Polarimetric directional field sensor

Abstract: A polarimetric directional field sensor comprises an emitter and receiver (1) of measurement signals, connected by optical fibres (2, 2a, 2b) to a portable probe (3). The probe (3) comprises an optical element (11, 13) sensitive to the field to be measured and means (9, 20) for polarizing the measurement signal. The optically sensitive element (11,13) is in the form of a birefringent crystal having a crystalline structure which provides at least one plane in which the induced birefringence is modified by a single component of the field to be measured. The crystal is cut and oriented in the probe so that the direction of propagation of the optical measurement signal inside the crystal is normal to this plane, the polarizing means (9, 20) being oriented at 45° to the orthogonal axes in which the crystal's refractive indices are modified by the desired component of the field.

Description: The present invention relates to a polarimetric field sensor. For the measurement of fields, particularly electric or magnetic fields, polarimetric optical sensors may be used. Such sensors exploit the changes in the state of polarization in birefringent crystals of an optical signal transmitted through them. Such sensors are especially useful because the sensitive element, or probe, can be very small and can be made from dielectric material, so that the field is not affected and safety is not compromised in the presence of high-voltage conductors or the like. Known sensors, on the other hand, although being sufficiently accurate in measuring field intensity at the point where the probe is located, are not capable of providing adequate information about the direction of the field, that is, they are not capable of detecting and providing information about the intensity of the field in one or more directions relative to the position of the probe. Whilst it is possible, from the measured value and following an appropriate calibration, to obtain the actual distribution of the field in the case of a well-defined field configuration, and for a given location of the probe, in the case of a substantially unknown field configuration such as in the proximity of a charged body having an irregular shape or with an irregular charge distribution, the sensor does not provide sufficient information to define the field. It has been indicated the advantage to provide a directional sensor capable of detecting only one component of an electric field to be measured in a well-defined direction, without such measurement being influenced by the other components of the field in an article entitled "Electromagnetic field components: their measurement using linear electrooptic and magnetooptic effects" published in "Applied Optics" vol 14, N° 11, pages 2712-2719 on November 1975. The measure of two components of an electric field has been indicated in the article entitled "Simultaneous measurement of two orthogonal components of electric field using a Pockels device" published on July 1989 in the "Review of scientific instruments" vol 60, N° 7, pages 1252-1257. According to this publication, see the figure 5 at page 1255, the light beam exiting from the electro-optical crystal is divided into two beams and each beam is made to pass in its own analyzer. Each one of the two light beams exiting from the electro-optic crystal mainly contains the information concerning one of the two electric components of the electric field. This means that in case of strong electric fields the two components are reciprocally influenced so that no precise measures are obtained. A known solution able to measure three components of an unknown electric field is described in the European Patent 453.693 (published 30.10.91) but for obtaining this a spherical configuration is to be imparted to the electro-optical crystal and only crystals having cubic crystallographic symmetry must be used. The object of the present invention is to identify the characteristics of a sensor capable of accomplishing a precise directional measurement, even in case of strong electric field, of the three components of the same without incurring in the limitation of the known devices. According to the present invention there is provided a polarimetric directional field sensor, comprising a measurement signal emitter, a measurement signal receiver, a probe, optical fibres connecting the probe to the emitter and to the receiver, wherein the probe comprises an electro-optical crystal for modifying the state of polarization of the optical signals transmitted therethrough in the presence of a field to be measured, the fibers transmitting into the crystal and receiving therefrom independent optical measurement signals, and means for polarizing the measurement signals, characterized in that the electro-optical crystal has a crystalline structure which provides three incident planes in each of which the change of the refraction characteristics along two orthogonal axes lying in the same plane is caused to be measured by a single component of the field independent of the other components of the field, said probe comprising a casing inside which are housed the ends of three optical fibres, with respective means of collimation, one of which fibres