Micromagnetics

Micromagnetics is a field of physics dealing with the prediction of magnetic behaviors at sub-micrometer length scales. The length scales considered are large enough for the atomic structure of the material to be ignored (the continuum approximation), yet small enough to resolve magnetic structures such as domain walls or vortices.

Micromagnetics can deal with static equilibria, by minimizing the magnetic energy, and with dynamic behavior, by solving the time-dependent dynamical equation.

History

Micromagnetics originated from a 1935 paper by Lev Landau and Evgeny Lifshitz on antidomain walls. Micromagnetics was then expanded upon by William Fuller Brown Jr. in several works in 1940-1941 using energy expressions taken from a 1938 paper by William Cronk Elmore. According to D. Wei, Brown introduced the name "micromagnetics" in 1958. The field prior to 1960 was summarised in Brown's book Micromagnetics. In the 1970's computational methods were developed for the analysis of recording media due to the introduction of personal computers.

Static micromagnetics

The purpose of static micromagnetics is to solve for the spatial distribution of the magnetization $\mathbf {M}$ at equilibrium. In most cases, as the temperature is much lower than the Curie temperature of the material considered, the modulus $|\mathbf {M} |$ of the magnetization is assumed to be everywhere equal to the saturation magnetization $M_{s}$. The problem then consists in finding the spatial orientation of the magnetization, which is given by the magnetization direction vector $\mathbf {m} =\mathbf {M} /M_{s}$, also called reduced magnetization.

The static equilibria are found by minimizing the magnetic energy,

$E=E_{\text{exch}} E_{\text{anis}} E_{\text{Z}} E_{\text{demag}} E_{\text{DMI}} E_{\text{m-e}},$

subject to the constraint $|\mathbf {M} |=M_{s}$ or $|\mathbf {m} |=1$.

The contributions to this energy are the following:

Exchange energy

The exchange energy is a phenomenological continuum description of the quantum-mechanical exchange interaction. It is written as:

$E_{\text{exch}}=A\int _{V}\left((\nabla m_{x})^{2} (\nabla m_{y})^{2} (\nabla m_{z})^{2}\right)\mathrm {d} V$

where $A$ is the exchange constant; $m_{x}$, $m_{y}$ and $m_{z}$ are the components of $\mathbf {m}$; and the integral is performed over the volume of the sample.

The exchange energy tends to favor configurations where the magnetization varies slowly across the sample. This energy is minimized when the magnetization is perfectly uniform. The exchange term is isotropic, so any direction is equally acceptable.

Anisotropy energy

Main articles: Magnetic anisotropy, Anisotropy energy, and Magnetocrystalline anisotropy

Magnetic anisotropy arises due to a combination of crystal structure and spin-orbit interaction. It can be generally written as:

$E_{\text{anis}}=\int _{V}F_{\text{anis}}(\mathbf {m} )\mathrm {d} V$

where $F_{\text{anis}}$, the anisotropy energy density, is a function of the orientation of the magnetization. Minimum-energy directions for $F_{\text{anis}}$ are called easy axes.

Time-reversal symmetry ensures that $F_{\text{anis}}$ is an even function of $\mathbf {m}$. The simplest such function is

$F_{\text{anis}}(\mathbf {m} )=-K_{1}m_{z}^{2},$

where K₁ is called the anisotropy constant. In this approximation, called uniaxial anisotropy, the easy axis is the $z$ axis.

The anisotropy energy favors magnetic configurations where the magnetization is everywhere aligned along an easy axis.

Zeeman energy

Main article: Zeeman energy

The Zeeman energy is the interaction energy between the magnetization and any externally applied field. It is written as:

$E_{\text{Z}}=-\mu _{0}\int _{V}\mathbf {M} \cdot \mathbf {H} _{\text{a}}\mathrm {d} V$

where $\mathbf {H} _{\text{a}}$ is the applied field and $\mu _{0}$ is the vacuum permeability.

The Zeeman energy favors alignment of the magnetization parallel to the applied field.

Energy of the demagnetizing field

Example of micromagnetic configuration. Compared to a uniform state, the flux closure structure lowers the energy of the demagnetizing field, at the expense of some exchange energy.

