The Fiber-Optic Gyroscope, Third Edition.
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Place / Publishing House: | Norwood : : Artech House,, 2022. ©2022. |
Year of Publication: | 2022 |
Edition: | 3rd ed. |
Language: | English |
Online Access: | |
Physical Description: | 1 online resource (509 pages) |
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Table of Contents:
- The Fiber-Optic Gyroscope, Third Edition
- Contents
- Foreword
- Preface to the First Edition
- Preface to the Second Edition
- Preface to the Third Edition
- Chapter 1 Introduction
- References
- Chapter 2 Principle of the Fiber-Optic Gyroscope
- 2.1 Sagnac-Laue Effect
- 2.1.1 A History of Optics from Aether to Relativity
- 2.1.2 Sagnac-Laue Effect in a Vacuum
- 2.1.3 Sagnac-Laue Effect in a Medium
- 2.2 Active and Passive Ring Resonators
- 2.2.1 Ring-Laser Gyroscope
- 2.2.2 Resonant Fiber-Optic Gyroscope
- 2.3 Passive Fiber-Ring Interferometer
- 2.3.1 Principle of the Interferometric Fiber-Optic Gyroscope
- 2.3.2 Theoretical Sensitivity of the I-FOG
- 2.3.3 Noise, Drift, and Scale Factor
- 2.3.4 ARW Versus Root PSD
- 2.3.5 Evaluation of Noise and Drift by Allan Variance (or Allan Deviation)
- 2.3.6 Allan Variance/Deviation Versus Standard Variance/Deviation
- 2.3.7 Bandwidth
- 2.3.8 Various Functions of a Gyro: Attitude Measurement, Gyro Compassing,and Inertial Navigation
- References
- Chapter 3 Reciprocity of a Fiber Ring Interferometer
- 3.1 Principle of Reciprocity
- 3.1.1 Single-Mode Reciprocity of Wave Propagation
- 3.1.2 Reciprocal Behavior of a Beam Splitter
- 3.2 Minimum Configuration of a Ring Fiber Interfero
- 3.2.1 Reciprocal Configuration
- 3.2.2 Reciprocal Biasing Modulation-Demodulation
- 3.2.3 Proper (or Eigen) Frequency
- 3.3 Reciprocity with All-Guided Schemes
- 3.3.1 Evanescent-Field Coupler (or X-Coupler or Four-Port Coupler)
- 3.3.2 Y-Junction
- 3.3.3 All-Fiber Approach
- 3.3.4 Hybrid Architectures with Integrated Optics:Y-Coupler Configuration
- 3.4 Problem of Polarization Reciprocity
- 3.4.1 Rejection Requirement with Ordinary Single-Mode Fiber
- 3.4.2 Use of Polarization-Maintaining (PM) Fiber
- 3.4.3 Use of Depolarizer
- 3.4.4 Use of an Unpolarized Source
- References.
- Chapter 4 Backreflection and Backscattering
- 4.1 Problem of Backreflection
- 4.1.1 Reduction of Backreflection with Slant Interfaces
- 4.1.2 Influence of Source Coherence
- 4.2 Problem of Backscattering
- 4.2.1 Coherent Backscattering
- 4.2.2 Use of a Broadband Source
- 4.2.3 Evaluation of the Residual Rayleigh Backscattering Noise
- References
- Chapter 5 Analysis of PolarizationNonreciprocities with BroadbandSource and High-BirefringencePolarization-Maintaining Fiber
- 5.1 Depolarization Effect in High-BirefringencePolarization-Maintaining Fibers
- 5.2 Analysis of Polarization Nonreciprocities in a Fiber GyroscopeUsing an All-Polarization-Maintaining Waveguide Configuration
- 5.2.1 Intensity-Type Effects
- 5.2.2 Comment About Length of Depolarization Ld Versus Length ofPolarization Correlation Lpc
- 5.2.3 Amplitude-Type Effects
- 5.3 Use of a Depolarizer
- 5.4 Testing with Optical Coherence Domain Polarimetry (OCDP), orToday, Distributed Polarization Crosstalk Analysis (DPXA)
- 5.4.1 OCDP, or DPXA, Based on Path-Matched White-Light Interferometry
- 5.4.2 OCDP/DPXA Using Optical Spectrum Analysis
- References
- Chapter 6 Time-Transience Related Nonreciprocal Effects
- 6.1 Effect of Temperature Transience: The Shupe Effect
- 6.2 Symmetrical Windings
- 6.3 Strain-Induced T-Dot Effect
- 6.4 Basics of Heat Diffusion and Temporal Signature of the Shupe and T-Dot Effects
- 6.5 Case of a Sinusoidal Temperature Variation
- 6.6 Simple Model of Thermally-Induced Differential Strainsin a Self-Standing Coil
- 6.6.1 Reminders About the Theory of Elasticity
- 6.6.2 Effect of the Fiber Coating
- 6.6.3 Simple Model of a Free-Standing Coil
- 6.7 Simple Viewing of Symmetrical Windings with the Thermally-Induced Differential Strains
- 6.8 Orthocyclic Winding for Hexagonal Close Packing
- 6.9 Effect of Acoustic Noise and Vibration.
