Patent Publication Number: US-7911196-B2

Title: Optical voltage sensor

Description:
RELATED APPLICATION 
     This application claims priority as a continuation application under 35 U.S.C. §120 to PCT/CH2006/00734 filed as an International Application on Dec. 22, 2006 and designating the U.S., the entire content of which is hereby incorporated by reference in its entirety. 
    
    
     FIELD 
     The present disclosure relates to an optical voltage sensor having at least one elongate optical sensing element, such as an optical fiber, for example, and a control unit. The sensing element can be configured to carry at least a first mode and a second mode of light, which are orthogonally polarized. The sensing element can be configured so that the birefringence between the two modes is dependent on the electric voltage to be measured. The control unit can be configured to generate light for the two modes in the sensing element and to measure the phase delay between the two modes. 
     BACKGROUND INFORMATION 
     The present disclosure identifies particular references by numerical designation. The references are specifically identified herein following the detailed description of exemplary embodiments. It has been known to measure voltages using optical means. 
     Some known optical voltage measurement techniques, such as those described in Refs. 1-3 identified below, rely on the piezoelectric effect. In these devices, a field-induced mechanical change in a piezoelectric material leads to stress in an optical sensing element (such as a fiber) that is mechanically coupled to the piezoelectric material. The stress, in turn, leads to a voltage-induced change of birefringence in the sensing element, which can be detected optically. 
     Other known optical voltage measurement techniques, such as that described in Ref. 10 identified below, rely on the electro-optic effect, in which an electric field changes the refractive index or birefringence of a material directly, e.g., through the linear Pockels effect. 
     In both techniques, a measurement of the phase delay (or a change thereof) between two orthogonally polarized light waves allows measurement of the electric field strength, or, more accurately, the integral of the same along the path of the light. 
     It has also been known to measure current by means of similar techniques, see, e.g., Refs. 5-7 identified below, in which a magnetic-field induced phase shift between left and right circularly polarized light waves in a fiber is measured by means of a suitable control unit. 
     SUMMARY 
     According to an exemplary embodiment, an optical voltage sensor is provided. The exemplary optical voltage sensor comprises at least one elongate optical sensing element configured to carry at least a first mode of light and a second mode of light. The modes have substantially orthogonal polarization with respect to each other, and a birefringence between the modes is dependent on an electric voltage to be measured. The exemplary optical voltage sensor also comprises a control unit configured to generate light for said two modes in said sensing element and to measure a phase delay suffered by said two modes due to said birefringence. In addition, the exemplary optical voltage sensor comprises at least one Faraday rotator arranged between said control unit and said sensing element, said at least one Faraday rotator being configured to rotate light by 45° for each pass therethrough. 
    
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
       Further embodiments, advantages and refinements of the present disclosure are explained in more detail below with reference to exemplary embodiments which are illustrated in the drawings, in which like reference symbols are used to denote like elements, and in which: 
         FIG. 1  shows an exemplary first embodiment of a piezoelectric sensor, 
         FIG. 2  shows an exemplary second embodiment of a piezoelectric sensor, 
         FIG. 3  shows an exemplary third embodiment of a piezoelectric sensor, 
         FIG. 4  shows an exemplary fourth embodiment of a piezoelectric sensor, 
         FIG. 5  shows an exemplary first arrangement of the piezoelectric elements, 
         FIG. 6  shows a sectional view along line VI-VI of  FIG. 5   
         FIG. 7  shows an exemplary second arrangement of the piezoelectric elements, 
         FIG. 8  shows a sectional view along line VIII-VIII of  FIG. 5 , 
         FIG. 9  shows an exemplary first embodiment of a electro-optic sensor, 
         FIG. 10  shows an exemplary second embodiment of an electro-optic sensor, and 
         FIG. 11  shows an alternative implementation of the rotator. 
     
    
    
     DETAILED DESCRIPTION 
     Exemplary embodiments of the present disclosure provide a voltage sensor that is configured to measure high voltages in the order of 10 kV or more, and that allows an expedient, accurate and standardized measurement. 
     Exemplary embodiments of the present disclosure are based on the realization that the addition of a Faraday rotator between the control unit and the sensing element allows the functionality of the electro-optic measuring element and its associated components to be converted to the functionality of a conventional magneto-optical current sensor, which in turn allows the use of advanced control units and measuring techniques developed for optical current sensors. 
