Polynomial model of the frequency characteristic of a slowly rotating vibrating laser gyro with differently amplified counterpropagating waves
Expressions are obtained for calculating the four first coefficients of a polynomial model of the frequency characteristic of a slowly rotating laser gyro on a vibration stage. The expressions are valid when the gyro operates at the gain line centre and currents in its arms are balanced, however, th...
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| Veröffentlicht in: | Quantum electronics (Woodbury, N.Y.) N.Y.), 2004-04, Vol.34 (4), p.388-392 |
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| container_end_page | 392 |
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| container_issue | 4 |
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| container_title | Quantum electronics (Woodbury, N.Y.) |
| container_volume | 34 |
| creator | Bondarenko, Evgenii A |
| description | Expressions are obtained for calculating the four first coefficients of a polynomial model of the frequency characteristic of a slowly rotating laser gyro on a vibration stage. The expressions are valid when the gyro operates at the gain line centre and currents in its arms are balanced, however, the amplifications of counterpropagating waves are slightly different due to slightly different Q factors of the resonator for these waves. Analysis of the expressions suggests that the difference in the amplification of counterpropagating waves of the laser gyro leads to the zero shift and produces the component of the output signal that does not commute with the angular velocity. (laser applications and other topics in quantum electronics) |
| doi_str_mv | 10.1070/QE2004v034n04ABEH002686 |
| format | Article |
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The expressions are valid when the gyro operates at the gain line centre and currents in its arms are balanced, however, the amplifications of counterpropagating waves are slightly different due to slightly different Q factors of the resonator for these waves. Analysis of the expressions suggests that the difference in the amplification of counterpropagating waves of the laser gyro leads to the zero shift and produces the component of the output signal that does not commute with the angular velocity. 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The expressions are valid when the gyro operates at the gain line centre and currents in its arms are balanced, however, the amplifications of counterpropagating waves are slightly different due to slightly different Q factors of the resonator for these waves. Analysis of the expressions suggests that the difference in the amplification of counterpropagating waves of the laser gyro leads to the zero shift and produces the component of the output signal that does not commute with the angular velocity. 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The expressions are valid when the gyro operates at the gain line centre and currents in its arms are balanced, however, the amplifications of counterpropagating waves are slightly different due to slightly different Q factors of the resonator for these waves. Analysis of the expressions suggests that the difference in the amplification of counterpropagating waves of the laser gyro leads to the zero shift and produces the component of the output signal that does not commute with the angular velocity. (laser applications and other topics in quantum electronics)</abstract><cop>Woodbury, NY</cop><pub>IOP Publishing</pub><doi>10.1070/QE2004v034n04ABEH002686</doi><tpages>5</tpages></addata></record> |
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| identifier | ISSN: 1063-7818 |
| ispartof | Quantum electronics (Woodbury, N.Y.), 2004-04, Vol.34 (4), p.388-392 |
| issn | 1063-7818 1468-4799 |
| language | eng |
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| source | Institute of Physics Journals |
| subjects | ANGULAR VELOCITY Beam characteristics: profile, intensity, and power spatial pattern formation CLASSICAL AND QUANTUM MECHANICS, GENERAL PHYSICS COLLECTIVE MODEL Design of specific laser systems ELECTRONIC EQUIPMENT Exact sciences and technology FREQUENCY ANALYSIS FUNCTIONS Fundamental areas of phenomenology (including applications) GYROFREQUENCY Laser optical systems: design and operation LASERS MATHEMATICAL MODELS NUCLEAR MODELS Optics Physics POLYNOMIALS RESONATORS ROTATION-VIBRATION MODEL VELOCITY WAVE PROPAGATION |
| title | Polynomial model of the frequency characteristic of a slowly rotating vibrating laser gyro with differently amplified counterpropagating waves |
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