Abstract An optically pumped magnetic resonance gyroscope wherein the direction of the magnetic fields intersecting the absorption cells of two interconnected spin generators may be oriented in the same or opposite directions, but are of unequal magnitude. The output from each spin generator comprises signals having frequencies characteristic of the two isotopes contained in the cell of each spin generator. These signals are applied to filter circuits each of which passes a desired frequency. Two signals are multiplied in frequency. A pair of phase difference sensors measure differences in phase between pairs of filter outputs, and controls the spin generators in such a manner as to return a first function of the phase differences to null. The output signal from the instrument, derived from a second function of the phase differences, represents the angular rotation of the gyro about a predetermined axis.
A nuclear magnetic resonance gyroscope which derives rotational information from the phases of precessing nuclear magnetic moments of mercury absorption cells for determining the angle of rotation of the gyroscope about a predetermined axis comprising: means for producing at least two unidirectional magnetic fields of differeing magnitudes said fields being oriented in the same direction, first and second absorption cells containing material for producing nuclear magnetic resonance signal in each cell said first and second cells being intersected by said unidirectioal magnetic fields, optical means for increasing the magnitude of the net magnetic moment of said first and second absorption cells, means for detecting the phase of output signals from said first and second absorption cells, and means for combining said detected phases to produce an output from said gyroscope indicative of the rotation of said gyroscope about said predetermined axis.
Claim 2
Dependent Claim
141 words
A nuclear magnetic resonance gyroscope which derives rotational information from the phases of precessing nuclear magnetic moments of mercury absorption cells for determining the angle of rotation of the gyroscope about a predetermined axis comprising: means for producing at least two unidirectional magnetic fields of differeing magnitudes said fields being oriented in the same direction, first and second absorption cells containing material for producing nuclear magnetic resonance signal in each cell said first and second cells being intersected by said unidirectioal magnetic fields, optical means for increasing the magnitude of the net magnetic moment of said first and second absorption cells, means for detecting the phase of output signals from said first and second absorption cells, and means for combining said detected phases to produce an output from said gyroscope indicative of the rotation of said gyroscope about said predetermined axis.
Claim 3
Dependent Claim
66 words
The nuclear gyroscope of claim 1 comprising: first and second readout lamps intersecting said first and second absorption cells, first and second photodetector means for detecting signals from said absorption cells, first and second alternating current coils for maintaining the magnetic resonance oscillation of said gyroscope, and a common amplifier to said first and second photodetector means for amplifying signals applied to said alternating current coils.