Northrop Corporation

V Warren Biricik

John W Tully

James M Rowe

Paul Kraatz

Frank R Nakatsukasa

Michael S Perlmutter

Wah L Lim

Henry T Minden

Rudolph W Modster

Harley A Perkins

Samuel J Holmes

Wesley J Thompson

Joseph M Bresman

Methods are disclosed for making semiconductor windows which are transparent to light in the infrared range which have good electrical conductivity and are formed of a substrate material (11) having a semiconductor coating (14) having a dopant included therein. The coating is diffused, grown or deposited on one surface of the substrate and is controlled to obtain both low electrical resistivity and high infrared transmissivity. The coating can be formed of the same material as the substrate or can be a different material. Windows having particular thermal properties are formed utilizing zinc selenide and zinc sulfide as the substrate.

Method of manufacture of optically transparent electrically conductive

A laser gyroscope is formed as a sealed, unitary assembly of mirrors optically contacted to a monolithic gyro block without any means, such as Brewster windows, for isolating the laser plasma from any of the mirrors. The mirrors are fabricated with hard multilayer dielectric films which can withstand plasma exposure. A magnetic mirror utilizing the transverse Kerr effect to separate the frequencies of counter-propagating beams, and to avoid lock-in, includes a Ni-Fe alloy layer over which is directly deposited a thin iron or iron alloy layer to form a rotationally switchable Kerr effect combination. The magnetic field for switching is generated by an electric current developed in two pairs of orthogonally disposed wires embedded in the substrate immediately below the iron and Ni-Fe alloy layers. A specially designed multilayer dielectric stack is disposed on one of the mirrors, for example over the iron and Ni-Fe alloy layers on the magnetic mirror, and is configured to suppress S mode oscillation in order to limit the gyro to P mode operation.

Ring laser gyro and magnetic mirror therefor

A semiconductor window which is transparent to light in the infrared range and which has good electrical conductivity is formed of a substrate material having a semiconductor coating having a dopant included therein. The coating is diffused, grown or deposited on one surface of the substrate and is controlled to obtain both low electrical resistivity and high infrared transmissivity. The coating can be formed of the same material as the substrate or can be a different material. Windows having particular thermal properties are formed utilizing zinc selenide and zinc sulfide as the substrate.

Optically transparent electrically conductive semiconductor windows

Method and apparatus for high accuracy measurement of non-reciprocal reflectivity of magnetic thin film materials and magnetic mirrors. An ellipsometer which employs a Helmholtz coil to supply magneto-optic modulation to p-polarized light and an acousto-optic modulator to provide intensity modulation is utilized in conjunction with a novel scheme of analyzer rotation and computational techniques to accurately measure non-reciprocal reflectivity. A microcomputer is used to provide controlled rotation of polarizing elements, data logging, data analysis, and output. The non-reciprocal reflectivity value is determined by the slope of the measured ratio of magneto-optically modulated and absolute intensities (.delta.I.sub.magnetic /I.sub.total), plotted against a function of the analyzer angle G(.PSI.).

Method and apparatus for measuring non-reciprocal loss of thin magnetic

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Rancho Palos Verdes, CA, United States of America

V Warren Biricik