- References
- Chapter 7 Truly Nonreciprocal Effects
- 7.1 Magneto-Optic Faraday Effect
- 7.2 Axial Magneto-Optic Effect
- 7.3 Nonlinear Kerr Effect
- References
- Chapter 8 Scale Factor Linearity and Accuracy
- 8.1 Problem of Scale Factor Linearity and Accuracy
- 8.2 Closed-Loop Operation Methods to Linearize Scale Factor
- 8.2.1 Use of a Frequency Shift
- 8.2.2 Use of an Analog Phase Ramp (or Serrodyne Modulation)
- 8.2.3 Use of a Digital Phase Ramp
- 8.2.4 All-Digital Closed-Loop Processing Method
- 8.2.5 Control of the Gain of the Modulation Chain with "Four-State"Modulation
- 8.2.6 Potential Spurious Lock-In (or Deadband) Effect
- 8.3 Scale Factor Accuracy
- 8.3.1 Problem of Scale Factor Accuracy
- 8.3.2 Wavelength Dependence of an Interferometer Response with a Broadband Source
- 8.3.3 Effect of Phase Modulation
- 8.3.4 Wavelength Control Schemes
- 8.3.5 Mean Wavelength Change with a Parasitic Interferometeror Polarimeter
- References
- Chapter 9 Recapitulation of the Optimal Operating Conditions and Technologies of the I-FOG
- 9.1 Optimal Operating Conditions
- 9.2 Broadband Source
- 9.2.1 Superluminescent Diode
- 9.2.2 Rare-Earth Doped Fiber ASE Sources
- 9.2.3 Excess RIN Compensation Techniques
- 9.3 Sensing Coil
- 9.4 "Heart" of the Interferometer
- 9.5 Detector and Processing Electronics
- 9.6 Summary of the Various Noises
- 9.7 Thermal Phase Noise (Optical Nyquist Noise)
- References
- Chapter 10 Alternative Approaches for the I-FOG
- 10.1 Alternative Optical Configurations
- 10.1.1 Use of a [3 × 3] Coupler
- 10.1.2 Use of a Quarter-Wave Plate
- 10.1.3 Use of a Laser Diode
- 10.2 Alternative Signal Processing Schemes
- 10.2.1 Open-Loop Scheme with Use of Multiple Harmonics
- 10.2.2 Second Harmonic Feedback
- 10.2.3 Gated Phase Modulation Feedback
- 10.2.4 Heterodyne and Pseudo-Heterodyne Schemes.
