arXiv subjects

Roy W. Chantrell

Publications and source records attributed to Roy W. Chantrell.

27 records · Page 2Linked to original sources

arXiv2018

Roles of heating and helicity in ultrafast all-optical magnetization switching in TbFeCo

Using time-resolved magneto-optical Kerr effect (TR-MOKE) method, helicity-dependent all-optical magnetization switching (HD-AOS) is observed in ferrimagnetic TbFeCo films. The thermal effect and opto-magneto effects are separately justified after single circularly polarized laser pulse. The integral evolution of this ultrafast switching is characterized on different time scales and the defined magnetization reversal time of 460 fs is the fastest ever observed. Combining the heat effect and inverse Faraday effect (IFE), micromagnetic simulations based on a single macro-spin model are performed that reproduce HD-AOS following a linear reversal mechanism.

cond-mat.mtrl-sci↗

arXiv2017

Manifestation of higher-order inter-granular exchange in magnetic recording media

Exchange coupling between magnetic grains is essential for maintaining the stability of stored information in magnetic recording media. Using an atomistic spin model, we have investigated the coupling between neighbouring magnetic grains where magnetic impurity atoms have migrated into the non-magnetic grain boundary. We find that when the impurity density is low a biquadratic term in addition to the bilinear term is required to properly describe the inter-granular exchange coupling. The temperature dependence both terms is found to follow a power law behaviour with the biquadratic exchange constant decaying faster than the bilinear. For increasing grain boundary thickness the inter-granular exchange is lower and decays faster with temperature. Further simulations of a grain at a bit boundary show an unexpected energy minimum for in-plane magnetisation which can only be reproduced using a biquadratic exchange term.

cond-mat.mtrl-sci↗

arXiv2017

Thermally nucleated magnetic reversal in CoFeB/MgO nanodots

Power consumption is the main limitation in the development of new high performance random access memory for portable electronic devices. Magnetic RAM (MRAM) with CoFeB/MgO based magnetic tunnel junctions (MTJs) is a promising candidate for reducing the power consumption given its non-volatile nature while achieveing high performance. The dynamic properties and switching mechanisms of MTJs are critical to understanding device operation and to enable scaling of devices below 30 nm in diameter. Here we show that the magnetic reversal mechanism is incoherent and that the switching is thermally nucleated at device operating temperatures. Moreover, we find an intrinsic thermal switching field distribution arising on the sub-nanosecond timescale even in the absence of size and anisotropy distributions or material defects. These features represent the characteristic signature of the dynamic properties in MTJs and give an intrinsic limit to reversal reliability in small magnetic nanodevices.

cond-mat.mtrl-sci↗

arXiv2016

All-optical switching in granular ferromagnets caused by magnetic circular dichroism

Magnetic recording using circularly polarized femto-second laser pulses is an emerging technology that would allow write speeds much faster than existing field driven methods. However, the mechanism that drives the magnetization switching in ferromagnets is unclear. Recent theories suggest that the interaction of the light with the magnetized media induces an opto-magnetic field within the media, known as the inverse Faraday effect. Here we show that an alternative mechanism, driven by thermal excitation over the anisotropy energy barrier and a difference in the energy absorption depending on polarization, can create a net magnetization over a series of laser pulses in an ensemble of single domain grains. Only a small difference in the absorption is required to reach magnetization levels observed experimentally and the model does not preclude the role of the inverse Faraday effect but removes the necessity that the opto-magnetic field is 10s of Tesla in strength.