     In particular, magneto-optical sensors, such as those disclosed in Refs. 5-7 identified below, employ control units that generate a first pair of linearly polarized light waves with orthogonal polarizations and send the first pair of linearly polarized light waves to the sensing equipment. The sensing equipment, in turn, returns the light waves as a second pair of linearly polarized light waves, again with orthogonal but swapped polarization directions, and the phase shift between the light waves of the second pair is a function of the current to be measured. Similarly, the control unit according to exemplary embodiments of the present disclosure can generate a first pair of linearly polarized light waves and send the first pair of linearly polarized light waves to the sensing equipment, which (with the help of the Faraday rotator) returns the light waves as a second pair of linearly polarized light waves, with both light waves being orthogonally polarized and the phase shift between the light waves of the second pair being a function of the voltage or electric field to be measured. 
     According to an exemplary embodiment, the voltage sensor can advantageously comprise at least a first sensing element and a second sensing element arranged in series. The sensing elements can coupled to each other in such a manner that light traveling under the first mode of propagation in the first sensing element is coupled into the second mode of the second sensing element, and vice versa. As described in more detail below, this exemplary configuration allows a series of undesired effects to be compensated and the roundtrip path imbalance of the waves to near zero to be reduced, which thereby allows interference-based measurements even when using a low coherence light source. 
     A low coherence light source, i.e. a light source having a coherence length in the sub-millimeter range (preferably &lt;0.1 mm), is advantageous because light waves generated by polarization cross coupling, e.g. at the fiber splices, interfere incoherently and thus do not deteriorate the sensor performance. 
     According to an exemplary embodiment, the voltage sensor is advantageously based on piezoelectric or electro-optic effects, see Refs. 1-3 identified below. According to an exemplary embodiment, a piezoelectric sensor can comprise a piezoelectric element with a sensing element mechanically mounted thereto such that a change of the voltage generates a stress-induced change of birefringence. The sensing element(s) of such an electro-optic sensor can be made of an electro-optic material whose birefringence changes linearly in the presence of an electric field, such as a material showing a sufficiently strong Pockels effect. 
     The term “sensing element” as employed herein can designate a waveguide, in particular an optical fiber, advantageously having a cross section comparable to the lateral extension of the light field. According to an exemplary embodiment, the waveguide can be polarization maintaining and support a single spatial mode. The mode can be excited with two orthogonal directions of polarization. The term “sensing element” can also designate an element that has a cross section larger than the lateral extension of the optical light field, in which case the (collimated) light beam can propagate substantially freely, i.e. unguided, through the element. 
     The term “mode” as employed herein designates a waveguide mode if the sensing element is used as a waveguide. The term “mode” as employed herein designates a linearly polarizated light beam that propagates through the sensing element unguided substantially without changing its state of polarization if the sensing element is not used as a wave guide. 
     Advantages of exemplary embodiments of the present disclosure will now be described in more detail below with reference to the drawings. 
     Piezo-Electric Voltage Sensors: 
       FIG. 1  shows an exemplary embodiment of a fiber-optic voltage sensor having a control unit  1  and two sensing elements  2  using a piezo-electrically induced birefringence change. 
     The control unit  1  can comprise a light source  3 , a phase modulator  4  for a non-reciprocal phase modulation, a light detector  5 , a signal processor  6 , and a polarization maintaining fiber coupler  7 . The control unit  1  and the sensing elements  2  can form a polarization-rotated reflection interferometer and use an interrogation technique as known from fiber gyroscopes; for details, see Refs. 4 and 5. 
