Abstract:
Disclosed herein is a magnetostatic wave device that employs a single-crystal thin film of the formula Y.sub.3-x M.sub.x Fe.sub.5-y N.sub.Y O.sub.12 (where M denotes at least one member selected from La, Bi, Lu, and Gd, N denotes at least one member selected from Al, In, and Sc, and x and y are defined as 0
Abstract:
A mixtureand method are disclosed for growing bismuth lutetium iron garnet crystals via liquid phase epitaxy on a gadolinium gallium garnet (GGG) substrate wherein the crystals exhibit a relatively high Faraday rotation and an improved optical absorption.
Abstract:
In the LPE growth of magnetic bubble domain garnets from a melt the overall dependence of the saturation magnetization on the growth temperature can be adjusted to make the bubble domain collapse field independent of the growth temperature. In the melts, from which these garnets are grown, two types of non-magnetic ions are substituted for the iron ions, each of which ions, if substituted alone, would result in garnet materials having opposite dependence of the saturation magnetization on the growth temperature.
Abstract:
A METHOD FOR PRODUCING A BUBBLE DOMAIN IN AMAGNETIC SINGLE CRYSTLA GARNET FILM-SUBSTRATE STRUCTURE IS DISCLOSED. THE METHOD INVOLVES THE EPTIAXIAL DEPOSITION OF AN IRON GARNET FILM OF THE PROPER ORIENTATION AND HAVING A NEGATIVE MAGNETOSTRICTION CONSTANT ON A GARNET SUBSTRATE IN WHICH THE ROOM TEMPERATURE LATTICE CONTHE FILM IS LARGER THAN THE ROOM TEMPERATURE LATTICE CONSTANT OF THE SUBSTRATE BY AN AMOUNT GREATER THAN ABOUT 0.035 ANGATROM.
Abstract:
A novel rare earth-based oxide garnet single crystal suitable as a material of the elements in a magneto-optical device to exhibit a greatly decreased light absorption loss is proposed, which is prepared by the liquid epitaxial growth method on a oxide garnet single crystal wafer and having a chemical composition represented by the general formulaGd.sub.a Ho.sub.b Eu.sub.d Bi.sub.3-a-b-d Fe.sub.5-c M.sub.c O.sub.12,in which M is an element or a combination of elements selected from the group consisting of aluminum, scandium, gallium and indium, the subscript a is a positive number in the range from 1.1 to 2.1, the subscript b is a positive number in the range from 0.1 to 0.9, the subscript c is 0 or a positive number not exceeding 0.5 and the subscript d is zero or a positive number not exceeding 0.6 or, in particular, in the range from 0.03 to 0.6 with the proviso that 3-a-b-d is in the range from 0.7 to 1.2.
Abstract:
A method for preparing an oriented and textured magnetic compound, comprising the steps of preparing a composition at a temperature such that it comprises crystallites of the compound in the presence of a liquid; subjecting the composition to a magnetic force producing crystallite sedimentation; cooling down the composition in the presence of a magnetic force while applying a suitable temperature gradient for improving the development of a desired texture in the sedimentation area.
Abstract:
A single crystal film of a hexagonal ferrite is deposited on a nonmagnetic, single crystal substrate with a film of a second ferrite material interposed between the substrate and the hexagonal ferrite film. In a preferred embodiment, the substrate is of nonmagnetic spinel and the second ferrite material is a spinel ferrite.
Abstract:
Herein disclosed is a magnetic garnet film for a magnetic bubble element, in which the temperature changing rate of a bubble collapse field is reduced by Gd and Ga and in which the operating characteristics of the bubbles are improved by La and Lu. The temperature coefficient of the bubble collapse field is -0.24 to 0%/.degree. C., and the operating characteristics are remarkably excellent, therefore, this garnet film is suitable for the small bubbles with a diameter smaller than or equal to 1 .mu.m.
Abstract:
Magnetic devices exemplified by bubble devices depend upon functional magnetic layers initially produced by epitaxy and reduced to effectively thinned surface layers by ion implantation. Implantation is at well-defined energy spectral levels which minimize effect on surface layers and which predominantly affect a "buried layer". As a result, such affected layer acts as a boundary layer of a functional layer which is spaced away from an interface between a substrate and a deposited layer.Commercial significance is primarily concerned with high bit density devices in which effectively thinned regions are less than 3 micrometers in thickness.