is oriented orthogonally to one of the cutting planes of the electro-optical crystal and the other fibres are parallel to said one fibre and aligned with respective prisms for deviating the optical signals transmitted thereby towards the corresponding planes of the crystal, the three planes of the crystal to which the optical signals are directed being mutually orthogonal, and that the polarizing means are oriented at 45° to the orthogonal axes along which the crystal's refractive indices are modified by the desired component of the field. The dependent claims refer to particular embodiments of the invention. Greater details may be obtained from the following detailed description, with reference to the enclosed drawings, in which there are shown : in Fig, 1 a schematic representation of an electric field transmission polarimetric sensor; in Fig. 2 schematic representation of an electric field reflection polarimetric sensor; in Fig. 3 the probe of the sensor of Fig. 2, partially in a cross-sectional view; in Fig. 4 the elements of the probe of a sensor represented in an exploded drawing, with the orientation of the components in accordance with a first embodiment of the invention; in Fig. 5 the elements of the probe of the sensor represented in an exploded drawing, with the orientation of the components in accordance with a second embodiment of the invention; in Fig. 6 the elements of the probe of the sensor represented in an exploded drawing, with the orientation of the components in accordance with a third embodiment of the invention; in Fig. 7 a side view of the probe of a sensor sensitive to several components of the field; in Fig. 8 a perspective view of the probe sensitive to three components of the field. As shown in Fig. 1, a polarimetric electric field sensor comprises a device 1 for emitting and receiving an optical measurement signal, connected by optical fibres 2 to a probe 3, to be positioned in an electric field E generated by external configuration of charged bodies 4. The device 1 comprises a light source for transmitting an optical signal, via an outward optical fibre 2a to the probe 3; the optical signal is polarized in the probe by means of a first polarizer and then passes through an electro-optical crystal and a second polarizer and then into a return fibre 2b. If the outward and return fibres 2a, 2b are of the type which maintain the polarization, the polarizers may alternatively be remote, that is, located within the device 1 or in any case at a distance from the probe; such an arrangement is practicable provided there is no danger that the state of polarization of the signal is not altered by undesirable external effects acting on the fibres, such as to limit the accuracy of the measurement. Such effects might occur, for example, if the fibres are of considerable length. As a result of the electro-optical effect, the polarization characteristics of the signal transmitted through the crystal are modified by the electrical field, and the signal is then transmitted, via the return fibre 2b, to the device 1, where changes in intensity of the return signal, arising from changes in the state of polarization introduced by the field, are analysed so that the value of the electric field E may be obtained. In an alternative embodiment, illustrated in Fig. 2, the probe crystal is provided with a reflective coating at the end face opposite that at which the optical signal is introduced. The signal is transmitted to the probe via an optical fibre 2 and polarized by a polarizer, transmitted through the crystal and reflected; the measurement signal again passes through the crystal and the polarizer in the opposite direction and returns to the device 1 through the same optical fibre 2 in which the signal was transmitted to the probe. The return signal may be separated within the device 1 and thus analysed in a manner similar to that described above. As illustrated in Figs. 1 and 2, the axis a of the probe 3 can be oriented freely with respect to the direction of the electric field E; in addition, the components of the probe, as discussed below, in turn have an orientation and exhibit an anisotropic behaviour. An example of the structure of the probe 3 is illustrated in greater detail in Fig. 3, in the case of a probe operating by reflection; it comprises a casing 5, suitably formed by two portions 5a, 5b, to which is connected an optical fibre 2, housed in a corresponding sheath 6. The end of the fibre 2 is inserted into a supporting ferrule 7 which in turn faces a focusing lens 8. On the other side of the lens 8 there is provided in sequence a polarizer 9, a delay plate 10 and a crystal 11, provided with a reflecting coating 12 on its end face. In order to make the probe sensitive to a single component of the field, the crystal 11 is a directional electro-optical crystal, that is, it has a crystalline structure which provides at least one plane in which the single field component causes a change in the refraction characteristics along two orthogonal axes lying in the plane. Such a crystal is, moreover, cut and oriented inside the probe so that the direction of the propagation of the measurement signal inside it, as indicated in Figs. 4, 5, and 6, is normal to the plane mentioned