Abstract An axial magnetic field applied to the laser gain medium of a laser gyro provides, through the Zeeman Effect, a pair of gain versus frequency profiles relating to respective counter-rotating waves (clockwise and counterclockwise) with their frequencies of maximum gain displaced from one another by an amount which is proportional to the applied magnetic field, and which is substantially equal to the frequency difference caused by an applied directional bias, such that the separation between the frequency of each wave and the frequency of maximum gain of the related gain profile is the same for both waves. This causes the counter-rotating waves to operate on points of equal phase (or index of refraction) on the corresponding dispersion characteristic curve associated with the related gain versus frequency profile. Under these conditions, even if the effective optical length of the gain medium changes in response, for example, to externally induced perturbations of the medium or of the resonant laser frequency, the change is essentially the same for each of the counter-rotating waves, and is thereby substantially cancelled when the wave frequencies are differenced to obtain a gyro output. For example, when cavity length drift causes increases or decreases in both frequencies, thereby causing the waves to intersect different portions of the related dispersion characteristic curve, which are typically not linear or stable, the pair of dispersion characteristics will have similar nonlinearity and instability, and errors resulting therefrom will be substantially cancelled.
A laser gyro comprising: a closed loop optical cavity including a plurality of mirrors defining an optical path; a laser gain medium disposed in said optical path, said laser gain medium having a gain versus frequency profile and a related dispersion profile having its zero point substantially at the frequency of maximum gain of the frequency versus gain profile with which it is associated; a directional bias means disposed in the optical path of said optical cavity for providing a directional bias resulting in a frequency difference between waves circulating in one direction in said optical cavity and waves circulating in the other direction in said optical cavity, said bias being equivalent to at least the largest angular rate to be sensed by said laser gyro; Zeeman Effect means providing a magnetic field within said laser gain medium oriented parallel to the waves circulating through said laser gain medium, said Zeeman Effect means providing two distinct gain versus frequency profiles in said laser gain medium, with two distinct corresponding dispersion profiles, said magnetic field having a magnitude to cause a frequency difference between the frequency of maximum gain of said two gain versus frequency profiles which is equal to the frequency difference between counter-rotating waves caused by said directional anisotropy means, the magnetic field of said Zeeman Effect means being related to the polarity of said directional anisotropy means so as to cause counter-rotating waves supported by each of said gain versus frequency profiles to be at substantially equal dispersion points on the related dispersion profiles; means for extracting the clockwise and counterclockwise waves from said cavity and for providing an output manifestation of angular rate of said laser gyro as a function of frequency difference between said clockwise and counterclockwise waves.
Claim 2
Dependent Claim
292 words
A laser gyro comprising: a closed loop optical cavity including a plurality of mirrors defining an optical path; a laser gain medium disposed in said optical path, said laser gain medium having a gain versus frequency profile and a related dispersion profile having its zero point substantially at the frequency of maximum gain of the frequency versus gain profile with which it is associated; a directional bias means disposed in the optical path of said optical cavity for providing a directional bias resulting in a frequency difference between waves circulating in one direction in said optical cavity and waves circulating in the other direction in said optical cavity, said bias being equivalent to at least the largest angular rate to be sensed by said laser gyro; Zeeman Effect means providing a magnetic field within said laser gain medium oriented parallel to the waves circulating through said laser gain medium, said Zeeman Effect means providing two distinct gain versus frequency profiles in said laser gain medium, with two distinct corresponding dispersion profiles, said magnetic field having a magnitude to cause a frequency difference between the frequency of maximum gain of said two gain versus frequency profiles which is equal to the frequency difference between counter-rotating waves caused by said directional anisotropy means, the magnetic field of said Zeeman Effect means being related to the polarity of said directional anisotropy means so as to cause counter-rotating waves supported by each of said gain versus frequency profiles to be at substantially equal dispersion points on the related dispersion profiles; means for extracting the clockwise and counterclockwise waves from said cavity and for providing an output manifestation of angular rate of said laser gyro as a function of frequency difference between said clockwise and counterclockwise waves.
Claim 3
Dependent Claim
142 words
A laser gyro according to claim 1, further comprising: a polarization anisotropy disposed in said optical path, wherein said optical cavity sustains laser oscillations in two different substantially mutually opposite polarizations at different frequencies, the difference in frequency between said mutually opposite polarizations being significantly greater than the frequency difference between counter-rotating waves created by said directional bias means, whereby the counter-rotating waves of one of said polarizations supported by each of said gain versus frequency profiles are at substantially equal dispersion points on the related dispersion profiles, and the counter-rotating waves of the other of said polarizations supported by each of said gain versus frequency profiles are at substantially equal dispersion points on the related dispersion profiles, the waves of one polarization being at different dispersion points on the related dispersion profiles than the waves of the other of said polarizations.