US 6,539,134 B1Grant
Polarization transformer
Issue Date:2003-03-25
•9 Claims
•3 Drawing Sheets
Abstract
A method for fabricating a transformer of linearly polarized light to elliptically polarized light is presented. The method involves twisting a birefringent fiber through angles that depend on the polarization desired. This technique obviates the need to splice fibers, as in common approaches. In the final step of the method, the polarization can be fine tuned by heating the fiber to cause the core of the fiber to diffuse into the cladding. Also, methods and systems are presented to transform substantially polarized light to substantially randomly polarized light.
Metadata
Assignee
- KVH Industries, Inc.
Inventor
- Richard B. Dyott
Application Information
Application Number:US 09/337,223
Filing Date:1999-06-22
Priority Date:1999-02-11
Art Unit:7
Classifications
IPC:
G02B 600
Field of Search:
385 11385 12385123
Patent Drawings (3 sheets)
Description
Cross-Reference to Related Applications
[0002] This application is based upon and claims priority to the following U.S. patent applications. U.S. provisional patent application, serial application No. 60/119,999, filed on Feb. 11, 1999; U.S. provisional patent application, serial application No. 60/120,000, filed on Feb. 11, 1999; U.S. provisional patent application, serial application No. 60/133,357, filed on May 10, 1999; and U.S. provisional patent application, serial application No. 60/134,154, filed on May 14, 1999. This application is also based upon U.S. application entitled Current Sensor, invented by Richard Dyott, which has been filed concurrently with the present application on Jun. 22, 1999. All of the aforementioned applications are hereby incorporated by reference.
Background of the Invention
[0003] 1. Field of the Invention
[0004] This application relates to optical devices that transform light between linearly and elliptically polarized states.
[0005] 2. Description of Related Art
[0006] Devices that transform linearly polarized light to circularly polarized light and the reverse are known in the literature. To make such optical devices, one may use one birefringent fiber with two beams of light of equal frequency and amplitude (or, equivalently, one beam that is the vector sum of these two beams). If the two beams are propagated perpendicular to an optic axis, circularly polarized light may result. Alternatively, linearly polarized light may be transformed to circularly polarized light by using one beam and two fibers.
[0007] In practice, constructing a single-beam transformer of linearly to circularly polarized light involves first starting with a length of transforming fiber greater than a predetermined length, and performing several iterations of cutting and measuring polarization until the polarization is deemed to be circular to within some specification. Needless to say, this is a tedious and lengthy procedure requiring lots of guesswork.
Summary of the Invention
[0008] A transformer of polarized light comprising a birefringent fiber which is twisted through an angle into a corkscrew shape at an appropriate distance from an end of the fiber is presented herein; the angle and distance are so chosen that linearly polarized light entering the other end of the fiber exits the fiber elliptically polarized. In various embodiments, the angle is approximately π/4 radians, or an odd multiple thereof, and the distance is approximately one quarter of a beatlength, or an odd multiple thereof. The transformer of polarized light may include an optical fiber twisted about a central axis running therethrough wherein the fiber is characterized by the absence of spliced sections.
[0009] A method of fabricating a transformer of polarized light comprising twisting a birefringent fiber through an angle to produce a corkscrew shape is also presented; twisting a birefringent fiber may include twisting the fiber through an angle of approximately π/4 radians, or an odd multiple thereof, and twisting the fiber at a distance of approximately one quarter of a beatlength, or an odd multiple thereof, from an end of the fiber.
[0010] A method of fabricating a transformer of polarized light is also presented which may include heating a birefringent fiber, having a core and a cladding, so as to cause the core to diffuse into the cladding, and thereby changing the state of polarization of light that may exit the fiber. The method may further include previously twisting the fiber through an angle to produce a corkscrew shape. (In one embodiment, this angle is π/4 radians.) Twisting the fiber includes twisting the fiber at a distance of approximately one quarter of a beatlength from an end of the fiber.
[0011] Also presented is a method of transforming substantially linearly polarized light into substantially circularly polarized light including twisting a birefringent fiber through an angle of π/4 radians to produce a corkscrew shape at a distance of approximately one quarter of a beatlength from an end of the fiber; shining substantially linearly polarized light through the other end of the fiber; and fine tuning the polarization of the light exiting the fiber by heating the fiber so as to cause the core to diffuse into the cladding, until the light is substantially circularly polarized. The twist in the fiber can be accomplished by heating the fiber before, during, or after the twisting.