above. Such a condition is identified by making reference to the main optical x-y-z axes of the crystalline materials used. As is known, such axes are the axes along which the fields E and D of an electromagnetic wave which is propagated in the crystal are parallel; they form an orthogonal 3-axis system and are always unambiguously defined in any anisotropic material. The crystals which satisfy the above condition may be identified by their having a particular crystal structure and by their belonging to a particular given symmetry group, identified according to international convention. Crystals suitable for the purpose can be selected from: monoclinic crystals: class 2 y-cut and z-cut; orthorhombic: class 222 x-cut, y-cut, z-cut and class 2mm z-cut; tetragonal: class 4 z-cut, class 4 z-cut, class 422 x-cut and y-cut, class 4mm z-cut, class 4 2m x-cut, y-cut or z-cut; rhombohedral: class 32 x-cut; hexagonal: class 622 x-cut or y-cut, class 6 m2 x-cut or y-cut; cubic: class 4 3m x-cut, y-cut or z-cut and class 23 x-cut, y-cut or z-cut. The indicated cutting planes (x-cut, y-cut, z-cut) are the planes for which the corresponding direction of optical propagation is normal to the plane, and the crystals must be oriented inside the sensor so that the arrangement of such planes is appropriate in relation to the direction of the measurement light. For the cubic crystals mentioned above the cutting plane, that is the plane containing the face 11a and on which the optical measurement signal is made to impinge orthogonally, can be normal to any of the x-, y- or z-directions (that is, it is a plane having Miller indices (100), (010), (001), respectively), while for the tetragonal crystals in classes 4, 4 and 4mm only the z-plane is acceptable; in class 422 the planes x and y, and in class 4 2m the planes x, y and z are acceptable. With the orthorhombic crystals in class 222 the acceptable cutting planes are those defined by the three directions x, y and z, while in class 2mm only the plane normal to the z-direction is acceptable; for rhombohedral crystals the cutting plane which may be used is the plane normal to the x-axis; for hexagonal crystals the plane normal to the x- or the y-axis and for monoclinic crystals the plane normal to the y- or the z-axis is acceptable. Among the above-mentioned crystalline groups the following are preferred: Monoclinic: class 2: Ca₂Nb₂O₇ Orthorhombic: class 222: KNa(C₄H₄O₆).H₂O (Rochelle salts) class 2mm: LiB₃O₅, KB₅O₈.H₂O and isomorphous compounds Tetragonal: class 4mm: BaTiO₃; class 4 2m: KH₂PO₄ and isomorphous compounds (also known as KDP) Rhombohedral: class 32: SiO₂ (quartz) Hexagonal: class 6 m2: GaSe, α-ZnS, CdS, CdSe Cubic: class 23: Bi₁₂GeO₂₀ and isomorphous compounds class 4 3m: Bi₄Ge₃O₁₂ and isomorphous compounds; CdTe, GaAs ,GaP, β-ZnS, ZnTe, CuCl, CuBr. Crystals suitable for use in the probe are crystals exhibiting the required conditions and which must also be substantially transparent to light having the wavelength used for the measurement signal. Thus the crystals should preferably have a half-length of the luminous intensity inside them not less than the length of the optical path within the crystal in the probe; in some applications, however, crystals with an attenuation higher than this value may be used, provided the output intensity of the crystal is sufficient for the measurement. As an example, an x-cut cubic crystal is represented diagrammatically in Fig. 4, wherein the cutting plane 11a is normal to the x-direction and the direction of propagation of the signal is parallel to the x-axis. In combination with such a crystal 11, the polarizer 9 is arranged with the polarization axis, indicated by the arrow P, oriented in a direction parallel to the z- or y-axis, that is, at 45° to the orthogonal axes along which the refraction indices of crystal 11 are modified by the desired component E x of the electric field. In the case of a cubic crystal, a y-cut or z-cut crystal would be appropriate for the measurement of the field component parallel to the corresponding y or z direction of propagation of light in the crystal. As an alternative, using for example a GaSe crystal (hexagonal 6 m2), with m perpendicular to the y-axis and with the direction of the propagation of the light in the crystal parallel to y (y-cut), as illustrated in Fig. 5, it is possible to measure the x-component (E x ) of the field, normal to the propagation direction, by arranging the polarizer with the polarization axis P oriented at 45° to x and z. Such a configuration is useful, for example, where the shape of the probe presents problems in its positioning in the measurement area, since its sensitivity in the direction orthogonal to the larger dimension of the probe can be exploited. In a further example, illustrated in Fig. 6, a crystal of quartz (SiO₂) (rhombohedral, class 32), or gallium selenide (GaSe) (hexagonal, class 6 m2) is used; in either case the end face 11a is perpendicular to the x-axis, that is, the crystal is x-cut. The polarizer 9 is arranged with the polarization axis P at 45° to the y- and z-axes; the field component measured is the component E x , along the x-axis. The delay plate 10 serves to introduce a phase shift between two orthogonal polarizations and is used