Main article: Demagnetizing field

The demagnetizing field is the magnetic field created by the magnetic sample upon itself. The associated energy is:

$E_{\text{demag}}=-{\frac {\mu _{0}}{2}}\int _{V}\mathbf {M} \cdot \mathbf {H} _{\text{d}}\mathrm {d} V$

where $\mathbf {H} _{\text{d}}$ is the demagnetizing field. The field satisfies

$\nabla \times \mathbf {H} _{\text{d}}=0$

and hence can be written as the gradient of a potential $\mathbf {H} _{\text{d}}=-\nabla U$. This field depends on the magnetic configuration itself, and it can be found by solving

$\nabla ^{2}U_{\text{in}}=\nabla \cdot \mathbf {M}$

inside of the body and

$\nabla ^{2}U_{\text{out}}=0$

outside of the body. These are supplemented with the boundary conditions on the surface of the body

$U_{\text{out}}=U_{\text{in}},\quad {\frac {\partial U_{\text{in}}}{\partial \mathbf {n} }}-{\frac {\partial U_{\text{out}}}{\partial \mathbf {n} }}=\mathbf {M} \cdot \mathbf {n}$

where $\mathbf {n}$ is the unit normal to the surface. Furthermore, the potential satisfies the condition that $|rU|$ and $|r^{2}\nabla U|$ remain bounded as $r\to \infty$. The solution of these equations (c.f. magnetostatics) is:

$U(\mathbf {r} )={\frac {1}{4\pi }}\left(-\int _{V}{\frac {\nabla '\cdot \mathbf {M} (\mathbf {r} ')}{|\mathbf {r} -\mathbf {r} '|}}\mathrm {d} V \int _{\partial V}{\frac {\mathbf {n} \cdot \mathbf {M} (\mathbf {r} ')}{|\mathbf {r} -\mathbf {r} '|}}\mathrm {d} S\right).$

The quantity $-\nabla \cdot \mathbf {M}$ is often called the volume charge density, and $\mathbf {M} \cdot \mathbf {n}$ is called the surface charge density. The energy of the demagnetizing field favors magnetic configurations that minimize magnetic charges. In particular, on the edges of the sample, the magnetization tends to run parallel to the surface. In most cases it is not possible to minimize this energy term at the same time as the others. The static equilibrium then is a compromise that minimizes the total magnetic energy, although it may not minimize individually any particular term.

Dzyaloshinskii–Moriya Interaction Energy

Main article: Antisymmetric exchange

This interaction arises when a crystal lacks inversion symmetry, encouraging the magnetization to be perpendicular to its neighbours. It directly competes with the exchange energy. It is modelled with the energy contribution

$$E_{\text{DMI}}=\int _{V}\mathbf {D} :(\nabla \mathbf {m} \times \mathbf {m} )$$

where $\mathbf {D}$ is the spiralization tensor, that depends upon the crystal class. For bulk DMI,

$E_{\text{DMI}}=\int _{V}D\mathbf {m} \cdot (\nabla \times \mathbf {m} ),$

and for a thin film in the $x-y$ plane interfacial DMI takes the form

$E_{\text{DMI}}=\int _{V}D(\mathbf {m} \cdot \nabla m_{z}-m_{z}\nabla \cdot \mathbf {m} ),$

and for materials with symmetry class $D_{2d}$ the energy contribution is

$E_{\text{DMI}}=\int _{V}D\mathbf {m} \cdot \left({\frac {\partial \mathbf {m} }{\partial x}}\times {\hat {x}}-{\frac {\partial \mathbf {m} }{\partial y}}\times {\hat {y}}\right).$

This term is important for the formation of magnetic skyrmions.