[0012] The invention further includes a transformer of polarized light comprising a birefringent fiber. The fiber has a first end through which the polarized light enters and a second end through which light exits. The fiber is also twisted through an angle into a corkscrew shape at an appropriate distance from the second end, the angle and distance so chosen that polarized light entering the first end exits the second end randomly polarized. The appropriate length may be greater than a decoherence length.
[0013] Also presented is a method of transforming substantially polarized light into substantially randomly polarized light including twisting a birefringent fiber, having a first end through which the substantially polarized light enters and a second end through which the substantially randomized light exits, through an angle of π/4 radians to produce a corkscrew shape at a distance of at least one decoherence length from the second end of the fiber; and shining substantially polarized light through the first end of the fiber to allow substantially randomly polarized light to exit the second end.
[0014] Also presented is a method of transforming substantially linearly polarized light into substantially circularly polarized light comprising twisting a birefringent fiber, having two ends, about its central axis through an angle approximately equal to an odd multiple of π/4 radians, at a distance of slightly more than odd multiple of one quarter of a beatlength from a first end of the fiber, shining substantially linearly polarized light through a second end of the fiber, and fine turning the polarization of the light exiting the first end of the fiber by heating the fiber between the twist and the first end, so as to cause the core to diffuse into the cladding, until the exiting light is substantially circularly polarized. The odd multiple of one quarter of a beatlength may be 1. The odd multiple of π/4 radians may be 1. The birefringent fiber may be twisted while being heated near the location of the twist or after having been heated near the location of the twist.
Brief Description of Drawings
[0015] FIG. 1 illustrates the conventional method of fabricating a transformer of linearly to circularly polarized light by splicing two fibers that are properly oriented.
[0016] FIG. 2 is a schematic of a twisted fiber of the present invention that obviates the need to splice fibers together.
[0017] FIG. 3 illustrates how fine tuning of the polarization can be achieved by heating the fiber to cause diffusion of the core into the cladding.
Detailed Description of the Preferred Embodiment(s)
[0018] It is often desirable to transform the polarization of a beam of light from one state to another. For this purpose optical devices have been fabricated that input linearly polarized light and output elliptically polarized light. These devices typically function by causing one of two incident linearly polarized light beams to lag behind the other by a pre-selected phase difference. Altering the relative phase of the two incident beams has the effect of changing the state of polarization of the light that exits the optical device. Before considering how these devices of the prior art perform the transformation of linearly to elliptically polarized light and before presenting the detailed description of the preferred embodiment of the present invention, it will be useful to first recall how elliptically polarized light arises.
[0019] Two orthogonal electric fields, Exand Ey, both propagating in the z direction can be described by the following two equations
[0020] Ex=iE0xcos(kz−ωt) (1)
[0021] and
[0022] Ey=j E0ycos(kz−ωt+δ), (2)
[0023] where i and j are unit vectors in the x and y directions, k is the propagation number, ω is the angular frequency, and δ is the relative phase difference between the two modes. The total electric field E is just given by the vector sum Ex+Ey. An observer standing at a fixed point on the z-axis and measuring the components Exand Eyof the total electric field simultaneously would find that these components would fall on the curve
[0024] (Ex/E0x)2+(Ey/E0y)2−2(Ex/E0x) (Ey/E0y)cos δ=sin2δ. (3)
[0025] Equation (3) is the well known equation of an ellipse making an angle α with the (Ex, Ey)-coordinate system, where
[0026] tan 2α=(2E0xE0ycos δ)÷(E0x2−E0y2). (4)
[0027] Hence, E corresponds to elliptically polarized light. From Equation (3) can be seen that the phase difference δ dictates some of the characteristics of the ellipse. For example, if δ were equal to an even multiple of 2π (i.e., if Exand Eyare in phase), then Equation (3) reduces to Ey=(E0y/E0x)Ex, which is the equation of a straight line; in that case, E is linearly polarized. On the other hand, if δ is equal to ±π/2, ±3π/2, ±5π/2, . . . , and assuming E0x=E0y=E0, Equation (3) reduces to E0x2+E0y2=E02, which is the equation of a circle. In that case, E is circularly polarized. Of course, linearly and circularly polarized light are just special cases of elliptically polarized light, a line and a circle being special types of ellipses.
[0028] From the above considerations, it is clear that if two perpendicular modes of light with equal amplitudes, such as that described by Equations (1) and (2) with E0x=E0y, enter an optical device, and proceed to exit the device with a phase shift of π/2, the result would be circularly polarized light. Typical optical devices that serve to transform linearly polarized light to circularly polarized light work on this principle.
