Optical modulation apparatus and measurement method

• US 5,091,983 A
• Filed: 11/29/1989
• Issued: 02/25/1992
• Est. Priority Date: 06/04/1987
• Status: Expired due to Fees

• Current Assignee: Walter Lukosz
• Original Assignee: Walter Lukosz
• Inventors: Lukosz, Walter
• Primary Examiner(s): Healy, Brian
• Application Number:
  US07/445,735
• Time in Patent Office: 818 Days
• Field of Search: 350/96.11, 350/96.12, 350/96.13, 350/96.14, 350/96.15, 350/96.18, 350/96.19, 350/320, 250/231.19, 250/227.18, 250/227.19, 250/227.28, 372/96
• US Class Current: 385/13
• CPC Class Codes: G01D 5/266 by interferometric means G01D5/353 takes precedence
• CPC Class Codes: G01D 5/35303 using a reference fibre, e.g. interferometric devices
• CPC Class Codes: G02B 26/02 for controlling the intensity of light G02B26/004 takes precedence
• CPC Class Codes: G02B 6/24 Coupling light guides
• CPC Class Codes: G02B 6/2821 using lateral coupling between contiguous fibres to split or combine optical signals
• CPC Class Codes: G02B 6/2826 using mechanical machining means for shaping of the couplers, e.g. grinding or polishing grinding, polishing in general B24
• CPC Class Codes: G02B 6/34 utilising prism or grating G02B6/293 takes precedence
• CPC Class Codes: G02F 1/011 in optical waveguides, not otherwise provided for in this subclass
• CPC Class Codes: G02F 1/0134 in optical waveguides
• CPC Class Codes: G02F 1/0147 based on thermo-optic effects G02F1/132 takes precedence
• CPC Class Codes: G02F 1/212 Mach-Zehnder type
• CPC Class Codes: G02F 1/213 Fabry-Perot type
• CPC Class Codes: G02F 1/215 Michelson type
• CPC Class Codes: G02F 1/225 in an optical waveguide structure
• CPC Class Codes: G02F 1/295 Analog deflection from or in an optical waveguide structure]
• CPC Class Codes: G02F 1/3132 of directional coupler type
• CPC Class Codes: G02F 1/3136 of interferometric switch type
• CPC Class Codes: G02F 1/3137 with intersecting or branching waveguides, e.g. X-switches and Y-junctions
• CPC Class Codes: G02F 1/335 having an optical waveguide structure
• CPC Class Codes: G02F 2201/302 grating coupler
• CPC Class Codes: G02F 2201/307 : Reflective grating, i.e. Bragg grating

Abstract

In an optical micromechanical method for changing the phase of guided waves and a measurement method for measuring very small mechanical displacements and/or mechanical forces or pressures, including the pressure of sound waves and ultrasonic waves, and/or accelerations, the distance d between a section (1'"'"') of an optical waveguide (1) in an integrated optic or fibre optic circuit and a phase-shifting element (5) separated from said section (1'"'"') by a gap (4) is varied by forces (6) or by thermal expansion due to changes in temperature. The phase of the guided wave (3) is thereby modulated, and reciprocally the changes in distance d and hence small mechanical displacements and the forces (6) which produce them are determined from the measured phase changes.

Claims

1. A method for changing the phase of guided waves and measuring very small mechanical displacements comprising the steps of

providing a waveguide (1) having a first waveguide section (1'"'"') with an effective refractive index N and a phase shifting element (5) spaced from the waveguide section (1'"'"') by a gap (4) having a width d,

filling the gap (4) with a medium having small absorption and a refractive index n<

N, and either

(a) varying the width d of the gap as a function of time while passing an optical wave (3) through the waveguide, the width d of the gap being sufficiently small so that the refractive index of the waveguide and the phase of the wave ar changed by interation of the evanescent field of the wave with phase-shifting element 3 or surface layers (13) of phase shifting element (5) facing the waveguide section (1'"'"'), while absorbing or coupling out of the waveguide section (1'"'"') substantially no power of the guided wave (3) by the phase shifting element (5), or

(b) measuring changes of the effective refractive index N and the phase of the optical wave (3) as a measure of changes of the width d.

