Control of magnetostatic waves in thin films by means of spatially nonuniform bias fields

Although magnetostatic wave devices normally employ spatially uniform magnetic bias, control of important features of the modes is afforded through judicious use of dc field gradients. Such control can be the basis for new forms of microwave signal processors.Gradients in either the field magnitude, direction, or both can be employed to affect wave dispersion or mode spectra. This is done to control prespecified characteristics such as frequency, rf energy distribution, impedance, and the velocity of energy propagation.Very general mathematical analyses of both the forward volume wave and surface wave geometries are developed for cases where the effective magnetic bias has, depending upon the mode, transverse spatial variation along either the ferrite film width or thickness caused by the applied field, saturation magnetization, magnetic anisotropy — or some combination.Computer simulation has been used to obtain eigenfrequencies and eigenmodes when the bias is uniform or nonuniform. The latter cases reveal that a great deal of control over the mode energy distributions can be exercised by the proper choice of gradients. For example, a forward volume wave can be forced to have strong field-displacement characteristics that are either nearly reciprocal or very strongly nonreciprocal.

[1]  R. Damon,et al.  Magnetostatic modes of a ferromagnet slab , 1961 .

[2]  F. Morgenthaler Dynamic magnetoelastic coupling in ferromagnets and antiferromagnets , 1972 .

[3]  F. Morgenthaler,et al.  Localized high-Q ferromagnetic resonance in nonuniform magnetic fields , 1977 .

[4]  F. Morgenthaler Magnetostatic waves bound to a DC field gradient , 1977 .

[5]  F. Morgenthaler Bound magnetostatic waves controlled by field gradients in YIG single crystals and epitaxial films , 1978 .

[6]  Two‐dimensional magnetostatic resonances in a thin film disk containing a magnetic bubble , 1979 .

[7]  Magnetostatic waves in nonuniform bias fields including exchange effects , 1980 .

[8]  F. Morgenthaler Synthesis of Magnetostatic Waves and Modes Using Nonuniform Bias Fields , 1980 .

[9]  Magnetostatic surface modes in nonuniform thin films with in‐plane bias fields , 1981 .

[10]  Novel Devices Based upon Field Gradient Control of Magnetostatic Modes and Waves , 1982 .

[11]  F. Morgenthaler Nondispersive magnetostatic forward volume waves under field gradient control , 1982 .

[12]  Numerical solution of the integral equations for MSSW , 1982 .

[13]  F. Morgenthaler,et al.  Investigation of the velocity of energy circulation of magnetostatic modes in ferrites , 1983 .

[14]  D. Stancil,et al.  Guiding magnetostatic surface waves with nonuniform in‐plane fields , 1983 .

[15]  Field gradient control of magnetostatic waves for microwave signal processing applications , 1983 .

[16]  Daniel D. Stancil,et al.  A new microwave ring resonator using guided magnetostatic surface waves , 1984 .