GB2046470A - Optical interferometers - Google Patents
Optical interferometers Download PDFInfo
- Publication number
- GB2046470A GB2046470A GB8009558A GB8009558A GB2046470A GB 2046470 A GB2046470 A GB 2046470A GB 8009558 A GB8009558 A GB 8009558A GB 8009558 A GB8009558 A GB 8009558A GB 2046470 A GB2046470 A GB 2046470A
- Authority
- GB
- United Kingdom
- Prior art keywords
- optical
- polarisation state
- polarisation
- waveguides
- coil
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01C—MEASURING DISTANCES, LEVELS OR BEARINGS; SURVEYING; NAVIGATION; GYROSCOPIC INSTRUMENTS; PHOTOGRAMMETRY OR VIDEOGRAMMETRY
- G01C19/00—Gyroscopes; Turn-sensitive devices using vibrating masses; Turn-sensitive devices without moving masses; Measuring angular rate using gyroscopic effects
- G01C19/58—Turn-sensitive devices without moving masses
- G01C19/64—Gyrometers using the Sagnac effect, i.e. rotation-induced shifts between counter-rotating electromagnetic beams
- G01C19/72—Gyrometers using the Sagnac effect, i.e. rotation-induced shifts between counter-rotating electromagnetic beams with counter-rotating light beams in a passive ring, e.g. fibre laser gyrometers
- G01C19/721—Details
Description
SPECIFICATION
Optical interferometers
The invention relates to optical interferometers of the type comprising an optical single mode waveguide which is wound to form a coil.
Ring Interferometers of this type, often described as ring-interferometers, are based on the Sagnac effect, which produces non-reciprocal transit time differences in the coil when the arrangement rotates relative to a reference system, which differences can be established by interferometer analysis. Atypical application of a ring interferometer of this kind is in the field of navigation.
It has been observed that the bi-refringent properties of an optical single mode waveguide can lead to difficulties. In order to eliminate these difficulties, it has been proposed that polarisation filters whose polarisation planes are parallel to one another be employed between the ends of the single mode light waveguide and receiving photo-detectors, as is described for example in our co-pending United
Kingdom Patent Applications Nos. 79.03274 (Specifi- cation No. 2,014,329A); No.79.03275 (Specification
No. 2,013,929A); and No.79.11687 (Specification No.
2,01 8,456A).
One object of the present invention is to provide a ring interferometer of the type referred to in the introduction which does not require polarisation filters of this kind, but in which ensures that the birefringence properties of optical waveguides do not lead to difficulties.
The invention consists in an optical interferometer comprising a single mode light waveguide which is wound to form a coil, said single mode light waveguide consisting of one or more waveguides each capable of conducting only one polarisation state, and/or utilising optical directional couplers which can couple only one polarisation state to couple associated waveguides.
This proposal, which appears surprisingly simple, has been found to promptly and readily eliminate the difficulties which can be caused due to birefringence.
An optical waveguide which is only capable of conducting one polarisation state can consist of a fibre or a strip conductor. Optical waveguides of this kind, which are capable of assuming only one polarisation state, are disclosed in an article published in Appl. Phys. Lett. (1978) on pages 814-816, and in an article published in Appl. Phys.
Lett. 33(1978) on pages 699-701, which maintain a linear polarisation.
The proposed arrangement of the present invention can be applied to all the above-mentioned ring interferometers, irrespective of their construction, and may be utilised in still other ring interferometers to advantage.
In embodiments in which the light is fed to the coil or discharged therefrom in free beam paths, it is essential that the light waveguide of the coil should only conduct one polarisation state. This is the case for example in our co-pending Patent Application
No.79.30275 (Specification No. 2,013,929A); and in
Application No. 79.11687 (Specification No.
2,018,456A), see Figures 1 to 3 therein.
The invention will now be described in detail as applied to the known types described in the copending Applications listed above.
If the light in an optical circuit is fed to the coil of an interferometer, and/or discharged therefrom via an additional Iightwaveguide, it is expedient that these additionally provided light waveguides should be able to conduct only one polarisation state. An optical interferometer to which this comment applies is described and illustrated for example, in the exemplary embodiment shown in Figure 1 of our co-pending Patent Application No. 79.03274 (Specification No.2,01 4,329A) or in Figure 4 of the two other
Patent Applications listed above.
This circuit also contains optical directional couplers. It is expedient if these optical directional couplers are also only able to couple one polarisation state.
The three alternative possibilities can be employed individually, or in any arbitrary combination.