2. A method according to claim 1 wherein the width d between the waveguide section (1'"'"') and the phase-shifting element (5) is smaller than four times the penetration depth Δ

z=(λ

/2π

) (N² -n²)^-1/2 of the evanescent field into the gap (4), where λ

is the wavelength in vacuum.

3. A method according to claim 2 wherein the gap (4) between the section (1'"'"') of the waveguide (1) and the phase-shifting element (5) is filled with a compressible medium or is evacuated.

4. Method according to claim 3, characterized in that the change of width d between the phase-shifting element (5) and the section (1'"'"') of the waveguide (1) is produced by a force (6) or several forces, preferably by mechanical forces, and/or pneumatic or hydrostatic pressures, or by pressures of sound or ultrasonic waves, and/or acceleration forces, and/or by electrostatically, electromagnetically, or piezoelectrically generated forces, or by forces exerted by acoustic surface waves.

5. Method according to claim 3, characterized in that the change in width d between the phase-shifting element (5) and the section (1'"'"') of the waveguide (1) is produced through thermal expansion or deformation of one, some, or all components chosen from the group consisting of waveguide (1), substrate (2), phase-shifting element (5) and its attachment (16;

16,14,15;

16,19) to the waveguide (1) or substrate (2), by temperature changes, which in particular are caused either by electric currents in an electrically conducting heating layer, consisting for example, of indium-tin-oxide (ITO), or in a thermo-electric element, which are attached to the substrat (2), the phase-shifting element (5), or the attachment (16;

16,14,15;

16,19), or by absorption of light or infrared radiation in waveguide section (1'"'"') or in the phase-shifting element (5), wherein either the light or infrared radiation is incident from outside or the guided optical wave (3) itself is partially absorbed.

6. Method according to claim 5, characterized in that the waveguide (1) has the form of a planar or strip waveguide on a substrate (2).

7. Method according to claim 5, characterized in that the waveguide (1) has the form of the core (21) of a fiber waveguide, the fiber cladding (22) of which is in the waveguide section (1'"'"') completely or partially removed, preferably one side of the fiber only.

8. Method according to claim 7, characterized in that an optical wave (3e ) is coupled into a waveguide (1) and is guided therein, and is incident on an integrated optic or fiber optic interferometer, preferably a Mach-Zehnder interferometer or Michelson interferometer, and that the distance d between a section (1a'"'"') of the waveguide (1a) in one leg of the interferometer and the phase-shifting element (5) located opposite to said section (1a'"'"') is varied, whereby the phase of the guided wave (3a ) in waveguide section (1a'"'"') and hence the intensities of the guided waves (3c;

3a,3b) at the output ports of the interferometer are changed, and that either the width d is varied as a function of time and thus a desired intensity modulation is impressed on the waves (3c;

3a,3b), or that by the effect of forces (6) or temperature changes induced unknown changes of the width d are determined from the intensity changes of one of the waves (3c;

3a,3b).

9. Method according to claim 7, characterized in that an optical wave (3e ) is coupled into and is guided in one of two strip waveguides (1a,1b) which form a directional coupler, and that the width d between section (1a'"'"') of the waveguide (1a) in the coupling region and the phase-shifting element (5) located opposite to it is varied, and hence the intensities of the guided waves (3a,3b) in the two waveguides (1a,1b) at the output ports are changed, or the guided wave (3e ) is switched from the one to the other output waveguide (1a,1b) of the directional coupler.

10. Method according to claim 7, characterized in that the width d is varied between a section (1'"'"') of an optical waveguide (1) inside of an integrated optic or fiber optic resonator, preferably a Fabry-Perot resonator or ring resonator, and a phase-shifting element (5) which is located opposite said section (1'"'"'), and thereby the resonance frequencies of the resonator and its transmittance and reflectance are changed, and that either a guided optical wave (3e ) is incident on the resonator and the intensities of the reflected (3r ) and transmitted waves (3t) are changed, or that the wavelengths are changed of the guided waves generated by amplification in an active medium inside the resonator.