     As illustrated in the exemplary configuration of  FIG. 1 , two orthogonal linearly polarized light waves (indicated by solid and dashed arrows) exit from the control unit  1  and travel through a polarization maintaining (pm) feed fiber  8  (e.g. an elliptical-core fiber) to a Faraday rotator  9  with a rotation angle of 45° per each pass therethrough (or, equivalently, a rotation angle of 45°+k·90° with k being any integer number). In other words, each light wave is rotated by approximately 45° each time it passes through the Faraday rotator  9 . The rotation is non-reciprocal. That is, the rotation as seen from an observer looking towards the light beam is, for example, clockwise if the beam propagates from left to right, but counter-clockwise if the beam propagates from right to left. The total rotation is thus approximately 90° (or 90°+k·180° with k being an integer number). The light waves exiting from the Faraday rotator  9  can be coupled into a first pm sensing fiber  10   a . The fast and slow axes of this sensing fiber  10   a  can oriented at approximately 45° with regard to the axes of the pm feed fiber  8  left of the rotator  9 . As a result, the polarization directions after the rotation can again coincide with the birefringent fiber axes. A second identical pm sensing fiber  10   b  can be spliced at a splice  12  with its axes rotated by approximately 90° with respect to the first sensing fiber  10   a . The waves polarized parallel to slow axis in the first fiber  10   a  can then be polarized along the fast axis in the second fiber  10   b , and vice versa. The waves can be reflected at the end of second fiber  10   b  by a mirror  15 , upon which the waves can then retrace their paths from the mirror  15 . A non-reciprocal Faraday rotator  9  can introduce another 45° rotation that adds to the first rotation. The total rotation on the way forward and backward is thus approximately 90°, i.e. the light waves again return with swapped polarizations to the control unit  1 , as in the current sensor of Ref. 5 identified below. This exemplary configuration is therefore advantageous because it keeps the total roundtrip path imbalance of the waves at or near zero and thus within the coherence length of the low coherent light source  3 . Furthermore temperature and vibration induced optical phase changes in the fiber between the modulator  4  and the Faraday rotator  9  largely cancel each other. Note that on a one way trip through the birefringent fibers  8 ,  10   a ,  10   b , the orthogonal waves accumulate a path difference due to their different group velocities. According to an exemplary embodiment, the path imbalance is 0.5 to 1 mm per meter of fiber at a wavelength of 820 nm. 
     According to the exemplary embodiment illustrated in  FIG. 1 , the two sensing fibers  10   a ,  10   b  to the right of Faraday rotator  9  can function as strain sensors and can be used to measure the periodic piezo-electric deformation of piezoelectric quartz transducer elements  11   a ,  11   b  under the influence of an alternating electric field (see below). The induced fiber strain can cause a differential phase shift between the two orthogonal waves. 
     The two transducer elements  11   a ,  11   b  can be arranged anti-parallel to each other, i.e., their polar axes x (2-fold crystal axis of quartz) are anti-parallel as shown in the example of  FIG. 1 . The phase shifts in the sensing fibers can then be of the same sign if the electric field directions E are the same (as indicated). 
     According to the exemplary embodiment illustrated in  FIG. 1 , the advantages of using a first and a second sensing fiber  10   a ,  10   b  and the transducer elements  11   a ,  11   b  arranged opposite to each other are as follows:
         The second pm sensing fiber  10   b  can balance the optical path imbalance between the two orthogonal waves introduced in the first sensing fiber  10   a . Again, this is necessary to keep the total path imbalance within the coherence length of a low coherent light source.   The second sensing fiber  10   b  can also compensate for thermal phase shifts in the first fiber  10   a  provided that the temperature of the two fibers is about the same. Compensation of large thermal phase shifts is necessary, because more sophisticated signal processing might otherwise be needed. According to an exemplary embodiment, the total phase changes could be designated to remain within an interval of ±π.   The second fiber  10   b  allows doubling of the sensitivity of the voltage sensor and effective cancellation of vibration-induced effects (see below).       

     According to an exemplary embodiment, the polarization-maintaining fibers can be elliptical-core fibers, so-called Panda or bowtie fibers, fibers with inner elliptical cladding, micro-structured fibers, or other types of pm fiber such as those disclosed in Refs. 8 and 9. 
     It should be noted that, with the detection technique according to the exemplary embodiment described above, the effective sensitivity of the two pm sensing fibers  10   a ,  10   b  to alternating strain can vary as a function of the time delay between the forward and backward propagating waves at the location of the strain-applying transducer elements  11   a ,  11   b , and thus as a function of the length of the fibers. The strain-induced phase shift can be at its maximum if the time delay is negligible as compared to the period of the alternating strain. The strain-induced phase shift can become zero if the delay corresponds to half a period of the strain. Furthermore, the effective sensitivities of the two sensing fibers  10   a ,  10   b  can differ from one another if the delay is not negligible. However, for the example considered below, in which a strain periodicity of 50 or 60 Hz and fiber lengths up to some meters is contemplated, the time delay is negligible and the delay effects can be disregarded. 
