Auxiliary DC field coil for improving rate bias instability of magnetic resonance gyroscopes

Claim 2

In a magnetic resonance gyro having first and second field generators, first and second detectors, first and second analyzers, a pumping lamp, first and second mirrors, first and second polarizers, a plasma containing readout lamp and first and second absorption cells for receiving light generated by the lamp, the gyro also having apparatus comprising: a first coil located adjacent an absorption cell for generating a DC H o field through the cell; and a second coil located in spaced proximate relation to the first coil for completing an inhomogeneous H o field in the cell, and driven with sufficient current wherein rate bias instability due to lamp translation effects is substantially compensated.

Claim 3

The subject matter set forth in claim 1 wherein said apparatus includes third and fourth coils which are respectively located adjacent the first and second coils, the third and fourth coils having a current driver and being series connected to generate a uniform H o field therebetween, the first and second coils having a current driver and being series connected in opposition to each other wherein the field generated by the third coil is in the same direction as that of the first coil and further wherein the field of the fourth coil is in opposition to the field of the second coil.

Claim 4

The subject matter set forth in claim 1 wherein said apparatus includes first and second DC current driving means for enabling each coil to operate with different current levels and includes a shielded cover enclosing said coils.

Claim 5

In a magnetic resonance gyroscope having first and second field generators, first and second detectors, first and second analyzers, a pumping lamp, first and second mirrors, first and second polarizers, the apparatus comprising: a plasma readout lamp for generating a beam; first and second absorption cells; and means generating an inhomogeneous H o DC field through at least one of the cells of such magnitude as to substantially compensate for rate bias instability due to readout lamp plasma shifts.

Claim 6

In a magnetic resonance gyroscope having first and second field generators, first and second detectors, first and second analyzers, a pumping lamp, first and second mirrors, first and second polarizers, the apparatus comprising: a plasma readout lamp for generating a beam; first and second absorption cells; and means generating an inhomogeneous H o DC field through at least one of the cells of such magnitude as to substantially compensate for rate bias instability due to readout lamp plasma shifts.

Claim 7

The subject matter set forth in claim 4 wherein the generating means comprises: a first coil located adjacent an absorption cell for generating a DC H o field through the cell; and a second coil located in spaced proximate relation to the first coil for completing an inhomogeneous H o field in the cell.

Claim 8

The subject matter set forth in claim 5 wherein third and fourth coils are respectively located adjacent the first and second coils, the third and fourth coils being series connected to generate a uniform H o field therebetween, the first and second coils being series connected in opposition to each other wherein the field generated by the third coil is in the same direction as that of the first and further wherein the field of the fourth coil is in opposition to the field of the second coil.

Claim 9

The subject matter set forth in claim 5 together with first and second DC current driving means for enabling each coil to operate with different current levels.

Claim 10

In a magnetic resonance gyroscope having first and second field generators, first and second detectors, first and second analyzers, a pumping lamp, first and second mirrors, first and second polarizers, a plasma filled readout lamp and first and second Hg isotope absorption cells, the gyroscope also having a coil assembly positioned adjacent at least one cell for generating an inhomogeneous H o field through the cells for reducing the rate bias instability due to lamp plasma shifts, wherein ##EQU4## is substantially equal to ##EQU5## where subscripts 1, 2 are labels for two mercury isotopes in the absorption cells; subscripts A, B are corresponding labels for the absorption cells; γ 1 and γ 2 are the absolute magnitudes of the gyromagnetic ratios for the two mercury isotopes in the absorption cells; and τ ij is the transverse relaxation time for isotope i (i=1, 2) in absorption cell j (j=A, B).

Claim 11

In a magnetic resonance gyroscope having first and second field generators, first and second detectors, first and second analyzers, a pumping lamp, first and second mirrors, first and second polarizers, a plasma filled readout lamp and first and second Hg isotope absorption cells, the gyroscope also having a coil assembly positioned adjacent at least one cell for generating an inhomogeneous H o field through the cells for reducing the rate bias instability due to lamp plasma shifts, wherein ##EQU4## is substantially equal to ##EQU5## where subscripts 1, 2 are labels for two mercury isotopes in the absorption cells; subscripts A, B are corresponding labels for the absorption cells; γ 1 and γ 2 are the absolute magnitudes of the gyromagnetic ratios for the two mercury isotopes in the absorption cells; and τ ij is the transverse relaxation time for isotope i (i=1, 2) in absorption cell j (j=A, B).

Claim 12

In a magnetic resonance gyroscope having first and second field generators, first and second detectors, first and second analyzers, a pumping lamp, first and second mirrors, first and second polarizers, a plasma filled readout lamp, first and second absorption cells, and experiencing rate bias instability due to lamp plasma shifts, a method for reducing said instability including the step of generating an inhomogeneous H o field across an absorption cell of the gyro wherein ##EQU6## is substantially equal to ##EQU7## where subscripts 1, 2 are labels for two mercury isotopes in the absorption cells; subscripts A, B are corresponding labels for the absorption cells; γ 1 and γ 2 are the absolute magnitudes of the gyromagnetic ratios for the two mercury isotopes in the absorption cells; and τ ij is the transverse relaxation time for isotope i (i=1, 2) in absorption cell j (j=A, B).

Claim 13

In a magnetic resonance gyroscope having first and second field generators, first and second detectors, first and second analyzers, a pumping lamp, first and second mirrors, first and second polarizers, a plasma filled readout lamp, first and second absorption cells, and experiencing rate bias instability due to lamp plasma shifts, a method for reducing said instability including the step of generating an inhomogeneous H o field across an absorption cell of the gyro wherein ##EQU6## is substantially equal to ##EQU7## where subscripts 1, 2 are labels for two mercury isotopes in the absorption cells; subscripts A, B are corresponding labels for the absorption cells; γ 1 and γ 2 are the absolute magnitudes of the gyromagnetic ratios for the two mercury isotopes in the absorption cells; and τ ij is the transverse relaxation time for isotope i (i=1, 2) in absorption cell j (j=A, B).

Claim 14

In a magnetic resonance gyroscope having first and second field generators, first and second detectors, first and second analyzers, a pumping lamp, first and second mirrors, first and second polarizers, at least two absorption cells and a plasma filled readout lamp, a method for reducing rate bias instability due to plasma shifts including the step of producing a predetermined temperature differential between the cells.

Claim 15

In a magnetic resonance gyroscope having first and second field generators, first and second detectors, first and second analyzers, a pumping lamp, first and second mirrors, first and second polarizers, at least two absorption cells and a plasma filled readout lamp, a method for reducing rate bias instability due to plasma shifts including the step of producing a predetermined temperature differential between the cells.