It will be obvious that the or each lightwaveguide which can conduct only one polarisation state, or the or each directional coupler which can couple only one polarisation state, should be so used in the construction of the ring interferometer that they achieve the same effect as that achieved by polarisation filters in the constructions described in the aforementioned Patent Applications.In the case of our Patent Application No. 79.03274 (Specification No. 2,014,329) this effect is safely achieved if both of the existing directional couplers can couple only one and the same polarisation state, and/or if ail the light waveguides of the optical circuit which are provided in addition to the coil, and from which the directional couplers are also constructed, can conduct only one and the same polarisation state. The waveguide of the coil itself can also consist of such an optical waveguide.If the waveguides of the optical circuit are conventional waveguides and their structure is provided for example with small curvatures and a short length, so that they do not involve any fundamentally disturbing effects, it is sufficient if only the light waveguide of the coil is a light waveguide which can conduct only one polarisation state.
1. An optical interferometer comprising a single mode light waveguide which is wound to form a coil, said single mode lightwaveguide consisting of one or more waveguides each capable of conducting only one polarisation state, and/or utilising optical directional couplers which can couple only one polarisation state to couple associated waveguides.
2. An optical interferometer as claimed in Claim 1, in which an additional optical single-mode waveguide capable of conducting only one polarisation state is provided, coupled to the existing waveguides of an optical interferometer in place of another type of polarisation filter.
**WARNING** end of DESC field may overlap start of CLMS **.
Claims (3)
1. An optical interferometer comprising a single mode light waveguide which is wound to form a coil, said single mode lightwaveguide consisting of one or more waveguides each capable of conducting only one polarisation state, and/or utilising optical directional couplers which can couple only one polarisation state to couple associated waveguides.
2. An optical interferometer as claimed in Claim 1, in which an additional optical single-mode waveguide capable of conducting only one polarisation state is provided, coupled to the existing waveguides of an optical interferometer in place of another type of polarisation filter.
3. An optical interferometer as claimed in Claim 1, substantially as described hereinbefore.
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DE19792911129 DE2911129A1 (en) | 1979-03-21 | 1979-03-21 | RING INTERFEROMETER WITH A SINGLE-MODE LIGHT-WAVE GUIDE WINDED TO A COIL |
Publications (2)
Publication Number | Publication Date |
---|---|
GB2046470A true GB2046470A (en) | 1980-11-12 |
GB2046470B GB2046470B (en) | 1983-08-03 |
Family
ID=6066031
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
GB8009558A Expired GB2046470B (en) | 1979-03-21 | 1980-03-21 | Optical interferometers |
Country Status (4)
Country | Link |
---|---|
JP (1) | JPS55128106A (en) |
DE (1) | DE2911129A1 (en) |
FR (1) | FR2452093A1 (en) |
GB (1) | GB2046470B (en) |
Cited By (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0059644A1 (en) * | 1981-03-04 | 1982-09-08 | Hitachi, Ltd. | Optical gyroscope |
EP0107373A2 (en) * | 1982-09-28 | 1984-05-02 | Fujitsu Limited | Fibre optic gyroscope |
US4519708A (en) * | 1981-05-20 | 1985-05-28 | Raytheon Company | Mode discrimination apparatus |
JPH03205507A (en) * | 1990-11-02 | 1991-09-09 | Hitachi Ltd | Optical gyroscope |
JPH08233583A (en) * | 1995-12-11 | 1996-09-13 | Hitachi Ltd | Optical fiber coil |
JP2574982B2 (en) | 1993-03-22 | 1997-01-22 | 株式会社日立製作所 | Optical fiber coil |
FR2824906A1 (en) * | 2001-05-18 | 2002-11-22 | Thales Sa | Fibre optic gyrometer non reciprocal measurement mechanism having light source and optical monomode filter with polarization separator producing light paths and polarization state detector. |
