Method for impressing gratings within fiber optics

• US 4,725,110 A
• Filed: 10/27/1986
• Issued: 02/16/1988
• Est. Priority Date: 08/13/1984
• Status: Expired due to Term

• Current Assignee: United Technologies Corporation (Rtx Corporation)
• Original Assignee: United Technologies Corporation (Rtx Corporation)
• Inventors: Meltz, Gerald, Snitzer, Elias, Glenn, William H.
• Primary Examiner(s): NOT, DEFINED
• Assistant Examiner(s): Lerner, Martin
• Application Number:
  US06/925,512
• Time in Patent Office: 477 Days
• Field of Search: 350/96.11, 350/96.19, 350/96.23, 350/3.61, 350/3.7, 350/3.70, 350/162.17, 350/162.2, 350/162.21, 356/32
• US Class Current: 359/3
• CPC Class Codes: G02B 5/18 Diffraction gratings holographic optical elements G02B5/32, G03H; integrally combined with optical fibres G02B6/02057; for coupling light guides G02B6/34; integrally combined with optical integrated light guides G02B6/12; grating systems G02B27/44
• CPC Class Codes: G02B 6/02133 using beam interference
• CPC Class Codes: G02B 6/022 using mechanical stress, e.g. tuning by compression or elongation, special geometrical shapes such as "dog-bone" or taper G02B6/02204 takes precedence; optical modulation using photo-elastic effect G02F1/0131
• CPC Class Codes: G02B 6/02204 using thermal effects, e.g. heating or cooling of a temperature sensitive mounting body optical modulation using thermo-optic effect G02F1/0147
• CPC Class Codes: G02B 6/124 Geodesic lenses or integrated gratings
• CPC Class Codes: Y10S 359/90 Methods

Abstract

A method of establishing a dielectric periodic index of refraction phase grating upon the core of an optical waveguide by intense angled application of several transverse beams of ultraviolet light, enabling the establishment of a distributed, spatially resolving optical fiber strain gauge.

Claims

1. A method of impressing at least one grating into at least one predetermined region of a core of an optical fiber which further includes a cladding surrounding the core and is centered on a longitudinal axis, comprising the steps of

making the core of a material of a material whose index of refraction can be permanently changed by exposing such material to light of a predetermined intensity at a wavelength in a predetermined range of the spectrum;

and

simultaneously exposing the core through the cladding to two light beams propagating at respective different angles of incidence relative to the longitudinal axis of the optical fiber toward and through the cladding into the predetermined region of the core to form an interference pattern of longitudinally varying intensity propagating transversely through the core and forming permanent periodic refractive index perturbations in the material of the predetermined region of the core in dependence on the intensity of the interference pattern.

2. The method as defined in claim 1, wherein said exposing step includes using light beams of a wavelength in the ultraviolet range of the spectrum.

3. The method as defined in claim 2, wherein the wavelength of said light beams is less than 300 nanometers.

4. The method as defined in claim 1, wherein said exposing step includes so selecting the angles of incidence of the light beams that the periodicity of the refractive index perturbations corresponds to one-half of a selected wavelength of light propagating through the optical fiber during the use thereof.

5. The method as defined in claim 4, and further comprising the step of additionally performing said exposing step through the cladding on at least one additional predetermined region of the core at respective additional angles of incidence that differ from one another and from those used during said exposing step to form a different interference pattern of longitudinally varying intensity propagating transversely through the core and forming permanent periodic refractive index perturbations in the material of the additional predetermined region of the core in dependence on the intensity of the interference pattern, the additional angles of incidence of the light beams being such that the periodicity of the refractive index perturbations corresponds to one-half of another selected wavelength of light propagating through the optical fiber during the use thereof.