Ellipsoidal optical coupling device

• US 4,422,714 A
• Filed: 03/17/1981
• Issued: 12/27/1983
• Est. Priority Date: 09/14/1979
• Status: Expired due to Fees

• Current Assignee: Cables Cortaillod SA
• Original Assignee: Cables Cortaillod SA
• Inventors: Widmer, Gilbert, Benoit, Pierre, Pellaux, Jean-Paul, Coche, Andre, Kerllenevich, Betty
• Primary Examiner(s): Lee, John D.
• Application Number:
  US06/245,647
• Time in Patent Office: 1,015 Days
• Field of Search: 350/96.15, 350/96.16, 350/96.18, 350/96.19, 350/3.72, 350/330, 350/331 R, 350/350 R, 350/314, 350/315, 356/135, 356/136, 356/137, 250/577
• US Class Current: 385/39
• CPC Class Codes: G01N 21/431 Dip refractometers, e.g. using optical fibres
• CPC Class Codes: G02B 6/264 with optical elements between opposed fibre ends which perform a function other than beam splitting having lens focusing means G02B6/32; utilising prism or grating G02B6/34
• CPC Class Codes: G02B 6/3522 the optical element enabling or impairing total internal reflection using evanescent coupling G02B6/3536
• CPC Class Codes: G02B 6/3532 the optical element being a wavelength independent filter or having spatially dependent transmission properties, e.g. neutral filter or neutral density wedge substrate with plurality of density filters
• CPC Class Codes: G02B 6/3534 the optical element being diffractive, i.e. a grating
• CPC Class Codes: G02B 6/3558 1xN switch, i.e. one input and a selectable single output of N possible outputs
• CPC Class Codes: G02B 6/3594 Characterised by additional functional means, e.g. means for variably attenuating or branching or means for switching differently polarized beams
• CPC Class Codes: G02F 1/1326 Liquid crystal optical waveguides or liquid crystal cells specially adapted for gating or modulating between optical waveguides
• CPC Class Codes: Y10S 250/903 with prism contacting liquid

Abstract

An optical coupling device wherein at least two light conductors are coupled through the intermediary of a transparent block in the shape of a half-ellipsoid on whose foci converge the end sections of the two light conductors. A light beam emerging from one conductor is reflected and transforms itself into a beam converging on the end of the second conductor. A slot permits the introduction of a liquid-crystal attenuating device connected to an alternating voltage source.

Claims

1. An optical coupling device for at least two light conductors, comprising a solid body at least a part of which consists of a half-ellipsoid of revolution made of a material transparent at least in the wavelength range of the light transmitted by these light conductors, the outer surface of said half-ellipsoid being placed in an ambient medium, means for positioning the end of one of said light conductors at one of the foci of said half-ellipsoid, second means for positioning the end of a second light conductor at the other focus of said half-ellipsoid, said positioning means orienting the optical axes of the two conductors whose ends have been placed at the foci of the half-ellipsoid in such a way that a divergent light beam emitted by one of these conductors is transformed, after having undergone a total reflection inside said half-ellipsoid, at the interface between said half-ellipsoid and said ambient medium into a beam converging on the end of the other conductor, said half-ellipsoid including a slot formed therein to permit the interposition along the path of said convergent beam of beam modifying means operative to modify a light beam transmitted through said half-ellipsoid.

2. An optical coupling device according to claim 1 wherein said positioning means include a base piece joined to said half-ellipsoid in the median plane containing the foci of the generating ellipse of said half-ellipsoid, and at least two light conductors having their ends embedded in said base piece.

3. An optical coupling device according to claim 1 wherein said slot is substantially perpendicular to the direction of a median ray of said convergent beam.

4. An optical coupling device according to claim 1 wherein said beam modifying means comprises at least one intensity filter.

5. An optical coupling device according to claim 4 wherein said beam modifying means is placed in a slot cut into said half-ellipsoid parallel to the median base plane of said half-ellipsoid.

6. An optical coupling device according to claim 5 wherein said beam modifying means includes a disk having a plurality of regions having, with respect to each other, different light absorption properties, said disk being rotatable around an axis perpendicular to the median base plane of said half-ellipsoid whereby different regions of the disk can be placed successively inside said slot.

7. An optical coupling device according to claim 1 wherein said beam modifying means comprises at least one holographic lens.

8. An optical coupling device according to claim 7 wherein said holographic lens is positioned in a slot cut into said half-ellipsoid, parallel to the median base plane of said half-ellipsoid.

9. An optical coupling device according to claim 7 wherein said holographic lens is designed in such a way that the zero order of diffraction of the holographic lens reconstitutes a first light beam converging toward the end of one light conductor placed at a focus of the ellipse generating said half-ellipsoid, while the first order of diffraction reconstitutes a second light beam converging toward the end of another light conductor.

10. An optical coupling device according to claim 1 wherein said beam modifying means comprises a liquid-crystal light-attenuating device.

11. An optical coupling device according to claim 10 wherein said light-attenuating device includes a liquid-crystal layer formed between two transparent plates made conductive along their inner faces in contact with the liquid crystal, and electric power means for applying a potential difference between said conductive opposite faces.

12. An optical coupling device according to claim 11 wherein said electric power means provides an alternating potential.

13. An optical coupling device according to claim 11 wherein said two plates are metallized on their inner faces.

14. An optical coupling device according to claim 11 wherein said two plates are made conductive utilizing a material selected from the group:

indium oxide and tin oxide.

15. An optical coupling device according to claim 11 wherein said liquid-crystal layer includes nematic substances.

16. An optical coupling device according to claim 15 wherein the light transmitted is a polarized light, said liquid crystal layer being sensitive to polarized light to undergo a torsion so that the orientations of the molecules at the level of the respective transparent plates are perpendicular.

17. Use of the device according to any one of the claims 10 to 15, as a means of subduing the light transmitted by the device.

18. Use of the device according to claim 17, as an electro-optical switch.

19. Use of the device according to claim 1, in order to detect a variation in the medium with which the convex face of the half-ellipsoid of revolution is in contact, wherein the light intensity transmitted by the optical coupling device is measured, from the end of one of the light conductors to the end of the other light conductor, before and after variation of the medium while at the same time maintaining the intensity of the incident light.

20. Use according to claim 19, in the case where the said variation, in the medium in contact with the convex face of the half-ellipsoid, results in the variation of the level of a liquid, wherein, after having placed the median base plane of the half-ellipsoid in a vertical position, at least one measure of light intensity corresponding to a level of the liquid is effected, such as the field of the convex face of the half-ellipsoid, on which total reflection is effected of the said divergent light beam, is a least partially immersed in the liquid.

21. Use according to claim 19, wherein the said light intensity measure is effected in a continuous manner, by recording the development, as a function of time, of the values of the light intensity transmitted by the coupling device.

22. Use according to claim 19, in the case where the said variation, in the medium in contact with the convex face of the half-ellipsoid, results in the presence of a gas in a liquid, wherein measures of light intensity are effected after having placed the half-ellipsoid of revolution, with its median plane in a horizontal position, inside a capsule where the gas is collected, this capsule having an internal volume corresponding to the gas volume to be detected.