[0029] For example, birefringent light fibers are anisotropic meaning that they do not have the same optical properties in all directions. Such fibers have the following properties: If two linearly polarized light beams are traveling along the fiber, or along the z axis, and furthermore one beam is polarized along the y axis and the other along the x axis, then, while the beam polarized along the y axis will travel at a speed v, the other beam that is polarized along the x axis will have a different speed. (In a birefringent fiber, the term “optic axis” may refer to either the fast or the slow axis, which are taken here to be the x and y axes, both perpendicular to the propagation axis, taken here to be the z axis.) Such two beams moving perpendicular to an optic axis may enter the fiber in phase, but because of their disparate speeds will exit with a non-zero phase difference δ. The result, as was seen above, is elliptically polarized light.
[0030] In the time, Δt, that it takes the faster moving beam to traverse the birefringent fiber, the faster moving beam, with speed vfast, will outpace the slower moving beam, with speed vslow, by a distance (vfast−vslow)Δt. This last mentioned distance contains (vfast−vslow)Δt/λslowwaves of the slower moving beam having wavelength λslow. Noting that Δt=L/vfast, where L is the fiber length, the phase difference between the two beams is given by
[0031] δ=2π(vfast−vslow)L/(λslowvfast). (5)
[0032] This last equation can be rewritten by substituting
[0033] vfast=λfastν, (6)
[0034] and
[0035] vslow=λslowν, (7)
[0036] where ν is the common frequency of the slow and fast beams, to yield
[0037] L=(δ/2π) (1/λslow−1/λfast)−1 (8)
[0038] This last equation makes clear that one can tailor a birefringent fiber to act as a transformer of linearly polarized light into elliptically polarized light simply by choosing the correct length, L, of fiber, although this length depends on the frequency of the light through Equations (7) and (8). The length of fiber that results in a phase difference of 2π and that therefore leaves the polarization unchanged is known as a beatlength, denoted by Lb, and will play a role in the discussion below.
[0039] The above discussion may be generalized to show that if instead of purely monochromatic light, light containing a spectrum of wavelengths is employed, birefringent fibers may be employed to convert such linearly polarized light to elliptically polarized light, where the degree of polarization of the output light decreases with increasing width of the input spectrum. In addition, the above discussion may be generalized to show that the polarization transformer will convert elliptically polarized light into linearly polarized light, if the light propagates through the fiber in the reverse direction.
[0040] To make optical devices that transform linearly polarized light into elliptically polarized light, one may use a birefringent fiber with two beams of light of equal frequency and amplitude (or, equivalently, one beam that is the vector sum of these two beams, since, as is known in the art, a single beam of linearly polarized light may be described as the vector sum of two beams, each with a single linear polarization component; conversely, two linearly polarized beams may be vector summed into a single linearly polarized beam). Alternatively, polarization components of unequal amplitude may be employed. As was discussed above, if the two beams are propagated perpendicular to the x axis, and their polarizations are along the x and y axes, elliptically polarized light may result. Alternatively, linearly polarized light may be transformed to circularly polarized light by using one beam and two birefringent fibers, one of which is rotated by 45 degrees with respect to the other about the common propagation axis of the fibers, and of length Lb/4.
[0041] Referring to FIG. 1, such a single-beam transformer of linearly polarized light to circularly polarized light may be constructed by fusing two silica or glass birefringent fibers. One of these fibers is the transmitting fiber 2 that delivers light to a second birefringent fiber known as the transforming fiber 4. The transforming fiber 4 is cut to a length of Lb/4. In addition, the relative orientation of the two fibers is chosen so that the transmitting fiber 2 is rotated π/4 radians with respect to the transforming fiber, about the common propagation axis of the two fibers, as indicated by the transmitting fiber cross section 6 and the transforming fiber cross section 8. Such a splicing operation may be done with a commercially available fusion splicer. However, any misalignment of the fibers results in some light being lost at the splice 10. Moreover, as Equation 5 makes clear, errors in the phase difference δ grow linearly with errors in the fiber length L. In practice, constructing a single-beam transformer of linearly to circularly polarized light involves first starting with a length of transforming fiber 4 greater than Lb/4, and performing several iterations of cutting and measuring polarization of light emerging from the end of the transforming fiber until the polarization is deemed to be circular to within some specification. Needless to say, this is a tedious and lengthy procedure requiring lots of guesswork.
