The magnetization profile and the related magnetic small-angle neutron scattering cross section of a single spherical nanoparticle with Néel surface anisotropy is analytically investigated. We employ a Hamiltonian that comprises the isotropic exchange interaction, an external magnetic field, a uniaxial magnetocrystalline anisotropy in the core of the particle, and the Néel anisotropy at the surface.Using a perturbation approach, the determination of the magnetization profile can be reduced to a Helmholtz equation with Neumann boundary condition, whose solution is represented by an infinite series in terms of spherical harmonics and spherical Bessel functions. From the resulting infinite series expansion, we analytically calculate the Fourier transform, which is algebraically related to the magnetic small-angle neutron scattering cross section. The approximate analytical solution is compared to the numerical solution using the Landau-Lifshitz equation, which accounts for the full nonlinearity of the problem.
I. INTRODUCTIONMagnetic small-angle neutron scattering (SANS) is a powerful technique for investigating spin structures on the mesoscopic length scale (∼ 1−100 nm) and inside the volume of magnetic materials [1,2]. Recent SANS studies on magnetic nanoparticles, in particular employing spin-polarized neutrons, unanimously demonstrate that their spin textures are highly complex and exhibit a variety of nonuniform, canted, or core-shell-type configurations (see, e.g. Refs. [3][4][5][6][7][8][9][10][11][12][13][14][15] and references therein). The magnetic SANS data analysis largely relies on structural form-factor-models for the cross section, borrowed from nuclear SANS, which do not properly account for the existing spin inhomogeneity inside magnetic nanoparticles or nanomagnets (NM).Progress in magnetic SANS theory [16][17][18][19][20][21][22][23][24][25] strongly suggests that for the analysis of experimental magnetic SANS data the spatial nanometer scale variation of the orientation and magnitude of the magnetization vector field must be taken into account, and that macrospinbased models-assuming a uniform magnetization-are not adequate. The starting point for a proper analysis of the scattering problem is a micromagnetic continuum expression for