with its birefringence axes at 45° to the polarization plane. The response of the sensor is dependent on the phase shift produced by the plate and thus, by means of the plate 10, it is possible to impart a constant phase shift, which is added to the variable shift introduced by the measured electric field, which will permit operation near a desired value of electric field, such as in a linear area of the response curve. In view of the substantially cosinusoidal shape of the response curve of a polarimetric probe, if it desired to operate in a linear response region near a zero average value of the field, the shift to be introduced is equal to one quarter wavelength; in the reflection probe of Figs. 2 and 3 the plate 10 is traversed twice by the measurement signal, and it is thus arranged to produce a shift of one eighth of a wavelength for each passage, so that, after two successive passages, the over-all phase shift is the desired quarter wavelength. In the non-reflective sensor of Fig. 1, wherein the delay plate 10 is traversed only once by the measurement signal, in order to operate near a zero field value, a plate providing a phase shift of a quarter wavelength is used. In cases where the probe has to operate in the presence of different field values, the material and the thickness of the delay plate is selected so as to obtain the desired phase shift in accordance with known techniques. The delay plate, irrespective of the phase shift, is formed from birefringent material; in order to obtain a directional sensor such a plate is formed either from non-electro-optical anisotropic birefringent material, e.g. mica, with two axes of linear birefringence perpendicular to the direction of propagation and at 45° to the axis of polarization, or from an electro-optical anisotropic birefringent material, whose birefringence characteristics are modified by the same field component (and only by that one) which has an effect on the probe crystal. When the plate is formed from non-electro-optical material, its orientation has no influence on the directionality of the sensor. When, on the other hand, an electro-optical material is used, this may be selected from the following crystalline classes: Tetragonal: class 4 and 4 (z-cut) Orthorhombic: class 2mm (z-cut) Rhombohedral: class 32 (x-cut) Hexagonal: class 6 m2 (x-cut or y-cut). A preferred material for the delay plate is x-cut quartz. Birefringence induced on the x-cut quartz by an electric field E in the x-direction produces a variation in the refractive indices of the main axes y, z which thus produces a phase delay modulated by the electric field; if the main axes of a delay plate of such material are parallel to the induced birefringence axes of the sensitive crystal 11 such phase delay is added to that produced by the field itself on the crystal, contributing to the sensitivity of the probe in the desired direction, without other field components being detected. For such conditions, the plate is oriented with its birefringence axes at 45° to the axis of polarization P. For crystals 11 which measure the field component in the direction of propagation of the optical measurement signal and in which the induced birefringence is at 45° to the axes, the y- and z axes of the quartz delay plate must be oriented at 45° to the main optical axes of the crystal 11, such as, for example, in the case of the cubic crystal represented in Fig. 4. In the case where the induced birefringence is along the main axes (Fig. 6) the axes of the delay plate must be aligned with these and the axis P of the polarizer must be at 45° to both (say, with GaSe x-cut). The use of a probe containing a delay plate with a different orientation or with materials other than those discussed above, introduces a directionality defect in the sensor, that is, a sensitivity to field components in addition to the one desired, which may range from 10% to 100% of the desired component itself; thus for many uses, such as the measurement of the field configuration around a high-voltage body or device, in which not only the magnitude of the field but also its direction is unknown, it is appropriate that the delay plate also satisfy the above criteria of directionality, since an error in the measurement could lead to unacceptable results. As illustrated in Fig. 3, a sensor suitable for measuring a component of the electric field has been fabricated using a crystal of bismuth germanate (Bi₄Ge₃O₁₂, cubic, class 4 3m, also known as BGO), having a prismatic shape of length 10 mm and cross-section 3x3 mm; the crystal has been cut so that the larger dimension is in the z-direction, while the smaller sides are in the x- and y-directions (referred to the main optical axes), as highlighted by the reference axes in the figure. The measurement signal is transmitted into the crystal along the z-direction of the crystal. The delay plate is made from x-cut quartz of 1 mm thickness and a cross-section of 3x3 mm; the y- and z-axes of the plate are at 45° to the x- and y-axes of the BGO crystal. The polarizer is made from glass of 1 mm thickness and a cross-section of 3x3 mm; the polarization axis is parallel to one of the x- or y-axes of the BGO crystal (at 45° to the y- and z-axes of the quartz plate). The