[0042] The present invention resolves some of the aforementioned problems by presenting an alternate method of fabricating a single-beam transformer of polarized light. Referring to FIG. 2, instead of splicing two fibers offset by π/4 radians, in the method of the present invention a single birefringent fiber 12 is twisted about its central axis by this angle. In an alternate embodiment, the fiber may be twisted by an angle of an odd multiple of π/4 radians. The twist 14 in the fiber may be accomplished by heating the birefringent fiber 12 using arc electrodes 16, or other local heat source known to those of skill in the art. This may be done while applying torsion to twist the fiber, using methods known to those of skill in the art.
[0043] Referring to FIG. 3, in lieu of the tedious iterations of cutting and monitoring, in the method of the present invention, fine tuning is achieved by heating the portion of the fiber beyond the twist with a diffusing arc 26 produced by arc electrodes 22, or other local heat source known to those of skill in the art, to cause diffusion of the fiber core into the cladding. The heating can continue until a polarization monitor 24 indicates that the right polarization state is achieved. The effect of the diffusion is to expand the fields of the fiber modes and so reduce the effective difference vfast−vslow, thereby increasing the beat length.
[0044] The steps of twisting and diffusing are conceptually independent, and each can be used profitably to make transformers of linearly to elliptically polarized light. Varying the angle through which the birefringent fiber 12 is twisted is tantamount to varying the amplitudes E0xand E0yof Equation (3) and results in different states of elliptically polarized light. The step of diffusing, on the other hand, can be used any time some fine tuning of the polarization is required. For example, after splicing two fibers of appropriate length according to conventional methods, the state of polarization can be fine tuned by causing the core to diffuse into the cladding.
[0045] One can also fabricate a transformer using one birefringent fiber and two beams of linearly polarized light. If the two beams are propagated perpendicular to the x axis, and their polarizations are along the x and y axes, elliptically polarized light results. After cutting the single fiber to an appropriate length, fine tuning of the sought-after polarization can be achieved by heating the fiber to cause diffusion of the core into the cladding as mentioned above.
[0046] The present invention presents a more convenient method to fabricate a transformer of polarized light. The first step of the method obviates the need to splice a transmitting fiber 2 to a transforming birefringent fiber 4 of length Lb/4 with the aim of producing a transformer of linearly to circularly polarized light. Instead, a convenient length of a birefringent fiber 12 is heated to the softening point of the glass and then twisted through an angle of approximately π/4 radians. In some embodiments, an angle approximately equal to an odd multiple of π/4 may be employed. The sense of the output polarization (i.e., whether the light is right- or left-circularly polarized) may be determined by the orientation of the input light's polarization vector with respect to the direction of the twist. In a preferred embodiment, the twisting should occur over as short a length as possible. Employing a twist rather than a splice between two fibers offset by an angle keeps optical losses low. What losses do occur may be scarcely measurable in practice.
[0047] In the next step of the invention, fine tuning is performed in the following manner. First, the birefringent fiber 12 is cut so that its length from the twist 14 to the end of the fiber is slightly larger than Lb/4. In an alternate embodiment, the length of the fiber after the twist may be approximately equal to an odd multiple of Lb/4. The twisted birefringent fiber 12 is positioned between the arc electrodes 22 of a fiber fusion splicer. A diffusing arc 26 may be struck at a current lower than that used for splicing in order to raise the temperature of the birefringent fiber 12 to a point below its melting point, but where the fiber core begins to diffuse into the cladding. The effect of the diffusion is to expand the fields of the fiber modes and so reduce the effective birefringence. The light emerging from the transformer is monitored during this operation with the use of a polarization monitor 24, and diffusion is stopped when the light is circularly polarized. FIG. 3 shows the arrangement.
[0048] Although what was described above is a preferred method for fabricating a single-beam transformer of linearly to circularly polarized light by the steps of twisting and diffusing, it should be understood that these two steps are independent and each may be profitably used individually. For example, to form a single-beam transformer of linearly to circularly polarized light, a single birefringent fiber can be twisted as described above, and then fine tuned not by the preferred method of diffusing, but by a conventional method of iterations of cutting the fiber to an appropriate length and monitoring the polarization.
[0049] Alternatively, two fibers may be spliced together as in usual approaches. The transforming fiber would then be cut to a length of approximately Lb/4. However, unlike the usual methods that then fine tune by iterations of cutting and monitoring, the tuning could proceed by causing the core to diffuse into the cladding, as described above.