- 10.2.5 Beat Detection with Phase Ramp Feedback
- 10.2.6 Dual Phase Ramp Feedback
- 10.3 Extended Dynamic Range with Multiple Wavelength Source
- References
- Chapter 11 Resonant Fiber-Optic Gyroscope
- 11.1 Principle of Operation of an All-Fiber Ring Cavity
- 11.2 Signal Processing Method
- 11.3 Reciprocity of a Ring Fiber Cavity
- 11.3.1 Introduction
- 11.3.2 Basic Reciprocity Within the Ring Resonator
- 11.3.3 Excitation and Detection of Resonances in a Ring Resonator
- 11.4 Other Parasitic Effects in the R-FOG
- Acknowledgment
- References
- Chapter 12 Conclusions
- 12.1 The State of Development and Expectations in 1993
- 12.2 The State of the Art, Two Decades Later, in 2014, for the Second Edition
- 12.2.1 FOG Versus RLG
- 12.2.2 FOG Manufacturers, in 2014
- 12.3 The State of the Art, Today, in 2021
- 12.4 Trends for the Future and Concluding Remarks
- References
- Appendix A Fundamentals of Opticsfor the Fiber Gyroscope
- A.1 Basic Parameters of an Optical Wave: Wavelength,Frequency, and Power
- A.2 Spontaneous Emission, Stimulated Emission, and Related Noises
- A.2.1 Fundamental Photon Noise
- A.2.2 Spontaneous Emission and Excess Relative Intensity Noise
- A.2.3 Resonant Stimulated Emission in a Laser Source
- A.2.4 Amplified Spontaneous Emission
- A.3 Propagation Equation in a Vacuum
- A.4 State of Polarization of an Optical Wave
- A.5 Propagation in a Dielectric Medium
- A.5.1 Index of Refraction
- A.5.2 Chromatic Dispersion, Group Velocity, and Group Velocity Dispersion
- A.5.3 E and B, or E and H?
- A.6 Dielectric Interface
- A.6.1 Refraction, Partial Reflection, and Total Internal Reflection
- A.6.2 Dielectric Planar Waveguidance
- A.7 Geometrical Optics
- A.7.1 Rays and Phase Front
- A.7.2 Plane Mirror and Beam Splitte
- A.7.3 Lenses
- A.8 Interferences.
- A.8.1 Principle of Two-Wave Interferometry
- A.8.2 Most Common Two-Wave Interferometers:Michelson and Mach-Zehnder Interferometers, Young Double-Slit
- A.8.3 Channeled Spectral Response of a Two-Wave Interferometer
- A.9 Multiple-Wave Interferences
- A.9.1 Fabry-Perot Interferometer
- A.9.2 Ring Resonant Cavi
- A.9.3 Multilayer Dielectric Mirror and Bragg Reflector
- A.9.4 Bulk-Optic Diffraction Grating
- A.10 Diffraction
- A.10.1 Fresnel Diffraction and Fraunhofer Diffraction
- A.10.2 Knife-Edge Fresnel Diffraction
- A.11 Gaussian Beam
- A.12 Coherence
- A.12.1 Basics of Coherence
- A.12.2 Mathematical Derivation of Temporal Coherence
- A.12.3 Concept of Wave Train
- A.12.4 Case of an Asymmetrical Spectrum
- A.12.5 Case of Propagation in a Dispersive Medium
- A.13 Birefringence
- A.13.1 Birefringence Index Difference
- A.13.2 Change of Polarization with Birefringence
- A.13.3 Interference with Birefringence
- A.14 Optical Spectrum Analysis
- Bibliography
- Appendix B Fundamentals of Fiber-Optics for the Fiber-Gyroscope
- B.1 Main Characteristics of a Single-Mode Optical Fiber
- B.1.1 Attenuation of a Silica Fiber
- B.1.2 Gaussian Profile of the Fundamental Mode
- B.1.3 Beat Length and h Parameter of a PM Fiber
- B.1.4 Protective Coating
- B.1.5 Temperature Dependence of Propagation in a PM Fiber
- B.2 Discrete Modal Guidance in a Step-Index Fiber
- B.3 Guidance in a Single-Mode Fiber
- B.3.1 Amplitude Distribution of the Fundamental LP01 Mode
- B.3.2 Effective Index neff and Phase Velocity vϕ of the Fundamental LP01 Mode
- B.3.3 Group Index ng of the Fundamental LP01 Mode
- B.3.4 Case of a Parabolic Index Profile
- B.3.5 Modes of a Few-Mode Fiber
- B.4 Coupling in a Single-Mode Fiber and Its Loss Mechanisms
- B.4.1 Free-Space Coupling
- B.4.2 Misalignment Coupling Losses.
- B.4.3 Mode-Diameter Mismatch Loss of LP01 Mode.