrystalline anisotropy of bulk Ni, suggesting that surface effects are negligible in the present samples. In addition, the contribution from dipolar interactions to the total anisotropy energy Ea in specimens with 5 wt.% Ni was found to be comparable to the intrinsic magnetocrystalline anisotropy barrier. -
Discovery of Ferromagnetism with Large Magnetic Anisotropy in Zrmnp and Hfmnp Tej N
Discovery of ferromagnetism with large magnetic anisotropy in ZrMnP and HfMnP Tej N. Lamichhane,1,2 Valentin Taufour,1,2 Morgan W. Masters,1 David S. Parker,3 Udhara S. Kaluarachchi,1,2 Srinivasa Thimmaiah,2 Sergey L. Bud’ko,1,2 and Paul C. Canfield1,2 1)Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, U.S.A. 2)The Ames Laboratory, US Department of Energy, Iowa State University, Ames, Iowa 50011, USA 3)Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, TN 37831, USA ZrMnP and HfMnP single crystals are grown by a self-flux growth technique and structural as well as tem- perature dependent magnetic and transport properties are studied. Both compounds have an orthorhombic crystal structure. ZrMnP and HfMnP are ferromagnetic with Curie temperatures around 370 K and 320 K respectively. The spontaneous magnetizations of ZrMnP and HfMnP are determined to be 1.9 µB/f.u. and 2.1 µB/f.u. respectively at 50 K. The magnetocaloric effect of ZrMnP in term of entropy change (∆S) is estimated to be −6.7 kJm−3K−1 around 369 K. The easy axis of magnetization is [100] for both compounds, with a small anisotropy relative to the [010] axis. At 50 K, the anisotropy field along the [001] axis is ∼ 4.6T for ZrMnP and ∼ 10 T for HfMnP. Such large magnetic anisotropy is remarkable considering the absence of rare-earth elements in these compounds. The first principle calculation correctly predicts the magnetization and hard axis orientation for both compounds, and predicts the experimental HfMnP anisotropy field within 25 percent. -
Magnetic Anisotropy in Molecular Nanomagnets
Spectroscopic Investigations of Magnetic Anisotropy in Molecular Nanomagnets ECMM workshop on Magnetic Anisotropy Karlsruhe, 11th‐12th October 2013 Prof. Dr. Joris van Slageren Institut für Physikalische Chemie Dr. Shang‐Da Jiang 1. Physikalisches Institut Universität Stuttgart Germany Contents 2 1. Introduction 4. Inelastic Neutron Scattering 1.1 Magnetic Anisotropy 4.1 Theoretical background and Experimental Considerations 1.2 Magnetic Anisotropy in Transition Metal Clusters 4.2 Examples 1.3 Magnetic Anisotropy in f‐Elements 5. Electronic Absorption and Luminescence 2. Single‐crystal SQUID measurements 5.1 Electronic Absorption (f elements) 2.1 Motivation 5.2 Luminescence (f elements) 2.2 Magnetic susceptibility tensor 5.3 Magnetic circular dichroism (transition metal clusters, f elements). 2.3 Determination 3. High‐frequency EPR spectroscopy 3.1 Theoretical background and Experimental Considerations 3.2 Examples 3.3 Frequency Domain EPR Contents Literature 3 A. Abragam/B. Bleany – Electron Paramagnetic Resonance of Transition Ions, 1970 N.M. Atherton – Principles of Electron Spin Resonance, 1993. R. Boča – Theoretical Foundations of Molecular Magnetism, 1999 R. Carlin –Magnetochemistry, 1986 C. Görller‐Wallrand, K. Binnemans in Handbook on the Physics and Chemistry of Rare Earths, Vol. 23, http://dx.doi.org/10.1016/S0168‐1273(96)23006‐5 O. Kahn –Molecular Magnetism, 1993 F.E. Mabbs/D.J. Machin – Magnetism and Transition Metal Complexes, Chapman and Hall, London, 1973 K.R. Lea, M.J.M. Leask, W.P. Wolf, J. Phys. Chem. Solids, 23, 1381 (1962) H. Lueken – Magnetochemie, 1999 H. Lueken – Course of lectures on magnetism of lanthanide ions under varying ligand and magnetic fields, http://obelix.physik.uni‐ bielefeld.de/~schnack/molmag/material/Lueken‐kurslan_report.pdf 2008 D.J. -
Controlling the Magnetic Anisotropy of Van Der Waals Ferromagnet Fe3gete2
Controlling the magnetic anisotropy of van der Waals ferromagnet Fe3GeTe2 through hole doping Se Young Park1,2,†, Dong Seob Kim3,†, Yu Liu4, Jinwoong Hwang5,6, Younghak Kim7, Wondong Kim8, Jae-Young Kim9, Cedomir Petrovic4, Choongyu Hwang6, Sung-Kwan Mo5, Hyung-jun Kim3, Byoung-Chul Min3, Hyun Cheol Koo3, Joonyeon Chang3, Chaun Jang3,*, Jun Woo Choi3,*, and Hyejin Ryu3,* 1Center for Correlated Electron Systems, Institute for Basic Science (IBS), Seoul 08826, Korea 2Department of Physics and Astronomy, Seoul National University (SNU), Seoul 08826, Korea 3Center for Spintronics, Korea Institute of Science and Technology (KIST), Seoul 02792, Korea 4Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, United States 5Advanced Light Source, Lawrence Berkeley National Laboratory, Berkeley, CA 94720, USA 6Department of Physics, Pusan National