[0050] Finally, instead of twisting a birefringent fiber through an angle of π/4 radians, which corresponds to choosing E0x=E0yin Equation (3), the fiber could be twisted through varying angles. This would be effectively equivalent to varying the amplitudes E0xand E0y. As can be seen from this equation, even if the length of the fiber would lead to a phase difference of π/4 radians, the result would generally be elliptically polarized light that is non-circular.
[0051] The above methods have involved fabricating a single-beam transformer of linearly to circularly, or in the case where the twisting angle is not π/4 radians or an odd multiple thereof, elliptically polarized light. As mentioned above, one can also build a transformer using one birefringent fiber and two beams of orthogonally linearly polarized light (of course, two beams of superposed light is equivalent to a single beam equal to the vector sum of the two constituent beams). If the two beams are propagated along the z axis perpendicular to the x axis, and their polarizations are along the x and y axes, elliptically polarized light may result. According to Equations 3, 4, and 5, the type of elliptically polarized light that results depends on the length of the fiber, L. After cutting a birefringent fiber to an appropriate length, fine tuning of the polarization can proceed by diffusing the core into the cladding, as described above.
[0052] In a related application of the present invention, the twisting procedure described above may also be used to construct depolarizing fiber. If light having a band of different frequencies enters a fiber with the type of twist described above, after traveling a certain length known as the decoherence length (see Richard B. Dyott, Elliptical Fiber Waveguides,Artech House, which is incorporated herein by reference), the emergent light will be randomly polarized even if the light entering the fiber was polarized. Such randomly polarized light may have various applications known to those of ordinary skill in the art.
[0053] The transformer of linearly to circularly polarized light described above can be used in a current sensor exploiting the Faraday Effect in a Sagnac interferometer. A main feature of a Sagnac interferometer is a splitting of a beam of light into two beams. By using mirrors or optical fibers, both beams of light are made to traverse at least one loop, but in opposite directions. At the end of the trip around the loop, both beams are recombined thus allowing interference to occur. Any disturbance that affects one or both beams as they are traversing the loop has the potential to alter the interference pattern observed when the beams recombine. Rotating the device is the traditional disturbance associated with Sagnac's name. Another disturbance, giving rise to the Faraday Effect, involves applying an external magnetic field to the medium that forms the loop through which the light travels. Under the influence of such a field, the properties of the light-transmitting medium forming the loop are altered so as to cause a change in the direction of polarization of the light. In turn, this change in the direction of polarization results in a change in the interference pattern observed. These types of disturbances that give rise to a modification in the observed interference pattern are known as non-reciprocal disturbances. They are so-called because, unlike reciprocal effects in which the change produced in one beam cancels with that produced in the other, the changes produced in the two beams reinforce to yield a modification in the resultant interference pattern.
[0054] There is therefore in place a technique for measuring the current through a conductor: as a consequence of the Biot-Savart Law, an infinitely long conducting wire, for example, carrying a current i, gives rise to a magnetic field whose magnitude at a distance R from the wire is μ0i÷(2πR), where uo is the permeability of free space. If the Sagnac interferometer described above is immersed in this magnetic field, the properties of the fiber that composes the coil will change so as to affect the interference pattern observed. Thus, from the change in this pattern, the current i can be inferred. Similar current sensors are known in the prior art, e.g., Interferometer device for measurement of magnetic fields and electric current pickup comprising a device, U.S. Pat. No. 4,560,867, naming Papuchon; Michel; Arditty; Herve; Puech; Claude as inventors, which is incorporated by reference herein. The design of current sensors is similar to that of fiber optic rotation sensors of the type that appears in Fiber Optic Rotation Sensor or Gyroscope with Improved Sensing Coil, U.S. Pat. No. 5,552,887, naming Dyott, Richard B. as inventor, which is incorporated by reference herein.
[0055] It will be understood by those of ordinary skill in the art, that perfectly linearly or circularly polarized light may be an idealization that can not be realized. I.e., in practice, there may exist uncontrollable factors that give rise to some deviations from perfectly linearly or circularly polarized light. Therefore, it should be understood that when reference is made to linearly or circularly polarized light the meaning of these terms should be taken to mean effectively or approximately linearly or circularly polarized light.
[0056] While the invention has been disclosed in connection with the preferred embodiments shown and described in detail, various modifications and improvements thereon will become readily apparent to those skilled in the art. Accordingly, the spirit and scope of the present invention is to be limited only by the following claims.