11. Method according to claim 7, characterized in that a wave (3) guided in an optical waveguide (1) impinges on a grating, (8) which acts as a Bragg reflector, and that the width d between the waveguide (1) and a phase-shifting element (5) located opposite to said waveguide in the region of the grating (8) is varied, whereby the wavelength for which optimum Bragg reflection occurs and the reflectance and transmittance of the Bragg reflector are changed and hence the intensities of the transmitted (3t) and reflected (3r ) guided waves dependent on their frequencies are changed, or that guided waves (3) are generated in the region of the grating (8) in a waveguide 1 with amplification, i.e., in a so called DFB (distributed feedback) laser, whereby their wavelengths, i.e. the emission frequencies of the DFB lasers are changed.

12. Method according to claim 7, characterized in that an optical wave (3e ) is by a grating coupler (8) coupled into a waveguide (1) and that the distance d between the waveguide section (1'"'"') and a phase-shifting element (5) which is located opposite to said section (1'"'"') in the region of the grating coupler (8) is varied, whereby the intensity of the incoupled guided wave (3) and hence the intensity of the non-incoupled part of the incident optical wave (3e ) are changed.

13. Method according to claim 7, characterized in that an optical wave (3) guided in a waveguide (1) is outcoupled by a grating coupler (8) and that the width d between the waveguide section (1'"'"') and a phase-shifting element (5), which is located opposite to said section (1'"'"') in the region of the grating coupler (8), is varied uniformly and/or like a wedge in direction of propagation of the guided wave (3), whereby the direction and/or focusing of the outcoupled beam (3a ) are changed.

14. Method according to claim 7, characterized in that an optical wave (3) is guided in a planar waveguide (1) and that theΔ

distance d between a section (1'"'"') of the waveguide (1) and a phase-shifting element (5), which is located opposite to said section (1'"'"'), is formed like a wedge transverse to the direction of propagation of the guided wave (3) and that the wedge angle is varied, whereby the guided wave (3) is deflected and the deflection angle (β

) of the deflected wave (3d ) after the phase-shifting element (5) is changed, and/or has the form of a quadratic curve, the curvature of which is varied, whereby the guided wave (3d ) after the phase-shifting element (5) is focused or defocused and the focusing is changed.

15. Method according to claim 14, characterized in that light of a laser (9) is coupled into a planar waveguide (1) on a substrate (2), and is incident divergently on a grating coupler (8) with curved grating lines and non-constant grating period and is outcoupled by it, whereby the outcoupled wave (3a ) is focused to a focus (11), and that with a phase-shifting element (5) opposite the section (1'"'"') of the planar waveguide (1), and/or with a phase-shifting element (5) opposite the grating coupler (8) the focus (11) is displaced in one direction or two orthogonal directions, respectively.

16. Method according to claim 7, characterized in that a guided wave (3e ) is coupled into one of two strip waveguides (1a,1b), which intersect under a small angle and thus form an X-switch, and that the width d between the waveguide sections (1a'"'"',1b'"'"') in their cross-over region and a phase-shifting element (5) located oppositely is changed, preferably in such a way that a in direction perpendicular to the two strip waveguides a wedge like gap (4) is formed between the phase-shifting element (5) and the waveguide sections (1a'"'"',1b'"'"') and the substrate surface, respectively, and the wedge angle is changed, whereby the wave (3e ) at the output of the X-switch is switched from one strip waveguide (1a) to the other strip waveguide (1b), or the intensities of the guided waves (3a ) and (3b ) at the output ports are modulated, respectively.

17. Method according to claim 16, characterized in that in an integrated optic or fiber optic Mach-Zehnder interferometer, directional coupler, or X-switch, which as 2×

2 switch matrices optically interconnect two input waveguides (1a) and (1b) with two output waveguides (1a) and (1b), the distance d between the phase-shifting element (5) and the waveguide sections (1a'"'"';

1a'"'"',1b'"'"') is adjusted in such a way, that either the input waveguide (1a) is optically interconnected only with the output waveguide (1a) and simultaneously the input waveguide (1b) only with the output waveguide (1b), or the input waveguide (1a) is optically interconnected only with the output waveguide (1b) and simultaneously the input waveguide (1b) only with the output waveguide (1a), and that by a change of the width d the switch matrix can be switched from the first mentioned parallel state into the last mentioned cross state.