Magnetoelastic Energy

The magnetoelastic energy describes the energy storage due to elastic lattice distortions. It may be neglected if magnetoelastic coupled effects are neglected. There exists a preferred local distortion of the crystalline solid associated with the magnetization director $\mathbf {m}$. For a simple small-strain model, one can assume this strain to be isochoric and fully isotropic in the lateral direction, yielding the deviatoric ansatz $$\mathbf {\varepsilon } _{0}(\mathbf {m} )={\frac {3}{2}}\lambda _{\text{s}}\,\left[\mathbf {m} \otimes \mathbf {m} -{\frac {1}{3}}\mathbf {1} \right]$$ where the material parameter $\lambda _{\text{s}}$ is the isotropic magnetostrictive constant. The elastic energy density is assumed to be a function of the elastic, stress-producing strains $\mathbf {\varepsilon } _{e}:=\mathbf {\varepsilon } -\mathbf {\varepsilon } _{0}$. A quadratic form for the magnetoelastic energy is $$E_{\text{m-e}}={\frac {1}{2}}\int _{V}[\mathbf {\varepsilon } -\mathbf {\varepsilon } _{0}(\mathbf {m} )]:\mathbb {C} :[\mathbf {\varepsilon } -\mathbf {\varepsilon } _{0}(\mathbf {m} )]$$ where $\mathbb {C} :=\lambda \mathbf {1} \otimes \mathbf {1} 2\mu \mathbb {I}$ is the fourth-order elasticity tensor. Here the elastic response is assumed to be isotropic (based on the two Lamé constants $\lambda$ and $\mu$). Taking into account the constant length of $\mathbf {m}$, we obtain the invariant-based representation $$E_{\text{m-e}}=\int _{V}{\frac {\lambda }{2}}{\mbox{tr}}^{2}[\mathbf {\varepsilon } ] \mu \,{\mbox{tr}}[\mathbf {\varepsilon } ^{2}]-3\mu E{\big \{}{\mbox{tr}}[\mathbf {\varepsilon } (\mathbf {m} \otimes \mathbf {m} )]-{\frac {1}{3}}{\mbox{tr}}[\mathbf {\varepsilon } ]{\big \}}.$$

This energy term contributes to magnetostriction.

Dynamic micromagnetics

The purpose of dynamic micromagnetics is to predict the time evolution of the magnetic configuration. This is especially important if the sample is subject to some non-steady conditions such as the application of a field pulse or an AC field. This is done by solving the Landau-Lifshitz-Gilbert equation, which is a partial differential equation describing the evolution of the magnetization in terms of the local effective field acting on it.

Effective field

The effective field is the local field felt by the magnetization. The only real fields however are the magnetostatic field and the applied field. It can be described informally as the derivative of the magnetic energy density with respect to the orientation of the magnetization, as in:

$\mathbf {H} _{\mathrm {eff} }=-{\frac {1}{\mu _{0}M_{s}}}{\frac {\mathrm {d} ^{2}E}{\mathrm {d} \mathbf {m} \mathrm {d} V}}$

where dE/dV is the energy density. In variational terms, a change dm of the magnetization and the associated change dE of the magnetic energy are related by:

$\mathrm {d} E=-\mu _{0}M_{s}\int _{V}(\mathrm {d} \mathbf {m} )\cdot \mathbf {H} _{\text{eff}}\,\mathrm {d} V$

Since m is a unit vector, dm is always perpendicular to m. Then the above definition leaves unspecified the component of H_eff that is parallel to m. This is usually not a problem, as this component has no effect on the magnetization dynamics.

From the expression of the different contributions to the magnetic energy, the effective field can be found to be (excluding the DMI and magnetoelastic contributions):

$\mathbf {H} _{\mathrm {eff} }={\frac {2A}{\mu _{0}M_{s}}}\nabla ^{2}\mathbf {m} -{\frac {1}{\mu _{0}M_{s}}}{\frac {\partial F_{\text{anis}}}{\partial \mathbf {m} }} \mathbf {H} _{\text{a}} \mathbf {H} _{\text{d}}$

Landau-Lifshitz-Gilbert equation

The terms of the Landau-Lifshitz-Gilbert equation: precession (red) and damping (blue). The trajectory of the magnetization (dotted spiral) is drawn under the simplifying assumption that the effective field H_eff is constant.

Main article: Landau-Lifshitz-Gilbert equation

This is the equation of motion of the magnetization. It describes a Larmor precession of the magnetization around the effective field, with an additional damping term arising from the coupling of the magnetic system to the environment. The equation can be written in the so-called Gilbert form (or implicit form) as:

${\frac {\partial \mathbf {m} }{\partial t}}=-|\gamma |\mathbf {m} \times \mathbf {H} _{\mathrm {eff} } \alpha \mathbf {m} \times {\frac {\partial \mathbf {m} }{\partial t}}$

where $\gamma$ is the electron gyromagnetic ratio and $\alpha$ the Gilbert damping constant.