Claims
What is claimed is:
1. A method of transforming substantially linearly polarized light into substantially circularly polarized light comprising
a) twisting a birefringent fiber through an angle of π/4 radians to produce a corkscrew shape at a distance of one quarter of a beatlength from an end of the fiber;
b) shining substantially linearly polarized light through an end of the fiber furthest from the twist; and
c) fine tuning the substantially circularly polarized light exiting the fiber by heating the fiber so as to cause the core to diffuse into the cladding.
2. A method of transforming substantially linearly polarized light into substantially circularly polarized light as in claim 1 wherein twisting a birefringent fiber occurs after heating the fiber.
3. A method of transforming substantially polarized light into substantially randomly polarized light comprising
a) twisting a birefringent fiber, said fiber having a first end through which the substantially polarized light enters and a second end through which the substantially randomized light exits, through an angle of π/4 radians about a central axis running therethrough, at a distance of at least one decoherence length from the second end of the fiber; and
b) shining substantially polarized light through the first end of the fiber to allow substantially randomly polarized light to exit the second end.
4. A method of transforming substantially linearly polarized light into substantially circularly polarized light comprising
a) twisting a birefringent fiber, having two ends, about its central axis through an angle approximately equal to an odd multiple of π/4 radians, at a distance of slightly more than an odd multiple of one quarter of a beatlength from a first end of the fiber;
b) shining substantially linearly polarized light through a second end of the fiber; and
c) fine tuning the polarization of the light exiting the first end of the fiber by heating the fiber between the twist and the first end, so as to cause the core to diffuse into the cladding, until the exiting light is substantially circularly polarized.
5. The method of transforming substantially linearly polarized light into substantially circularly polarized light of claim 4, wherein the odd multiple of π/4 radians is 1.
6. The method of transforming substantially linearly polarized light into substantially circularly polarized light of claim 4, wherein the odd multiple of one quarter of a beatlength is 1.
7. The method of transforming substantially linearly polarized light into substantially circularly polarized light of claim 6, wherein the odd multiple of π/4 radians is 1.
8. The method of transforming substantially linearly polarized light into substantially circularly polarized light of claim 4, wherein the birefringent fiber is twisted while being heated near the location of the twist.
9. The method of transforming substantially linearly polarized light into substantially circularly polarized light of claim 4, wherein the birefringent fiber is twisted after having been heated near the location of the twist.
Patent Citations (86)
| Patent | Date | Inventor | Cited By |
|---|---|---|---|
| US4756589(A) | 1986-01-01 | Bricheno et al. | Applicant |
| US4571650(A) | 1986-02-01 | Ojima et al. | Applicant |
| US4603931(A) | 1986-08-01 | Yoshimasa et al. | Applicant |
| US4615582(A) | 1986-10-01 | Lefevre et al. | Applicant |
| US4630229(A) | 1986-12-01 | D'Hondt | Applicant |
| US4630890(A) | 1986-12-01 | Ashkin et al. | Applicant |
| US4637722(A) | 1987-01-01 | Kim | Applicant |
| US4668264(A) | 1987-05-01 | Dyott | Applicant |
| US4669264(A) | 1987-05-01 | Dyott | Applicant |
| US4697876(A) | 1987-10-01 | Dyott | Applicant |