Family Cites Families (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE2804103A1 (en) * | 1978-01-31 | 1979-08-02 | Siemens Ag | INTERFEROMETER WITH A COIL FROM A SINGLE-MODE WAVE CONDUCTOR |
DE2804119A1 (en) * | 1978-01-31 | 1979-08-02 | Siemens Ag | INTERFEROMETER WITH A COIL FROM A SINGLE-MODE WAVE CONDUCTOR |
DE2814476A1 (en) * | 1978-04-04 | 1979-10-18 | Siemens Ag | INTERFEROMETER WITH A COIL FROM A SINGLE-MODE WAVE CONDUCTOR |
-
1979
- 1979-03-21 DE DE19792911129 patent/DE2911129A1/en active Granted
-
1980
- 1980-03-10 FR FR8005314A patent/FR2452093A1/en active Granted
- 1980-03-17 JP JP3385780A patent/JPS55128106A/en active Pending
- 1980-03-21 GB GB8009558A patent/GB2046470B/en not_active Expired
Cited By (11)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0059644A1 (en) * | 1981-03-04 | 1982-09-08 | Hitachi, Ltd. | Optical gyroscope |
US4483617A (en) * | 1981-03-04 | 1984-11-20 | Hitachi, Ltd. | Optical gyroscope with large propagation constant difference |
US4519708A (en) * | 1981-05-20 | 1985-05-28 | Raytheon Company | Mode discrimination apparatus |
EP0107373A2 (en) * | 1982-09-28 | 1984-05-02 | Fujitsu Limited | Fibre optic gyroscope |
EP0107373A3 (en) * | 1982-09-28 | 1986-11-12 | Fujitsu Limited | Fibre optic gyroscope |
JPH03205507A (en) * | 1990-11-02 | 1991-09-09 | Hitachi Ltd | Optical gyroscope |
JP2574982B2 (en) | 1993-03-22 | 1997-01-22 | 株式会社日立製作所 | Optical fiber coil |
JPH08233583A (en) * | 1995-12-11 | 1996-09-13 | Hitachi Ltd | Optical fiber coil |
FR2824906A1 (en) * | 2001-05-18 | 2002-11-22 | Thales Sa | Fibre optic gyrometer non reciprocal measurement mechanism having light source and optical monomode filter with polarization separator producing light paths and polarization state detector. |
WO2002095332A1 (en) * | 2001-05-18 | 2002-11-28 | Thales | Device for measuring a non-reciprocal effect, in particular fibre-optic gyro |
US7130053B2 (en) | 2001-05-18 | 2006-10-31 | Thales | Device for measuring a non-reciprocal effect, in particular fiber-optic gyro |
Also Published As
Publication number | Publication date |
---|---|
FR2452093A1 (en) | 1980-10-17 |
FR2452093B1 (en) | 1984-10-19 |
GB2046470B (en) | 1983-08-03 |
JPS55128106A (en) | 1980-10-03 |
DE2911129C2 (en) | 1991-05-08 |
DE2911129A1 (en) | 1980-10-16 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
US4354760A (en) | Ring interferometer comprising a single-mode light waveguide | |
CA1284908C (en) | Optical power splitter and polarization splitter | |
GB1368598A (en) | Light beam polarization modulator | |
ES2169196T3 (en) | ROTATION PERCEPTOR. | |
US4653917A (en) | Fiber optic gyroscope operating with unpolarized light source | |
DE69009902T2 (en) | Single-mode fiber for one direction of polarization. | |
CA2345561A1 (en) | Fiber-optic current sensor | |
GB2014329B (en) | Optical interferometers for use in angular velocity measurement by the sagnac effect | |
US11549812B2 (en) | Compact optical-fibre Sagnac interferometer | |
JP2000513812A (en) | 3-axis optical fiber gyroscope | |
BR9911403A (en) | Monolithic coaxial device | |
CN110470292A (en) | A kind of self seeding frequency locking resonance type optical gyroscope and its working method | |
GB2046470A (en) | Optical interferometers | |
EP0260885A3 (en) | Dual fiber optic gyroscope | |
BR8406079A (en) | DIRECTIONAL COUPLER | |
SE8900942D0 (en) | FIBEROPTICAL GYRON | |
ATE114077T1 (en) | WAVEGUIDE TWIST. | |
Kim et al. | Acousto-Optic Frequency Shifting in Two-Mode Optical Fibers | |
CN107764253A (en) | Optical fibre gyro | |
Peng et al. | Observation and analysis of noise due to birefringence modulation in a fibre-optic gyroscope | |
Gonthier et al. | Compact all-fiber wavelength filter synthesis for 1300/1550 nm demultiplexing isolation | |
JP2552603B2 (en) | Fiber optic gyro | |
KR890000911A (en) | Optical waveguide coupler | |
Ahmed et al. | Proposed interferometric filters | |
Davis | Introduction to fiberoptic sensors. |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
732 | Registration of transactions, instruments or events in the register (sect. 32/1977) | ||
PE20 | Patent expired after termination of 20 years |
Effective date: 20000320 |