Self biased ferrite resonators

Claim 1

A method for preparing an M-type, self-biased, hexagonal ferrite resonator composed of single crystals of barium hexaferrite on a spinel substrate which comprises the steps of: A. forming a homogenized, supersaturated melt composition by dissolving a solute composed of a mixture of Ba O, Fe 2 O 3 and ZnO into a molten flux composed of Ba CO 3 and B 2 O 3 in which the mole ratio of B a CO 3 : B 2 O 3 is 1.75, the mole ratio of Fe 2 O 3 : (B a CO 3 +B 2 O 3 ) is 0.164, and the mole ratio of Zn O: Fe 2 O 3 is 0.100; B. maintaining said melt composition at a temperature of from about 911° C. to 921° C. while simultaneously immersing a Mg (In, Ga) 2 O 4 spinel substrate into said melt composition for a period of time sufficient to effect the deposition on the surface of said substrate of barium hexaferrite single crystals that are substantially free of defects which can act as nucleation sites for magnetic domains; C. subjecting said single crystals to a magnetic field that is directed along the easy axis of anisotropy of said crystals and of sufficient magnitude to produce magnetic saturation in said crystals; and D. reducing said magnetic field to zero to produce single crystals capable of being maintained in a metastable state of magnetic saturation with zero applied field.

Claim 2

A method for preparing an M-type, self-biased, hexagonal ferrite resonator composed of single crystals of barium hexaferrite on a spinel substrate which comprises the steps of: A. forming a homogenized, supersaturated melt composition by dissolving a solute composed of a mixture of Ba O, Fe 2 O 3 and ZnO into a molten flux composed of Ba CO 3 and B 2 O 3 in which the mole ratio of B a CO 3 : B 2 O 3 is 1.75, the mole ratio of Fe 2 O 3 : (B a CO 3 +B 2 O 3 ) is 0.164, and the mole ratio of Zn O: Fe 2 O 3 is 0.100; B. maintaining said melt composition at a temperature of from about 911° C. to 921° C. while simultaneously immersing a Mg (In, Ga) 2 O 4 spinel substrate into said melt composition for a period of time sufficient to effect the deposition on the surface of said substrate of barium hexaferrite single crystals that are substantially free of defects which can act as nucleation sites for magnetic domains; C. subjecting said single crystals to a magnetic field that is directed along the easy axis of anisotropy of said crystals and of sufficient magnitude to produce magnetic saturation in said crystals; and D. reducing said magnetic field to zero to produce single crystals capable of being maintained in a metastable state of magnetic saturation with zero applied field.