light constituting the measurement signal is transmitted to the probe via a fibre 2 of the multimode 50/125 type and is focused by a lens 8 having a variable refractive index and a diameter of 2 mm. The probe casing is made entirely from dielectric material. The sensitivity of the probe is such that it is possible, in combination with suitable known emission, reception and signal processing devices to measure electric fields in air ranging from a few V/mm to a few kV/mm, at frequencies ranging from that of the mains voltage (< 50 Hz) to atmospheric impulses (> 500 kHz), with a directional error of less than 1%. A probe of the above structure is thus sensitive to a single field component, parallel or normal to the direction of propagation of the optical measurement signal, which conveniently coincides with the probe's longitudinal axis; thus if the probe itself is placed in an unknown electric field and oriented in a pre-determined direction, it is possible to obtain an indication of the component of the electric field in that direction. If the probe is subsequently oriented in another direction, or if it is placed in a new position, it is then possible to measure the field in such new direction or position, until the configuration of the desired field is established, in relation to the specific measurement requirements. Where it is desired to establish simultaneously, with a single probe, the value of all the vector components of the field, it is convenient to use a probe of the type shown in Fig. 7 in side view and exploded in Fig. 8: in such a probe an electro-optical crystal 13, having a cubic shape, receives from three independent fibres 14, 15, 16 respective measurement signals at three mutually orthogonal faces; each fibre is housed in a respective ferrule 17 and the emergent beam of light is collimated by a respective lens 18. In order for the fibres 14, 15, 16 to be parallel to one another at their points of connection to the probe, two of them may conveniently be provided with a respective prism 19, suitable for deviating the beam of light through 90°. There is thus in the optical path of the signal emitted by each fibre a respective polarizer 20 and a delay plate 21, while the faces of the crystal 13 opposite to the ones receiving the measurement signals are provided with respective reflective coatings 22. With such a structure there are measurement signals in the three directions inside the crystal 13, whereby it is possible to obtain the complete configuration of the field, using a probe having particularly small dimensions, but which introduces limited disturbances into the measured field and which also measures the three components at a single point, thus ensuring the necessary accuracy. In order to perform the measurement in the three directions the crystal 13 must be an electro-optical crystal: (i) which is transparent at the wavelength(s) of the measurement signals, as described above; (ii) for which there exist three mutually orthogonal directions; and (iii) for which the condition of directionality obtains, so that the crystalline structure provides for each such direction a corresponding plane in which the modification of the refraction characteristics along two orthogonal axes lying in the plane is caused by only one component of the field, so that for each direction of propagation three independent field components are measured. Crystals suitable for the purpose are: Cubic: class 4 3m and 23 (x-cut, y-cut, z-cut) Orthorhombic: class 222 (x-cut, y-cut, z-cut) Tetragonal: class 4 2m (x-cut, y-cut, z-cut) Preferably crystals for three-directional sensors are cubic crystals of classes 4 3m and 23; such crystals are not naturally birefringent and have equal sensitivity along the three axes. If measurements of only two field vector components are desired, that is if a two-directional probe is desired, the probe can have a structure similar to that represented, and the same materials may be used for the crystals 13, but with one of the fibres and the corresponding polarizer and delay plate removed. In all such one-, two- or three-directional sensors, the crystal's cutting plane preferably has a tolerance lower than 5/10ths of a degree with respect to the theoretical crystallographic plane, and an equal tolerance is required for the direction of incidence of the optical signal with respect to such plane; this ensures an error in the measurement of directionality of the order of 1 to 2%, that is the sensitivity to field components other than the desired one is equal to 1 to 2% of the sensitivity in the correct direction, which is acceptable for the majority of uses without imposing undue difficulties in the manufacture of the crystal. In order to obtain greater measurement accuracy, with a directionality error of less than 0.1 to 0.3%, a cutting tolerance of the surface and of the optical signal's angle of incidence such as to admit an angular error of less than 6' must be adopted. For the axis of polarization of polarizer 9 a modest error of inclination does not affect directionality to an appreciable extent; a commonly applied tolerance value ranges from 0.1° to 1°. Many variations of the above sensors may be introduced, without departing from the scope of the present invention.

