Fiber-optic luminescence sensor utilizing interference in a thin layer structure

• US 4,581,530 A
• Filed: 11/21/1983
• Issued: 04/08/1986
• Est. Priority Date: 11/22/1982
• Status: Expired due to Fees

• Current Assignee: ASEA AB Vasteras Sweden
• Original Assignee: Asea Aktiebolag (ABB Limited)
• Inventors: Brogardh, Torgny, Hok, Bertil, Ovren, Christer
• Primary Examiner(s): Westin, Edward P.
• Application Number:
  US06/554,058
• Time in Patent Office: 869 Days
• Field of Search: 250/227, 250/231 R, 250/231 P, 350/96.15, 350/96.20, 350/96.29, 73/705, 73/655, 73/800, 356/32, 356/35.5
• US Class Current: 250/227.21
• CPC Class Codes: G01D 5/268 using optical fibres G01D5/28 - G01D5/38 take precedence

Abstract

A fiber-optic sensor for measuring a physical quantity or sensing changes therein, consists of a transmitter and receiver unit respectively arranged to transmit and receive optical energy and an optical fiber for transmission of said optical energy to and from a sensor located at the measurement point. The sensor has at least one solid body, which is arranged to emit photoluminescent optical energy in at least one wavelength range, and a volume limited by at least two substantially plane-parallel surfaces, the separation of which is smaller than half the coherence length for either the transmitted or luminescent optical energy, whereby an interference pattern will differently affect the transmission of optical energy to the receiver unit as the optical length between said parallel surfaces changes with changes in the physical quantity being sensed.

Claims

1. A fiber-optic sensor for detecting a change in a physical quantity which comprises

two substantially plane parallel interfaces spaced apart by a small enough distance to ensure that multiple reflections of optical energy at a given wavelength between said interfaces will give rise to constructive and destructive interference,

a body of solid material attached to one of said interfaces capable of emitting photoluminescent optical energy when excited with incident optical energy, one of said photoluminescent and incident optical energies having a wavelength corresponding to said given wavelength,

optical fiber means, for conveying incident optical energy to said interfaces and said body of solid material and conveying interference-affected incident and photoluminescent optical energies away from said interface, and

means to allow the change in the physical quantity to affect the optical path length of optical energy in the separation between said parallel interfaces.

2. A fiber-optical sensor according to claim 1, in which the physical separation between the plane-parallel interfaces is arranged to vary with the physical quantity to be measured, and is thus a measure of said quantity.

3. A fiber-optic sensor according to claim 1, in which the magnitude of the refractive index in a volume limited by the plane-parallel interfaces is arranged to constitute a measure of the quantity to be measured.

4. A fiber-optic sensor according to claim 1, in which the deviation from parallelism of the substantially plane parallel interfaces does not exceed one-tenth of a wavelength of at least one of the photoluminescent and incident optical energies.

5. A fiber-optic sensor according to claim 1, in which one of the plane-parallel interfaces is an end surface of the optical fiber means.

6. A fiber-optic sensor according to claim 1, in which the plane-parallel interfaces incorporate at least one reflective coating.

7. A fiber-optic sensor according to claim 6, in which the reflecting coating consists of a dielectric material.

8. A fiber-optic sensor according to claim 7, in which the thickness of the dielectric material is a multiple of half the wavelength for one of the photoluminescent and incident optical energies.

9. A fiber-optic sensor according to claim 6, in which the reflecting coating is a metallic material.

10. A fiber-optic sensor according to claim 1, in which the physical separation between the plane-parallel interfaces is determined by a spacer and an elastic portion of the body of photoluminescent material.

11. A fiber-optic sensor according to claim 1, in which the solid body comprises at least one semiconductor material.

12. A fiber-optic sensor according to claim 11, in which the semiconductor material is selected from the group consisting of GaAs and Al_x Ga_1-x As.

13. A fiber-optic sensor according to claim 1, in which the volume between the parallel interfaces is optically transparent at said given wavelength.

14. A fiber-optic sensor according to claim 1, in which at least one of the plane-parallel interfaces is part of a diaphragm, the deflection of which is a measure of the physical quantity which is to be sensed.

15. A fiber-optic sensor according to claim 1, in which the solid body is optically transparent at said given wavelength and is doped with metal ions having photoluminescent properties.

16. A fiber-optic sensor according to claim 15, in which the doping metal ions are neodymium ions.

17. A fiber-optic sensor according to claim 1, in which the sensor includes at least one lens element attached to said at least one of said interfaces.

18. A fiber-optic sensor according to claim 17, in which said lens element is a GRIN lens.

19. A fiber-optic measuring system for detecting a change in a physical quantity comprising a sensor, a transmitter and receiver unit, arranged to transmit and receive optical energy, and at least one optical fiber means for the transmission of optical energy to and from the sensor located at the point of measurement, characterized in that the sensor comprises at least one solid body, which is arranged to emit photoluminescent optical energy in at least one wavelength range, as well as a volume which is limited by at least two substantially plane-parallel interfaces the mutual separation of which is smaller than half the wavelength for the optical energy emitted from the transmitter unit or the photoluminescent optical energy emitted from the sensor.

20. A method of detecting a change in the optical length between two substantially parallel surfaces generating optical interference patterns due to multiple reflections of optical energy in the gap between said two surfaces, which method comprises supplying incident optical energy and photoluminescent optical energy excited by said incident energy to said gap in such a manner that one of said optical energy supplies is more significantly affected by changes in the interference pattern than the other, and monitoring changes in intensity of at least one of said optical energy supplies to provide a measure of the change in the optical length.