Slanted Bragg Grating Refractometer, Using the Optical Power Diffracted to the Radiation-Mode Continuum

• US 20080129985A1
• Filed: 12/07/2005
• Published: 06/05/2008
• Est. Priority Date: 12/10/2004
• Status: Abandoned Application

• Current Assignee: Commissariat a L'Energie Atomique (French Alternative Energies and Atomic Energy Commission)
• Original Assignee: Commissariat a L'Energie Atomique (French Alternative Energies and Atomic Energy Commission)
• Inventors: Ferdinand, Pierre, Prudhomme, Cecile, Laffont, Guillaume
• Application Number:
  US11/792,757
• Publication Number:
  US 20080129985A1
• Time in Patent Office: Days
• US Class Current: 356/128
• CPC Class Codes: G01N 21/431 Dip refractometers, e.g. using optical fibres
• CPC Class Codes: G02B 6/124 Geodesic lenses or integrated gratings

Abstract

This refractometer includes at least one optical waveguide (2) comprising at least one slanted Bragg grating (4), formed in a part of the waveguide, which is placed in contact with the medium (7) of which the refraction index is to be determined, a light source (10) coupled to the waveguide in order to send this light there and have it interact with the grating, means (17) for measuring the optical power of the light diffracted to the radiation-mode continuum, when the light transmitted by the source interacts with the grating, and electronic processing means (22) for supplying the value of the refraction index of the medium based on this optical power.

Claims

1. System for measuring the refraction index of at least one medium, which system includes:

at least one optical waveguide (2, 44) having first and second ends and comprising at least one slanted Bragg grating (4, R₁ . . . R_N, R_F1 . . . R_FN), formed in a part of the waveguide, which is placed in contact with the medium, and

a light source (10, 46, 50) optically coupled with the first end of the waveguide in order to send this light there and have it interact with the grating,

this system being characterised in that it also includes;

first means (17, P₁ . . . P_N) for measuring the optical power of the light diffracted to the radiation-mode continuum, when the light transmitted by the source interacts with the grating, and

electronic processing means (22, 48, 54) provided for supplying the value of the refraction index of the medium based on this optical power.

2. System according to claim 1, wherein the optical waveguide is an optical fibre (2, 44).

3. System according to claim 1, wherein the optical waveguide is an integrated waveguide.

4. System according to claim 1, wherein the first measurement means include a first photodetector (17, P₁ . . . P_N).

5. System according to claim 4, wherein the first measurement means also include an optic (24, 32) provided for collecting the diffracted light and concentrating it on the first photodetector.

6. System according to claim 5, wherein the optic is a lens or an objective (24) or a selfoc-type lens (32).

7. System according to claim 5, wherein the first measurement means also include a prism (26) with a reflective surface or a mirror, by means of which the optic collects the light.

8. System according to claim 4, wherein the first measurement means also include an optic prism with a concave reflective surface or a concave mirror for collecting the diffracted light and concentrating it on the first photodetector.

9. System according to claim 5, wherein it also includes an optical fibre (34) that connects the optic to the first detector.

10. System according to claim 1, wherein it also includes second means (18, D₁ . . . D_N) for measuring the optical power of the light that is transmitted, by the slanted Bragg grating, up to the second end of the optical waveguide, and in which the electronic processing means are provided for determining the ratio of the optical power of the light diffracted to the radiation-mode continuum over the optical power of the light transmitted by the slanted Bragg grating.

11. System according to claim 10, wherein the second measurement means include a second photodetector (18, D₁ . . . D_N).

12. System according to claim 11, wherein the second measurement means also include an optic (20) for collecting the transmitted light and concentrating it on the second photodetector.

13. System according to claim 10, also including:

a light reflector (38) that is placed at the second end of the optical waveguide and provided for reflecting, into this optical waveguide, the light transmitted by the slanted Bragg grating, and

means (40, 42) for optical coupling between, on the one hand, the first end of the optical waveguide and the second measurement means, and, on the other hand, this first end and the light source (10).

14. System according to claim 13, wherein the optical coupling means include a 2×

2-type optical coupler (40) or an optical circulator (42).

15. System according to claim 1, including a plurality of slanted Bragg gratings (R₁ . . . R_N) that have the same spectral response.

16. System according to claim 1, including:

N slanted Bragg gratings (R₁ . . . R_N) that have the same spectral response, with N being an integer equal to at least 2, and these gratings being counted from the source,

for each grating, second means (D₁ . . . D_N) for measuring the optical power of the light transmitted by this grating, and

for each of the N−

1 first gratings, an optical coupler (C₁ . . . C_N-1) for sampling light, mounted on the optical waveguide, between the associated grating and the next grating, and provided for sending the sampled light to the second corresponding measurement means,

and in which the electronic processing means (48) are provided for determining, for each grating, the ratio of the optical power of the light diffracted by this grating to the radiation-mode continuum over the optical power of the light transmitted by this grating.

17. System according to claim 1, including a plurality of slanted Bragg gratings of which the spectral responses are different from one another.

18. System according to claim 1, including:

N slanted Bragg gratings (R₁ . . . R_N) of which the spectral responses are different from one another, with N being an integer equal to at least 2, and these gratings being counted from the source,

for each grating, second means (D₁ . . . D_N) for measuring the optical power of the light transmitted by this grating, and

for each of the N−

1 first gratings, an optical coupler (C₁ . . . C_N-1) for sampling light, mounted on the optical waveguide, between the associated grating and the next grating, and provided for sending the sampled light to the second corresponding measurement means,

and in which the electronic processing means (48) are provided for determining, for each grating, the ratio of the optical power of the light diffracted by this grating to the radiation-mode continuum over the optical power of the light transmitted by this grating.

19. System according to claim 1, including:

N slanted Bragg gratings (R_F1 . . . R_FN), which are centred on spectral windows different from one another, with N being an integer equal to at least 2, and these gratings being counted from the source,

for each grating, second means (D₁ . . . D_N) for measuring the optical power of the light transmitted by this grating, and

for each of the N−

1 first gratings, an optical coupler (C₁ . . . C_N-1) for sampling light, mounted on the optical waveguide, between the associated grating and the next grating, and provided for sending the sampled light to the second corresponding measurement means,

and in which the electronic processing means (48) are provided for determining, for each grating, the ratio of the optical power of the light diffracted by this grating to the radiation-mode continuum over the optical power of the light transmitted by this grating.

20. System according to claim 1, including a plurality of optical waveguides and optical switching means (52), provided for successively sending the light supplied by the source into the optical waveguides.

21. System according to claim 1, wherein the light supplied by the source is amplitude-modulated, at a predefined frequency, and a synchronous detection technique is implemented with the measurement means in order to recover the optical power supplied by these measurement means.