       FIG. 2  shows an exemplary modification of the configuration illustrated in  FIG. 1 . According to the exemplary embodiment illustrated in  FIG. 2 , a pm fiber coupler  13  and the two pm sensing fibers  10   a ,  10   b  can form a loop mirror. The coupler end at the Faraday rotator  9  can be oriented like the first sensing fiber  10   a  section in  FIG. 1 . The loop can contain two 90°-splices  12 ,  14 . The splices can divide the loop in two halves with identical lengths. An extra reflector is not needed. Two pairs of orthogonal polarizations with orientations as indicated in the example of  FIG. 2  counter-propagate in the loop. The functions of the two loop halves are the same as the ones of the two sensing fibers  10   a ,  10   b  in  FIG. 1 . The phase shifts in the fibers  10   a ,  10   b  add if the crystallographic x-directions and the field directions E are as indicated in  FIG. 2 . A potential advantage of this exemplary configuration is that for a symmetric arrangement of the transducer elements  11   a ,  11   b , the effective sensitivities can always be the same independent of the time delay (while the sensitivities again decrease with increasing delay). 
     The phase modulator  4  in the exemplary configurations illustrated in  FIGS. 1 and 2  is an integrated-optics lithium modulator, see, e.g., Ref. 4 identified below. The modulator can also function as a polarizer. Another alternative is a piezoelectric modulator as illustrated in Ref. 5 identified below. 
       FIG. 3  shows the same exemplary configuration as in  FIG. 1 , except for a different type of integrated-optics phase modulator  4 . According to the exemplary configuration illustrated in  FIG. 3 , the modulator  4  is a birefringence modulator which can directly modulate the phase of orthogonal light waves. The pm coupler  7  of  FIG. 2  is then no longer needed. Depolarized light from light source  3  (depolarizer not shown) can be polarized in a fiber polarizer  21  and subsequently coupled into an entrance pm fiber lead  22  of the modulator at splice  23 , for example. The polarization direction is at approximately 45° to the axes of the pm fiber lead (45° splice). As a result, two orthogonal waves of equal amplitude are excited. The fast and slow axes of both pm fiber leads  22 ,  8  of modulator  4  can be parallel to the electro-optic axes of the modulator. 
     Alternatively, a piezoelectric modulator as illustrated in Ref. 6 identified below may be used as a birefringence modulator. 
       FIG. 4  shows an exemplary implementation of the disclosure based on a Sagnac type interferometer using two Faraday rotators  8 . According to the exemplary embodiment illustrated in  FIG. 4 , there are two counter-propagating waves having parallel polarizations between the modulator  4  and the rotators  8 , and orthogonal polarizations in the first and second pm sensing fibers  10   a ,  10   b  with the transducer elements  11   a ,  11   b . The orientation of the fiber cores at the rotators  8  is as described above. The sensing fibers can both be rotated in the same direction, i.e. both clockwise or both counter-clockwise, with regard to the planes of polarization of the forward traveling waves between modulator  4  and the rotators  8 . The phase shifts in the fibers  10   a ,  10   b  add if the crystallographic x-directions and the field directions E are as indicated in  FIG. 4 . 
       FIGS. 5 and 6  show an exemplary arrangement of a piezo-optic voltage sensor of the type of  FIGS. 1-4  for a line integration of the electric field according to an exemplary embodiment. Only the field sensing part of the sensor is shown, i.e., the two pm sensing fibers  10   a ,  10   b  and the transducer elements  11   a ,  11   b . The transducer elements  11   a ,  11   b  can be identical quartz beams (or platelets), for example, according to Ref. 2 identified below. In the exemplary embodiment illustrated in  FIGS. 5 and 6 , two transducer elements can be assigned to each sensing fiber  10   a ,  10   b . Such transducer elements may be arranged between ground and high-voltage potentials with (equidistant), non-negligible spacing between them or they can form an essentially continuous quartz bridge as shown in the example of  FIG. 5 . In the latter case, the beams can have a length of, e.g., 200 mm and a cross-section of, e.g., 2×2 mm 2 . The measurement of, e.g., 245 kV in high voltage substations may require 10-12 of such quartzes, for example. The longitudinal axis of the beams and the direction of the fiber can coincide with a crystallographic x-direction (2-fold crystal axis). Quartz is a exemplary material for the piezo-electric transducers due to its superior material properties. Others appropriate materials are given in Refs. 1 and 2 identified below. 
     The two sensing fibers  10   a ,  10   b  can, for example, be attached to the transducer elements  11   a ,  11   b  with the 90°-splice  12  at half the distance between ground and high-voltage (Faraday rotator and mirror). The optical phase shifts of the two fiber sections caused by the thermal expansion of the quartzes can then be the same and cancel each other. 