| US4712866(A) | 1987-12-01 | Dyott | Applicant |
| US4733938(A) | 1988-03-01 | Lefevre et al. | Applicant |
| US4740085(A) | 1988-04-01 | Lim | Applicant |
| US4755021(A) | 1988-07-01 | Dyott | Applicant |
| US4765739(A) | 1988-08-01 | Koizumi et al. | Applicant |
| US4776700(A) | 1988-10-01 | Frigo | Applicant |
| US4796993(A) | 1989-01-01 | Sonobe et al. | Applicant |
| US4815817(A) | 1989-03-01 | Levinson | Applicant |
| US4842409(A) | 1989-06-01 | Arditty et al. | Applicant |
| US4848910(A) | 1989-07-01 | Dupraz | Applicant |
| US4883358(A) | 1989-11-01 | Okada | Applicant |
| US4887900(A) | 1989-12-01 | Hall | Applicant |
| US4943132(A) | 1990-07-01 | Huang | Examiner |
| US5033854(A) | 1991-07-01 | Matthews et al. | Applicant |
| US5048962(A) | 1991-09-01 | Kurokawa et al. | Applicant |
| US5074665(A) | 1991-12-01 | Huang et al. | Applicant |
| US5080489(A) | 1992-01-01 | Nishikawa et al. | Applicant |
| US5096312(A) | 1992-03-01 | Huang | Applicant |
| US5106193(A) | 1992-04-01 | Fesler et al. | Applicant |
| US5133600(A) | 1992-07-01 | Schröder | Applicant |
| US5135555(A) | 1992-08-01 | Coyle, Jr. et al. | Applicant |
| US5289257(A) | 1994-02-01 | Kurokawa et al. | Applicant |
| US5289258(A) | 1994-02-01 | Szafraniec et al. | Applicant |
| US5331404(A) | 1994-07-01 | Moeller et al. | Applicant |
| US5351123(A) | 1994-09-01 | Spahlinger | Applicant |
| US5359413(A) | 1994-10-01 | Chang et al. | Applicant |
| US5365338(A) | 1994-11-01 | Bramson | Applicant |
| US5412471(A) | 1995-05-01 | Tada et al. | Applicant |
| US5459575(A) | 1995-10-01 | Malvern | Applicant |
| US5469257(A) | 1995-11-01 | Blake et al. | Applicant |
| US5469267(A) | 1995-11-01 | Wang | Applicant |
| US5471301(A) | 1995-11-01 | Kumagai et al. | Applicant |
| US5493396(A) | 1996-02-01 | Sewell | Applicant |
| US5500909(A) | 1996-03-01 | Meier | Applicant |
| US5504684(A) | 1996-04-01 | Lau et al. | Applicant |
| US5552887(A) | 1996-09-01 | Dyott | Applicant |
| US5559908(A) | 1996-09-01 | August et al. | Applicant |
| US5644397(A) | 1997-07-01 | Blake | Applicant |
| US5654906(A) | 1997-08-01 | Youngquist | Applicant |
| US5655035(A) | 1997-08-01 | Burmenko | Applicant |
| US5682241(A) | 1997-10-01 | Mark et al. | Applicant |
| US5701177(A) | 1997-12-01 | Kumagai et al. | Applicant |
| US5701376(A) | 1997-12-01 | Masataka | Applicant |
| US5767509(A) | 1998-06-01 | Cardova et al. | Applicant |
| US5781675(A) | 1998-07-01 | Tseng et al. | Applicant |
| US5854864(A) | 1998-12-01 | Knoesen et al. | Applicant |
| US5898496(A) | 1999-04-01 | Huang et al. | Applicant |
| US5946097(A) | 1999-08-01 | Sanders et al. | Applicant |
| US5953121(A) | 1999-09-01 | Bohnert et al. | Applicant |
| US5987195(A) | 1999-11-01 | Blake | Examiner |
| US6023331(A) | 2000-02-01 | Blake et al. | Applicant |
| US6025915(A) | 2000-02-01 | Michal et al. | Applicant |
| US6047095(A) | 2000-04-01 | Knoesen et al. | Applicant |
| US6075915(A) | 2000-06-01 | Koops et al. | Applicant |
| US6148131(A) | 2000-11-01 | Geertman | Examiner |
| US6396965(B1) | 2000-11-01 | Anderson | Applicant |
| US6163632(A) | 2000-12-01 | Rickman et al. | Examiner |
| US6389185(B1) | 2001-01-01 | Meise et al. | Applicant |
| US6185033(B1) | 2001-02-01 | Bose et al. | Applicant |
| US6233371(B1) | 2001-05-01 | Kim et al. | Examiner |
| US6301400(B1) | 2001-10-01 | Sanders | Examiner |
| US6351310(B1) | 2002-02-01 | Emge et al. | Applicant |
| US6370289(B1) | 2002-04-01 | Bennett | Applicant |
| DE330510 | 1984-08-01 | Applicant | |
| DE3615305 | 1987-11-01 | Applicant | |
| DE3742201 | 1989-06-01 | Applicant | |
| EP551874 | 1993-07-01 | Applicant | |
| EP586242 | 1994-03-01 | Applicant | |
| EP686867 | 1995-12-01 | Applicant | |
| EP722081 | 1996-07-01 | Applicant | |