Claims: A polarimetric directional field sensor, comprising a measurement signal emitter (1), a measurement signal receiver (1), a probe (3), optical fibres (2, 2a, 2b; 14, 15, 16) connecting the probe (3) to the emitter (1) and to the receiver (1), wherein the probe (3) comprises an electro-optical crystal (11, 13) for modifying the state of polarization of the optical signals transmitted therethrough in the presence of a field to be measured, the fibres (14, 15, 16) transmitting into the crystal (11, 13) and receiving therefrom independent optical measurement signals, and means (9, 20) for polarizing the measurement signals, characterized in that the electro-optical crystal (11, 13) has a crystalline structure which provides three incident planes in each of which the change of the refraction characteristics along two orthogonal axes lying in the same plane is caused to be measured by a single component of the field independent of the other components of the field, said probe (3) comprising a casing inside which are housed the ends of three optical fibres (14, 15, 16), with respective means (18) of collimation, one of which fibres is oriented orthogonally to one of the cutting planes of the electro-optical crystal (11, 13) and the other fibres are parallel to said one fibre and aligned with respective prisms (19) for deviating the optical signals transmitted thereby towards the corresponding planes of the crystal (11, 13), the three planes of the crystal (11, 13) to which the optical signals are directed being mutually orthogonal, and that the polarizing means (9, 20) are oriented at 45° to the orthogonal axes along which the crystal's refractive indices are modified by the desired component of the field. A polarimetric directional field sensor according to claim 1, characterized in that the electro-optical crystal is selected from crystals: cubic: classes 4 3m and 23 x-cut, y-cut or z-cut; orthorhombic: class 222 x-cut, y-cut or z-cut; tetragonal: class 4 2m x-cut, y-cut or z-cut; with the corresponding cutting planes oriented orthogonally to the direction of propagation of the optical measurement signal inside the crystal (11, 13). A polarimetric directional field sensor according to claim 2, characterized in that the electro-optical crystal (11, 13) is a cubic crystal of the class 4 3m or 23. A polarimetric directional field sensor according to claim 1, characterized in that the probe comprises delay plates (21) made from birefringent material and positioned in the path of the optical measurement signals, and arranged for imparting a constant predetermined phase shift between two orthogonal polarizations of the optical measurement signals, each delay plate (21) being oriented with its optical birefringence axes substantially at 45° to the plane of polarization. A polarimetric directional field sensor according to claim 4, characterized in that the delay plate (21) is formed from non-electro-optical birefringent material. A polarimetric directional field sensor according to claim 4, characterized in that the delay plate (21) is made from electro-optical birefringent material and is oriented so that its birefringence characteristics are changed by the same field component to which the electro-optical crystal (11, 13) is sensitive. A polarimetric directional field sensor according to claim 6, characterized in that the delay plate (21) is made from electro-optical anisotropic birefringent material, selected from crystals: tetragonal: class 4 and 4 , z-cut; orthorhombic: class 2mm, z-cut; rhombohedral: class 32, x-cut; hexagonal: class 6 m2, x-cut, y-cut. A polarimetric directional field sensor according to claim 7, characterized in that the material is x-cut quartz. A polarimetric directional field sensor according to claim 6, characterized in that the crystal (11, 13) has a birefringence induced at 45° to the main optical axes and the optical measurement signal or each optical measurement signal is propagated parallel to the component or to the components of the field to be measured, and the delay plate (21) is oriented with the y- and z-axes at 45° to the main optical axes of the birefringent crystal (11, 13). A polarimetric directional field sensor according to claim 6, characterized in that the crystal (11, 13) has a birefringence induced along its main optical axes and the delay plate (21) is oriented with the y- and z-axes along the main optical axes of the birefringent crystal. A polarimetric directional field sensor according to claim 1, characterized in that the cutting plane of the electro-optical crystal (11, 13) has an orientational tolerance of less than 5/10ths of a degree with respect to the prescribed theoretical plane. A polarimetric directional field sensor according to claim 11, characterized in that the cutting plane of the electro-optical crystal (11, 13) has an orientational tolerance of less than 6' with respect to the prescribed theoretical plane. A polarimetric directional field sensor according to claim 1, characterized in that the plane of polarization has an orientational tolerance of less than 1° with respect to the prescribed theoretical plane.

Inventors: SIMONELLI FRANCESCO, SIMONELLI, FRANCESCO
Applicants: PIRELLI CAVI SPA, PIRELLI CAVI S.P.A.
Application year: 1991
Main classification: G01R29
IPC codes: G01R29, G01R1