Opto-electronic detection device for remotely detecting a physical magnitude

• US 4,867,565 A
• Filed: 11/12/1987
• Issued: 09/19/1989
• Est. Priority Date: 03/13/1986
• Status: Expired due to Fees

• Current Assignee: Bertin & CIE BP N 3 78373 Plaisir Cedex France
• Original Assignee: Bertin & CIE
• Inventors: Lequime, Michel
• Primary Examiner(s): McGraw, Vincent P.
• Assistant Examiner(s): TURNER, SAMUEL A
• Application Number:
  US07/127,900
• Time in Patent Office: 677 Days
• Field of Search: 356/351, 351/346
• US Class Current: 356/453
• CPC Class Codes: G01D 5/344 using polarisation G01D5/35303 takes precedence
• CPC Class Codes: G01K 11/00 Measuring temperature based upon physical or chemical changes not covered by groups G01K3/00, G01K5/00, G01K7/00 or G01K9/00

Abstract

A spectrum modulation encoding sensor subjected to the physical magnitude to be measured is connected by an optical fiber to a source of incoherent light, and by an optical fiber to a static demodulation system comprising a set of birefringent elements producing a birefringence gradient along a privileged optical direction x; the system demodulates the signal provided by the sensor optically by means of a Fourier transform.

Claims

1. An opto-electronic detection device for remotely detecting a physical magnitude, the device comprising:

a source of incoherent light,

an interferometric sensor subjecting the incoherent light from the source to a periodic or quasi-periodic modulation of its spectrum at a frequency which is a function of a magnitude to be measured,

a first optical fiber connecting the source of light to the sensor with the corresponding optical path length difference in the sensor being greater than the coherence length of the source,

a spectrum analyzing means including;

a optical demodulation system essentially constituted by a set of birefringent elements placed between a polarizer and an analyzer which are parallel, for obtaining a birefringence gradient along a privileged optical direction x,

a multipoint linear detector oriented parallel to the privileged optical direction and having a plurality of photosensitive elements, and electronic circuits for acquiring and processing the signals produced by the detector,

the demodulation system performing a Fourier transform of the light modulated by the said magnitude in the sensor, permitting to determine the instantaneous path length difference in the sensor and thus the value of the physical magnitude to be measured, and

a second optical fiber connecting the sensor to the spectrum analyzing means.

2. A device according to claim 1, wherein the sensor comprises collimator optics having the end of the first optical fiber placed at the focus thereof and providing a parallel beam of light striking a sensor polarizer followed by a plate of single axis birefringent material cut parallel to its axis, a sensor analyzer placed downstream from the plate, and output optics having the end of the second optical fiber placed at the focus thereof.

3. A device according to claim 1, wherein the demodulation system comprises collimation optics having the corresponding end of the second fiber placed at the focus thereof and providing a parallel light beam striking the polarizer followed by the birefringent elements, the polarizer and the analyzer being inclined at 45°

relative to the privileged optical direction x.

4. A device according to claim 3, wherein the birefringent elements comprises a prism of the Wollaston type constituted by two elementary birefringent prisms stuck together along a face which is inclined relative to privileged direction x and disposed in crossed manner, connection optics optionally being provided between the analyzer and the detector in order to form an image of the field of interference fringes thereon.

5. A device according to claim 4, wherein the interferometric sensor comprises a plate of birefringent material and the demodulation system comprises also a plate of birefringent material identical to that of the interferometric sensor, placed between the polarizer and the prism with its slow axis being oriented in the same way as the slow axis of the first elementary prism of the Wollaston type prism.

6. A device according to claim 3, wherein the demodulation system comprises two birefringent prisms of the Wollaston type, which prisms are disposed symmetrically about a halfwave plate which is achromatic over the spectrum width of the light source in order to obtain a localization plane for the field of fringes which is parallel to the faces of the prisms.

7. A device according to claim 4, wherein one of the elementary prisms of the Wollaston type prism is cut with an axis that slopes relative to its inlet face.

8. A device according to claim 4, wherein both elementary prisms of the Wollaston type prism are identically oriented and are separated by a halfwave plate placed between their stuck-together faces.

9. A device according to claim 1, 2, 3, 4 or 5 wherein a phase modulation device is disposed between the polarizer and the birefringent elements of the demodulation system.

10. A device according to claim 9, wherein phase modulation device comprises a halfwave plate rotating about the optical axis of the demodulation system, and a fixed quarterwave plate having one of its axes coinciding with the polarization direction associated with the polarizer.

11. A device according to claim 9, wherein the phase modulation device comprises a set of n phase shifting plates with an increment of 2.sub.π

/n, together with means for causing said plates to move successively between the polarizer and the birefringent elements in the demodulation system.

12. A device according to claim 1, 2, 3, 4 or 5 wherein a plurality of spectrum modulation encoding sensors each having a birefringent plate are connected to the source of light by way of the first optical fiber and to the demodulation system by way of the second optical fiber and multiplexed by optical path differences they provide, the device further comprising a set of birefringent plates which are identical to those in the plurality of spectrum modulation encoding sensors and which are placed in the demodulation system between the polarizer and the birefringent elements and which are associated with means for causing the plates to be moved successively between the polarizer and the set of birefringent elements.

13. A device according to claim 12, wherein the birefringent plates are placed in housings in a disk mounted to rotate about an axis which is parallel to the optical axis of the demodulation system, said disk including an empty housing.

14. A device according to claim 12, wherein each birefringent plate is a shared field plate comprising a circular base plate having two semicircular plates of the same thickness at the base plate applied thereto, with one of the semicircular plates having the same orientation as the base plate and the other of the semicircular plates having the opposite orientation, the join line between the two semicircular plates being perpendicular to the privileged optical direction x.

15. A device according to claim 12, wherein each birefringent plate is a semicircular plate whose diametral edge extends radially relative to the optical axis of the demodulation system to lie parallel to the privileged direction x, and in that two multipoint linear detectors are disposed touching each other to analyze the two half fields of interference fringes.

16. A device according to claim 1, 2, 3, 4 or 5 wherein the light source is of modulatable spectrum width and is constituted by superposing a plurality of LEDs having different central wavelengths, with the spectrum width of the source being modulated by adjusting feed currents to the LEDs.