University, Busan 46241, Korea 7Pohang Accelerator Laboratory, Pohang University of Science and Technology, Pohang 37673 Korea 8Quantum Technology Institute, Korea Research Institute of Standards and Science (KRISS), Daejeon 34113, Korea 9Center for Artificial Low Dimensional Electronic Systems, Institute for Basic Science (IBS), Pohang 37673, Republic of Korea † These authors contributed equally to this work. 1 *(C.J.) e-mail: [email protected], Tel: +82-2-958-6713. (J. C.) e-mail: [email protected], Tel: +82-2-958-6445. (H.R.) e-mail: [email protected], +82-2-958-5705. Abstract Identifying material parameters affecting properties of ferromagnets is key to optimize materials better suited for spintronics. Magnetic anisotropy is of particular importance in van der Waals magnets, since it not only influences magnetic and spin transport properties, but also is essential to stabilizing magnetic order in the two dimensional limit. -
Magnetic Anisotropy
5 Magnetic anisotropy Magnetization reversal in thin films and some relevant experimental methods Maciej Urbaniak IFM PAN 2012 Today's plan ● Magnetocrystalline anisotropy ● Shape anisotropy ● Surface anisotropy ● Stress anisotropy Urbaniak Magnetization reversal in thin films and... Anisotropy of hysteresis – hysteresis of a sphere Fe Co easy axis Ni image source: S. Blügel, Magnetische Anisotropie und Magnetostriktion, Schriften des Forschungszentrums Jülich ISBN 3-89336-235-5, 1999 Urbaniak Magnetization reversal in thin films and... Anisotropy of hysteresis – hysteresis of a sphere 1.0 0.5 hard-axis reversal Fe Co s 0.0 easy axis M / M -0.5 -1.0 -10 -5 0 5 10 H[a.u] ●hard-axis reversal is characterized Niby higher field needed to saturate the sample ●the easy-axis reversal is usually characterized by higher hysteresis losses image source: S. Blügel, Magnetische Anisotropie und Magnetostriktion, Schriften des Forschungszentrums Jülich ISBN 3-89336-235-5, 1999 Urbaniak Magnetization reversal in thin films and... Anisotropy of hysteresis ●In case of large sphere (containing many atoms) the shape of the sample does not introduce additional anisotropy ●In small clusters the magnetization reversal is complicated by the reduction of symmetry (and the increased relative contribution of surface atoms) In Fe sphere of radius 1μm the surface atoms constitute roughly 0.04% of all atoms Urbaniak Magnetization reversal in thin films and... Anisotropy of hysteresis ●In case of large sphere (containing many atoms) the shape of the sample does not introduce additional anisotropy ●In small clusters the magnetization reversal is complicated by the reduction of symmetry (and the increased relative contribution of surface atoms) sphere-like – no breaking of crystal symmetry for high r M. -
Magnetism and Interactions Within the Single Domain Limit
Magnetism and interactions within the single domain limit: reversal, logic and information storage Zheng Li A dissertation Submitted in partial fulfillment of the requirement for the degree of Doctor of Philosophy University of Washington 2015 Reading Committee: Dr. Kannan M. Krishnan, Chair Dr. Karl F. Bohringer Dr. Marjorie Olmstead Program Authorized to Offer Degree: Materials Science & Engineering © Copyright 2015 Zheng Li ABSTRACT Magnetism and interactions within the single domain limit: reversal, logic and information storage Zheng Li Chair of the Supervisory Committee: Dr. Kannan M. Krishnan Materials Science & Engineering Magnetism and magnetic material research on mesoscopic length scale, especially on the size-dependent scaling laws have drawn much attention. From a scientific point of view, magnetic phenomena would vary dramatically as a function of length, corresponding to the multi-single magnetic domain transition. From an industrial point of view, the application of magnetic interaction within the single domain limit has been proposed and studied in the context of magnetic recording and information processing. In this thesis, we discuss the characteristic lengths in a magnetic system resulting from the competition between different energy terms. Further, we studied the two basic interactions within the single domain limit: dipole interaction and exchange interaction using two examples with practical applications: magnetic quantum-dot cellular automata (MQCA) logic and bit patterned media (BPM) magnetic recording. Dipole interactions within the single domain limit for shape-tuned nanomagnet array was studied in this thesis. We proposed a 45° clocking mechanism which would intrinsically eliminate clocking misalignments. This clocking field was demonstrated in both nanomagnet arrays for signal propagation and majority gates for logic operation.