It can be shown that this is mathematically equivalent to the following Landau-Lifshitz (or explicit) form:

${\frac {\partial \mathbf {m} }{\partial t}}=-{\frac {|\gamma |}{1 \alpha ^{2}}}\mathbf {m} \times \mathbf {H} _{\mathrm {eff} }-{\frac {\alpha |\gamma |}{1 \alpha ^{2}}}\mathbf {m} \times (\mathbf {m} \times \mathbf {H} _{\text{eff}}),$

where $\alpha$ is the Gilbert Damping constant, characterizing how quickly the damping term takes away energy from the system ($\alpha$ = 0, no damping, permanent precession). These equations preserve the constraint $|\mathbf {m} |=1$, as

${\frac {\mathrm {d} }{\mathrm {d} t}}|\mathbf {m} |^{2}=2\mathbf {m} \cdot {\frac {\partial \mathbf {m} }{\partial t}}=0.$

Applications

The interaction of micromagnetics with mechanics is also of interest in the context of industrial applications that deal with magneto-acoustic resonance such as in hypersound speakers, high frequency magnetostrictive transducers etc. FEM simulations taking into account the effect of magnetostriction into micromagnetics are of importance. Such simulations use models described above within a finite element framework.

Apart from conventional magnetic domains and domain-walls, the theory also treats the statics and dynamics of topological line and point configurations, e.g. magnetic vortex and antivortex states; or even 3d-Bloch points, where, for example, the magnetization leads radially into all directions from the origin, or into topologically equivalent configurations. Thus in space, and also in time, nano- (and even pico-)scales are used.

The corresponding topological quantum numbers are thought to be used as information carriers, to apply the most recent, and already studied, propositions in information technology.

Another application that has emerged in the last decade is the application of micromagnetics towards neuronal stimulation. In this discipline, numerical methods such as finite-element analysis are used to analyze the electric/magnetic fields generated by the stimulation apparatus; then the results are validated or explored further using in-vivo or in-vitro neuronal stimulation. Several distinct set of neurons have been studied using this methodology including retinal neurons, cochlear neurons, vestibular neurons, and cortical neurons of embryonic rats.

See also

• Magnetism
• Magnetic nanoparticles

Further reading

• Abert, Claas (2019). "Micromagnetics and spintronics: models and numerical methods (open access)". European Physical Journal B. 92 (6): 120. arXiv:1810.12365. Bibcode:2019EPJB...92..120A. doi:10.1140/epjb/e2019-90599-6.
• Brown, William Fuller Jr. (1978) [1963]. Micromagnetics. New York: Wiley. ISBN 978-0-88275-665-3.
• Gilbert, Thomas L. (2004). "A Phenomenological Theory of Damping in Ferromagnetic Materials". IEEE Transactions on Magnetics. 40 (6): 3443–3449. Bibcode:2004ITM....40.3443G. doi:10.1109/TMAG.2004.836740. ISSN 0018-9464. S2CID 35628797.
• Kruzik Martin, Prohl Andreas (2006). "Recent Developments in the Modeling, Analysis, and Numerics of Ferromagnetism". SIAM Review. 48 (3): 439–483. Bibcode:2006SIAMR..48..439K. doi:10.1137/S0036144504446187.
• Maugin, Gérard A. (1988). Continuum mechanics of electromagnetic solids. Amsterdam: North-Holland. ISBN 978-0444703996.
• Prohl, Andreas (2001). Computational micromagnetism (1. Aufl. ed.). Stuttgart: Teubner. ISBN 9783519003588.
• Tiersten, H. F. (1964). "Coupled Magnetomechanical Equations for Magnetically Saturated Insulators". Journal of Mathematical Physics. 5 (9): 1298–1318. Bibcode:1964JMP.....5.1298T. doi:10.1063/1.1704239.
• Mukesh, S. (2017). "Modeling intracochlear magnetic stimulation: a Finite-Element Analysis". IEEE Transactions on Neural Systems and Rehabilitation Engineering. 25 (8): 1353–1362. doi:10.1109/TNSRE.2016.2624275. PMC 5750049. PMID 27831887.

External links

• μMAG -- Micromagnetic Modeling Activity Group.
• OOMMF -- Micromagnetic Modeling Tool.
• MuMax -- GPU-accelerated Micromagnetic Modeling Tool.