18. Method according to claim 17, characterized in that in M×

M'"'"' switch matrices which are formed by arrays of directional couplers, Mach-Zehnder interferometers, or X-switches, which serve as 2×

2 switch matrices and which each contain at least one phase-shifting element (5), the width d of the phase-shifting elements (5) from the corresponding waveguide sections (1a'"'"';

1a'"'"',1b'"'"') in the 2×

2 switch matrices are adjusted in such a way, that each of M input waveguides is optically interconnected as desired with one or several of M'"'"' output waveguides, where M and M'"'"' are integers >

2.

28. A method according to claim 2 wherein the width d between the waveguide section (1'"'"') and the phase-shifting element (5) is smalle than one penetration depth Δ

z.

29. A method according to claim 3 wherein the compressible medium is a gas.

19. An apparatus comprises an optical waveguide (1) or an integrated optic or fiber optic circuit, which contains at least one optical waveguide, and a phase-shifting element (5) located at a small variable width d opposite section (1'"'"') of the waveguide (1) and separated by a gap (4) from said section.

20. Apparatus according to claim 19, characterized in that the phase-shifting element (5) or its surface layers (13) facing the waveguide section (1'"'"') consist of materials which absorb no or little light at the used wavelength λ

and have refractive indices n_E smaller than the effective refractive index N of the wave (3) guided in the waveguide section (1'"'"').

21. Apparatus according to claim 20, characterized in that the surface of the phase-shifting element (5) or its surface layers (13), respectively, facing the waveguide section (1'"'"'), are either smooth or are provided with a surface structure, for example, with a grating (8) acting as an input or output coupler, or as a Bragg reflector.

22. Apparatus according to claim 21, characterized in that the phase-shifting element (5) opposite the waveguide section (1'"'"') is attached to a tongue or paddle (14), bridge (19), or membrane, which in turn with an attachment (16) is attached to the waveguide (1), a substrate (2), or a protection layer (10), wherein the tongue or paddle (14), bridge (19), or membrane preferably are miniaturized and for example consist of SiO₂, and are preferably covered with another layer (15), which for example has a different thermal expansion coefficient, or is a heating layer, a piezoelectric layer, or a metal layer.

23. Apparatus according to claim 22, characterized in that beneath the waveguide section (1'"'"'), in the substrate (2), or in the buffer layer (7) lying between waveguide (1) and substrate (2), a cavity is located as the gap (4) between the waveguide section (1'"'"') and the phase-shifting element (5), wherein preferably the phase-shifting element (5) is identical with that region of substrate (2) or buffer layer (7) adjacent to the gap (4), or that above the waveguide section (1'"'"') in the protection layer (10) on the waveguide (1) a cavity is provided as the gap (4) between the waveguide section (1'"'"') and the phase-shifting element (5), wherein preferably the phase-shifting element (5) is identical with that region of the protection layer (10) adjacent to the gap (4), or that in the case of a fiber waveguide in section (1'"'"') in the cladding (22) a cavity is provided as the gap (40 between fiber core (21) and the phase-shifting element (5), wherein preferably the phase-shifting element (5) is identical with the region of the cladding (22) adjacent to the gap (4).

24. Apparatus according to claim 19, characterized in that a cavity is provided as the gap (4) inside the waveguide section (1'"'"') and the regions of the waveguide section (1'"'"') adjacent to the gap (4) act simultaneously as waveguide (1'"'"') and as phase-shifting element (5).

25. Apparatus according to claim 24, characterized in that cavities, for example in the form of slits, bores, or holes are provided as gap (4) in the waveguide section (1'"'"') a protection layer (10), the buffer layer (7), or a substrate (2), in fiber waveguides in the core (21) or in the cladding (22).

26. Apparatus according to claim 22, characterized in that the phase-shifting element (5) is attached to the substrate (2) with a holder (16;

16,14,15;

16,19).

27. Apparatus according to one of the claims 19 to 26, characterized in that the substrate (2) is a silicon wafer, the buffer layer (7) consists of SiO₂, and preferably the waveguide (1) consists of Si₃ N₄ and the phase-shifting element (5) and the protection layer (10) of SiO₂.