cond-mat.mes-hall↗

arXiv2014

Interaction potential of FePt with the MgO(001) surface

By means of density functional theory we have undertaken a structural, electronic and magnetic survey of the adsorption of the Fe_xPt_y(x,y=<4) clusters on MgO (001) surface under the generalized gradient approximation. We have tested different atomic adsorption geometries with the aim of scan a wider range of adsorption sites in order to determine the preferential surface covering. Our main conclusion in this respect is that the FePt wets the surface. The intracluster (before and after the adsorption) and cluster-to-surface binding mechanisms were investigated via the adsorption energy, charge transfer, density of states and hybridization analysis. The adsorption energy values increased for those geometries in which keeping the Fe or Pt atom @top-O, the outermost species was moved to cover the surface. In general the unsupported clusters present higher intracluster energies than the adsorbed ones being the average difference of 1.5 eV. In this regard there was a small reduction in the net magnetic moment of the supported clusters due to an internal and external rearrangement of the spin-up/-down charge. Furthermore, a complex and subtle charge transfer between different species takes place having an increasing the Pt and O population at the expense of the lost Fe charge.

cond-mat.mtrl-sci↗

arXiv2014

Atomistic modeling of magnetization reversal modes in $L1_{0}$ FePt nanodots with magnetically soft edges

Nanopatterned FePt nano-dots often exhibit low coercivity and a broad switching field distribution, which could arise due to edge damage during the patterning process causing a reduction in the $L1_{0}$ ordering required for a high magnetocrystalline anisotropy. Using an atomistic spin model, we study the magnetization reversal behavior of $L1_{0}$ FePt nanodots with soft magnetic edges. We show that reversal is initiated by nucleation for the whole range of edge widths studied. For narrow soft edges the individual nucleation events dominate reversal; for wider edges, multiple nucleation at the edge creates a circular domain wall at the interface which precedes complete reversal. Our simulations compare well with available analytical theories. The increased edge width further reduces and saturates the required nucleation field. The nucleation field and the activation volume manipulate the thermally induced switching field distribution. By control of the properties of dot edges using proper patterning methods, it should be possible to realize exchange spring bit patterned media without additional soft layers.

cond-mat.mtrl-sci↗

arXiv2014

Ultrafast thermally induced magnetic switching in synthetic ferrimagnets

Synthetic ferrimagnets are composite magnetic structures formed from two or more anti- ferromagnetically coupled magnetic sublattices with different magnetic moments. Here we report on atomistic spin simulations of the laser-induced magnetization dynamics on such synthetic ferrimag- nets, and demonstrate that the application of ultrashort laser pulses leads to sub-picoscond magnetization dynamics and all-optical switching in a similar manner as in ferrimagnetic alloys. Moreover, we present the essential material properties for successful laser-induced switching, demonstrating the feasibility of using a synthetic ferrimagnet as a high density magnetic storage element without the need of a write field.

cond-mat.mtrl-sci↗

arXiv2014

Higher order exchange interactions leading to metamagnetism in FeRh

The origin of the metamagnetic antiferromagnetic-ferromagnetic phase transition of FeRh is a subject of much debate. Competing explanations invoke magnetovolume effects and purely ther- modynamic transitions within the spin system. It is experimentally difficult to observe the changes in the magnetic system and the lattice simultaneously, leading to differing conclusions over which mechanism is responsible for the phase transition. A non-collinear electronic structure study by Mryasov [O.N. Mryasov, Phase Transitions 78, 197 (2005)] showed that non-linear behavior of the Rh moment leads to higher order exchange terms in FeRh. Using atomistic spin dynamics (ASD) we demonstrate that the phase transition can occur due to the competition between bilinear and the higher order four spin exchange terms in an effective spin Hamiltonian. The phase transition we see is of first order and shows thermal hysteresis in agreement with experimental observations. Simulating sub-picosecond laser heating we show an agreement with pump-probe experiments with a ferromagnetic response on a picosecond timescale.

cond-mat.mtrl-sci↗

arXiv2013

Atomistic spin model simulations of magnetic nanomaterials

Atomistic modelling of magnetic materials provides unprecedented detail about the underlying physical processes that govern their macroscopic properties, and allows the simulation of complex effects such as surface anisotropy, ultrafast laser-induced spin dynamics, exchange bias, and mi- crostructural effects. Here we present the key methods used in atomistic spin models which are then applied to a range of magnetic problems. We detail the parallelisation strategies used which enable the routine simulation of extended systems with full atomistic resolution.

cond-mat.mtrl-sci↗