| EP856737 | 1998-08-01 | Applicant | |
| EP871009 | 1998-10-01 | Applicant | |
| FR2535463 | 1984-05-01 | Applicant | |
| JP7209398 | 1995-08-01 | Applicant | |
| WO9858268 | 1998-12-01 | Applicant | |
| WO/36425 | 2000-07-01 | Applicant |
Non-Patent Literature (24)
- US 6,208,775, 3/2001, Dyott (withdrawn)Applicant
- Notification of Transmittal of the International Search Report.Applicant
- Alekseev et al; “Fiber Optic Gyroscope With Suppression of Excess Noise From the Radiation Source”, Technical Physical Letters, 24(9): 719-721, (Sep. 1998).Applicant
- Blake et al., “In-Line Sagnac Interferometer Current Sensor,” IEEE, pp. 116-121 (1995).Applicant
- Blake and Szarfraniec, “Random Noise in PM and Depolarized Fiber Gyros”, OSA Symposium Proceedings, 1997, OWB2, pp. 122-125.Applicant
- Bohnert. et al., “Field Test of Interferometric Optical Fiber High-Voltage and Current Sensors” SPIE, vol. 2360 pp. 16-19 (Feb. 1994).Applicant
- Bohnert. et al., “Temperature and Vibration Insensitive Fiber-Optic Current Sensor” ABB, vol. 2360 pp. 336-339 (Feb. 1994).Applicant
- Burns, et al., “Excess Noise in Fiber Gyroscope Sources”, IEEE Photonics Technology Letter vol. 2, No. 8, Aug. 1990, pp. 606-608.Applicant
- Clark et al., “Application of a PLL and ALL Noise Reduction Process in Optical Sensing System,” IEEE Translations on Industrial Electronics, vol. 44, No. 1, Feb. 1997, pp. 136-138.Applicant
- Dagenais et al., “Low-Frequency Intensity Noise Reduction for Fiber-Optic Sensor Applications,” Optical Fiber Sensors Conference, 1992, Jan. 29-31, pp. 177-180.Applicant
- Dupraz, J.P., “Fiber-Optic Interferometers for Current Measurement: Principles and Technology”, Alsthom Review No. 9:29-44 (Dec. 1987).Applicant
- Frosio, G. and Dändliker, “Reciprocal Reflection Interferometer for a Fiber-Optic Faraday Current Sensor”, Applied Optics 33 (25):6111-6122 (Sep. 1, 1994).Applicant
- Gronai Yuval et al.; “Digital Signal Processing For An Open-Loop Fiber-Optic Gyroscope”, Applied Society of America, Washington, U.S., vol. 34, No. 25, Sep. 1995, pp. 5849-5853.Applicant
- Killian M. Kevin; “Pointing Grade Optic Gyroscope”, IEEE AES Systems Magazine, pp. 6-10 (Jul. 1994).Applicant
- La Violette and Bossler; “Phase Modulation Control for An Interferometric Fiber Optic Gyroscope”, IEEE Plan 90, Position Location and Navigation Symposium, Las Vegas, (Mar. 20-23, 1990).Applicant
- Lefevre, “The Fiber-Optic Gyroscope”, Artech House, Boston, pp. 29-30 (1993).Applicant
- McCallion and Shimazu; “Side Polished Fiber Provides Functionality and Transparency”, Laser Focus World, 34 (9): S19-S24, (Sep. 1, 1998).Applicant
- Moeller and Burns, “1.06μm All-fiber Gyroscope with Noise Subtraction, Proceedings of the Conference on Optical Fiber Sensors”, IEEE-OSA, Moneterey, CA, 1992, pp. 82-85.Applicant
- Moeller and Burns, “Observation of Thermal Noise in a Dynamically Biased Fiber-Optic Gyro”, Optical Letters, 1996, vol. 21, pp. 171-173.Applicant
- Nikos Drakos, “Circular Polarization States for Light, and Quarter-Wave Plates,” Computer Based Learning Unit, University of Leeds (Mar. 2, 1998).Applicant
- Ono et al.; “A Small-Sized, Compact, Open-loop Fibre-Optic Gyroscope with Stabilized Scale Factor”, Meas. Sci. Technol. 1:1078-1083, (1990).Applicant
- Polynkin et al; “All-Optical Noise-Subtraction Scheme for a Fiber-Optic Gyroscope”, Optics Lettes, 25(3): 147-149, (Feb. 1, 2000).Applicant
- Rabelo et al.; “SNR Enhancement of Intensity Noise-Limited FOGs”, Journal of Lightwave Technology 18(12):2146-2150 (Dec. 2000).Applicant
- Short, et al., “Elimination of Birefringence Induced Scale Factor Errors in the In-Line Sagnac Interferometer Current Sensor”, Journal of Lightwave Technology 16 (10):1844-1850 (Oct. 1998).Applicant