Magnetization reversal in melt-quenched NdFeB

Melt-quenched NdFeB is an important modern permanent magnet material. However there still remains doubt as to the magnetization reversal mechanism which controls coercivity in material prepared by this processing route. To investigate this problem a new technique based on measurements of reversible magnetization along recoil curves has been used. The technique identifies the presence of free domain walls during magnetic reversal. For this study samples of isotropic (MQI), hot pressed (MQII) and die upset (MQIII) melt-quenched NdFeB were examined. The results indicate that in MQI free domain walls are not present during reversal and the reversal mechanism is most likely incoherent rotation of some form. Free domain walls are also not present during reversal in the majority of grains of MQII, even though initial magnetization measurements indicate that the grain size is large enough to support them. In MQIII free domain walls are present during reversal. These results are attributed to the reduced domain wall nucleation field in MQIII compared with MQII and the increased dipolar interactions in MQIII

Magnetization reversal in melt-quenched NdFeB

Melt-quenched NdFeB is an important modern permanent magnet material. However, there still remains doubt as to the magnetization reversal mechanism which controls coercivity in material prepared by this processing route. To investigate this problem a new technique based on measurements of reversible magnetization along recoil curves has been used. The technique identifies the presence of free domain walls during magnetic reversal. For this study samples of isotropic (MQI), hot pressed (MQII) and die upset (MQIII) melt-quenched NdFeB were examined. The results indicate that in MQI free domain walls are not present during reversal and the reversal mechanism is most likely incoherent rotation of some form. Free domain walls are also not present during reversal in the majority of grains of MQII, even though initial magnetization measurements indicate that the grain size is large enough to support them. In MQIII free domain walls are present during reversal. These results are attributed to the reduced domain wall nucleation field in MQIII compared with MQII and the increased dipolar interactions in MQIII

Spin wave valve in an exchange spring bilayer

Spin wave resonances are calculated for two exchange coupled ferromagnetic films with different magnetic anisotropies. In this structure a domain wall can be pinned near the interface and affect spin wave frequencies. We find that the exchange spring can decrease the decay length of excitations at the interface by enhancing the frequency mismatch between the two films. We also propose the function of such a structure as a spin wave “valve.” Dipolar contributions to the spin wave energies are estimated using a method adapted from an effective medium approximation in the magnetostatic limit

Interpretation of magnetisation dynamics using inductive magnetometry in thin films

We present ferromagnetic resonance data from a Py film using both a pulsed inductive microwave magnetometer (PIMM) and conventional FMR. An increase in the damping is seen at low field resonances in the PIMM data from what is expected using conventional FMR. This is explained by the influence of the PIMM’s spatially inhomogeneous excitation field and quantified using an intuitive argument. We demonstrate from this derivation how excitation of non-uniform wavevectors can explain the measured increase in damping at low fields observed by the PIMM. We also present results from a coupled Py and Cobalt system, demonstrating that inductive magnetometry can be a sensitive technique for measuring exchange coupling over interfaces and surfaces

Spin wave excitations in exchange spring Co/CoPt thin film bilayers

10.1016/j.jmmm.2004.04.061Journal of Magnetism and Magnetic Materials272-276I273-274JMMM

Light scattering from spin wave excitations in a Co/CoPt exchange spring

10.1016/j.jmmm.2004.11.519Journal of Magnetism and Magnetic Materials290-291 PART 1530-532JMMM