     The x-directions (or polar directions) of the quartzes of a given sensing fiber can point in the same direction. The x-directions along the second sensing fiber  10   b  can be in anti-parallel to the x-directions along the first sensing fiber  10   a . The sign of the optical phase shifts at increasing or decreasing field strength can then be the same at all transducer elements as required for the line integration of the field: The field-induced piezoelectric strains at the two sensing fibers can have opposite signs due to the anti-parallel crystal directions; the two sensing fibers can therefore react to a given change in strain with opposite sign dues to the 90° splice. As a result, the combined effects can have the same sign. The overall phase shift can be a measure for the line integral of the field and thus the voltage. A further benefit of this exemplary arrangement is that optical phase shifts caused by external common-mode mechanical perturbations such as vibrations cancel each other. 
     According to an exemplary embodiment, the sensing fibers  10   a ,  10   b  can have a coating which transmits, over a wide temperature range, such as −40 to 85° C., for example, the entire piezoelectric strain from the quartzes to the sensing fibers (for example, a thin polyimide coating or coating of diamond like carbon (DLC)). According to an exemplary embodiment, the sensing fibers can be attached to the quartzes with some extensional pre-strain. The pre-strain can be sufficiently large so that sufficient strain is still maintained when the quartzes contract at low temperatures. The sensing fibers may be mounted to the quartz surface or to a groove  16  in the surface with an appropriate bonding material. Alternatively, the fiber can be attached in a through-hole along x. 
     The series of quartzes can be attached to a common support structure  17  such as a strip of fiber re-enforced epoxy. The strip can be mounted for mechanical protection in a tube, cable or another enclosure. 
       FIGS. 7 and 8  show another exemplary arrangement in which the sensing elements  2  or sensing fibers  10   a ,  10   b  can be arranged side by side and optically coupled by a 90° splice  12  at neighboring ends  18   a ,  18   b . This exemplary configuration comprises two parallel series of piezoelectric transducer elements  11   a ,  11   b  with axis directions x and a fiber arrangement as indicated. The neighboring transducer elements  11   a  and  11   b  can be mounted to a common support structure  17  as shown in the example of  FIG. 8 . Advantages of this exemplary arrangement are as follows: (i) The sensitivity (optical phase shift per voltage change) is doubled as compared to  FIG. 5 . (ii) Vibration-induced phase changes are cancelled more completely since the two quartz series are very close to each other. (iii) Short wavelength vibrations are still common-mode. 
     Further Alternatives (not Illustrated):
         Instead of two sensing fibers, the sensor can contain three or more sensing fibers spliced at 90° and having lengths such that the total path imbalance of the orthogonal light waves is again zero. The fibers may be of the same or different type.   The sensing fibers can be attached to a series of transducer elements (or several series of transducer elements) such that the fibers pass each series several times, thus enhancing the sensitivity of the sensor.   The quartz beams or platelets can be replaced by quartz cylinders with the sensing fibers attached to the circumferential surface of the cylinders (see Ref. 2 identified below).   Only one sensing fiber can be attached to the transducer elements (quartzes) while the second section only serves for compensation of the path imbalance.       

     Electro-Optic Voltage Sensors: 
       FIG. 9  shows an exemplary electro-optic voltage sensor according to the present disclosure. The first and second sensing fibers  10   a ,  10   b  and the piezoelectric transducer elements  11   a ,  11   b  of  FIG. 1  can be replaced by an electro-optic crystal  19 . A collimator  20  between the 45° Faraday rotator  9  and crystal  19  generates a collimated beam which can be launched into crystal  19 . The beam double passes crystal  19  and is then coupled back into feed fiber  8 . Due to the 45°-rotator  9 , the light waves again return with swapped polarizations. 
     According to an exemplary embodiment, crystal  19  is suitable to line integration of the electric field. Appropriate crystal classes and crystal orientations are listed in Tables 1 and 2 of Ref. 10 identified below. The electro-optic axes of crystal  8  can be aligned at approximately 45° with respect to the birefringent axes of feed fiber  8 . The polarization directions of the orthogonal linearly polarized light waves in crystal  8  can then be parallel to the electro-optic axes. On their roundtrip through crystal  19 , the waves accumulate an electro-optic phase shift proportional to the applied voltage. The roundtrip phase shift can be twice as large as the single pass shift. Advantageously, the crystal belongs to one of the classes of Table 1 in Ref. 10. These crystals can free of any intrinsic birefringence. An exemplary material is Bi 4 (GeO 4 ) 3 (BGO). 
