System for transduction of displacement to optical phase shift
US-2019155065-A1 · May 23, 2019 · US
US11073412B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-11073412-B2 |
| Application number | US-201916664418-A |
| Country | US |
| Kind code | B2 |
| Filing date | Oct 25, 2019 |
| Priority date | Oct 26, 2018 |
| Publication date | Jul 27, 2021 |
| Grant date | Jul 27, 2021 |
A practical reading order for non-experts. Skip the full description unless you need deep technical detail.
What the patent document calls the invention.
A short plain-language summary of the technical disclosure.
Who owns or filed the patent and who is credited as inventor.
Filing, priority, publication, and grant dates set the timeline.
The legal scope of protection — read this for what is actually claimed.
Technology tags used to group this patent with similar filings.
Prior art links and similar publications in this corpus.
Official abstract text for this publication.
An opto-mechanical resonator including a waveguide formed by a plurality of first strips spaced apart from one another; and two mirrors disposed facing one another, which mirrors are optically reflective over at least part of a guide wavelength range of the waveguide. The waveguide extends between the two mirrors, and forms therewith an optically resonant cavity. At least part of the waveguide is held such that it is suspended over a substrate by at least one deformable mechanical element.
Opening claim text (preview).
The invention claimed is: 1. An opto-mechanical resonator comprising a waveguide formed by a plurality of first strips spaced apart from one another, wherein: the opto-mechanical resonator comprises at least two mirrors disposed facing one another, which mirrors are optically reflective over at least part of a guide wavelength range of the waveguide; the waveguide extends between the two mirrors, and forms therewith an optically resonant cavity; and a suspended region, comprising at least part of the waveguide, is held such that it is suspended over a substrate by at least one deformable mechanical element, and when undergoing deformation by way of the deformable mechanical element, the suspended region does not comprise a straight line but a curved line instead, resulting in a variation of the resonant wavelength of the opto-mechanical resonator. 2. The opto-mechanical resonator according to claim 1 , wherein the deformable mechanical element is fixed relative to the substrate, at least at one of the ends thereof along an axis parallel to the waveguide. 3. The opto-mechanical resonator according to claim 1 , wherein at least one deformable mechanical element comprises at least one arm, which extends along at least one axis parallel to the waveguide. 4. The opto-mechanical resonator according to claim 3 , wherein at least one deformable mechanical element comprises two arms, laterally framing the suspended region. 5. The opto-mechanical resonator according to claim 3 , wherein at least one deformable mechanical element comprises at least two series of segments, and wherein, in each series, the segments are distributed along an axis parallel to the waveguide and separated, in pairs, at least by a gap filled with a gas or a vacuum. 6. The opto-mechanical resonator according to claim 3 , wherein at least one deformable mechanical element comprises a deformable membrane, forming a support for the suspended region. 7. The opto-mechanical resonator according to claim 1 , wherein said mirrors are Bragg mirrors. 8. The opto-mechanical resonator according to claim 7 , wherein each of said Bragg mirrors comprises a plurality of second strips, each of which is made of the same material as the first strips of the waveguide. 9. The opto-mechanical resonator according to claim 7 , wherein at least part of at least one of said Bragg mirrors forms a part of the suspended region. 10. The opto-mechanical resonator according to claim 1 , wherein the first strips of the waveguide are distributed one after another according to a distribution pitch Λ such that: Λ < λ 0 2 n h where λ 0 is the central wavelength of the guide wavelength range of the waveguide; and n h is the average refractive index of the first strips. 11. A system comprising at least two opto-mechanical resonators, wherein: each opto-mechanical resonator comprises an optically resonant cavity, formed by a waveguide arranged between two mirrors, with the waveguide comprising a plurality of first strips spaced apart from one another; at least one of said opto-mechanical resonators forms an opto-mechanical resonator according to claim 1 ; and the opto-mechanical resonators are optically coupled in pairs by evanescent coupling. 12. A measuring device comprising at least one opto-mechanical resonator according to claim 1 , and at least one optical sensor, the optical sensor being arranged so as to receive a light beam (F out ) emerging from the opto-mechanical resonator after having undergone a plurality of forward-return movements therein, and being capable of measuring a fluctuation, as a function of time, of a physical property of said light beam.
with deflection of beams of light, e.g. for direct optical indication (G01D5/40 takes precedence; {mechanical adjustment G01D5/264}) · CPC title
Sensor · CPC title
Three-dimensional structures · CPC title
using optical fibres (G01D5/28 - G01D5/38 take precedence) · CPC title
by vibratory elements · CPC title
Related publications grouped by family.
Answers are generated from the same data shown on this page.