     In case of a birefringent crystal (Table 2), it is advantageous to use a series of two identical crystals  19   a ,  19   b  as shown in the example of  FIG. 10 . The axes of birefringence (which are also the electro-optic axes) of the two crystals  19   a ,  19   b  can have a 90°-offset and the longitudinal axes (a 2-fold axis for the materials of Table 2) can be anti-parallel. The phase shifts from the intrinsic birefringence can then cancel each other while the electro-optic phase shifts add. 
     An electro-optic crystal fiber may be used instead of a bulk electro-optic crystal. The collimator may be omitted in case of a crystalline single-mode fiber. 
     The electro-optic crystal could also be part of a loop mirror configuration according to the exemplary configuration of  FIG. 2  or the exemplary Sagnac configuration illustrated in  FIG. 5 . 
     Instead of using a 45°-Faraday rotator as shown in the preceding exemplary embodiments, the polarization directions of the returning light waves can be rotated by means of two polarization-insensitive optical circulators [ 11 ] as shown in the exemplary configuration of  FIG. 11 . Fibers a and b are again polarization maintaining. The lengths of the various fiber segments are such that the total path difference of the two orthogonal waves is again zero. Fiber b (or fiber a) may include a 90°-splice as indicated to rotate the polarizations. Alternatively, the fibers may be attached to the circulators with axes orientations such that polarization directions of the returning waves are swapped as desired. 
     The use of circulators instead of a simple Faraday rotator offers no advantages and is mentioned here only for the sake of completeness. Note that any circulator contains at least one Faraday rotator. 
     It will be appreciated by those skilled in the art that the present invention can be embodied in other specific forms without departing from the spirit or essential characteristics thereof. The presently disclosed embodiments are therefore considered in all respects to be illustrative and not restricted. The scope of the invention is indicated by the appended claims rather than the foregoing description and all changes that come within the meaning and range and equivalence thereof are intended to be embraced therein. 
     REFERENCES 
     
         
         1. EP 316 635, EP 316 619 
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         3. K. Bohnert, G. de Wit, and J. Nehring, Coherence-tuned Interrogation of a remote elliptical-core, dual-mode fiber strain sensor”, K. Bohnert, G. de Wit, and J. Nehring, J. of Lightwave Technology 13, 94 (1995). 
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         6. K. Bohnert, P. Gabus, J. Nehring, and H. Brändle, “Temperature and vibration insensitive fiber-optic current sensor”,  J. Lightw. Technol ., vol. 20, no. 2, pp. 267-276, 2002. 
         7. K. Bohnert, P. Gabus, H. Brändle, Peter Guggenbach, Fiber-optic dc current sensor for the electro-winning industry”, in 17 th  Int. Conference on Optical Fibre Sensors, Bruges, Belgium, May 23-27, 2005, edited by M. Voet, R. Willsch, W. Ecke, J. Jones, B. Culshaw, Proc. of SPIE Vol. 5855 (SPIE, Bellingham, Wash., 2005) 210-213. 
         8. J. Noda, K. Okamoto, and Y. Sasaki, “Polarization-maintaining fibers and their applications”, J. Lightw. Technol. 4, 1071-1089, 1986. 
         9. A. Orthigosa-Blanch et al., Highly birefringent photonic crystal fibers, Optics Letters 25, 1325, 2000. 
         10. EP 682 261 
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     LIST OF REFERENCE NUMERALS 
     
         
           1 : control unit 
           2 : sensing element 
           3 : light source 
           4 : phase modulator 
           5 : light detector 
           6 : signal processor 
           7 : pm fiber coupler 
           8 : feed fiber 
           9 : Faraday rotator 
           10   a ,  10   b : sensing fibers 
           11   a ,  11   b : piezoelectric transducer elements 
           12 : 90° splice 
           13 : pm fiber coupler 
           14 : 90° splice 
           15 : mirror 
           16 : groove 
           17 : support 
           18 : sensing fiber ends 
           19 ,  19   a ,  19   b : electro-optic crystals 
           20 : collimator 
           21 : fiber polarizer 
           22 : pm fiber lead 
           23 : splice