High efficiency mono-order concave diffraction grating

• US 9,176,282 B2
• Filed: 10/05/2012
• Issued: 11/03/2015
• Est. Priority Date: 10/06/2011
• Status: Active Grant

• Current Assignee: Valorbec S.E.C.
• Original Assignee: Valorbec S.E.C.
• Inventors: Pottier, Pierre, Packirisamy, Muthukumaran
• Primary Examiner(s): RAHLL, JERRY T
• Application Number:
  US14/350,140
• Publication Number:
  US 20140233891A1
• Time in Patent Office: 1,124 Days
• US Class Current: 1/1
• CPC Class Codes: G01J 3/0256 Compact construction
• CPC Class Codes: G01J 3/18 using diffraction elements, e.g. grating gratings per se G02B
• CPC Class Codes: G01J 3/20 Rowland circle spectrometers
• CPC Class Codes: G02B 27/4244 in wavelength selecting devices spectrometry G01J
• CPC Class Codes: G02B 5/1814 structurally combined with one or more further optical elements, e.g. lenses, mirrors, prisms or other diffraction gratings G02B5/189 takes precedence
• CPC Class Codes: G02B 5/1861 Reflection gratings characterised by their structure, e.g. step profile, contours of substrate or grooves, pitch variations, materials G02B5/1809, G02B5/1828, G02B5/1833, G02B5/1838 and G02B5/1847 take precedence
• CPC Class Codes: G02B 6/12007 forming wavelength selective elements, e.g. multiplexer, demultiplexer
• CPC Class Codes: G02B 6/124 Geodesic lenses or integrated gratings
• CPC Class Codes: G02B 6/29328 Diffractive elements operating in reflection
• CPC Class Codes: G02B 6/34 utilising prism or grating G02B6/293 takes precedence

Abstract

A concave diffraction grating for integrated optics is constructed by replacing the reflective metallic part by either multiple thin elements of metal or multiple elements of dielectric material, each partially reflecting the light, and arranged on elliptical fashion in order to distribute the diffraction/reflection of light and provide aberration-free focusing, by combining diffraction condition and Bragg condition of these curved reflectors.

Claims

1. A device comprising:

an arrangement of a plurality of adjacent linear, elliptically shaped elements, each of the elements having a finite thickness, wherein each linear element, along its length, is locally parallel to an adjacent linear element in a direction substantially normal to the linear element;

a grating surface defined by portions of at least a subset of the plurality of elements;

a first port and at least one second port located at foci of an ellipse defining the elliptical shape of the plurality of elements.

2. The device of claim 1, wherein the plurality of elements each have a reflective metalized surface.

3. The device of claim 1, wherein the plurality of elements substantially form a Bragg reflective grating.

4. The device of claim 1, wherein the first port and at least one second port fall on a Rowland circle, and at least a portion of the grating surface falls on the Rowland circle.

5. The device of claim 1 in which the device uses a combination of materials having indices of refraction n₂ and n₁ and include at least one of:

silica (n₂) in silica (n₁);

air (n₂) in silica (n₁);

air (n₂) in silicon (n₁); and

silica (n₂) in silicon (n₁).

6. A device which has a diffraction grating comprising a plurality of adjacent linear elements, wherein each linear element, along its length, is substantially locally parallel to an adjacent linear element in a direction substantially normal to the linear element and wherein the elements providing the reflection are curved for their reflective properties in relation to their neighbours and/or for focusing.

7. The device according to claim 6, wherein the elements providing the reflection are substantially locally parallel.

8. The device according to claim 6, wherein the elements providing the reflection are substantially locally equidistant from one another.

9. The device according to claim 6, wherein the elements providing the reflection each have a substantially elliptical shape to provide output efficiency and aberration-free focusing with foci located at a device input and a device output.

10. The device according to claim 6, wherein the elements providing the reflection are metallic.

11. The device according to claim 6, wherein the elements providing the reflection are dielectrics.

12. The device according to claim 6, wherein a grating diffraction condition and a Bragg condition are based on different optical path differences, but each optical path difference is substantially a multiple of one or more wavelengths.

13. The device according to claim 6, wherein the elements providing the reflection are air, gas or vacuum grooves in any one of:

silicon dioxide;

silicon; and

III-V semiconductor elements.

14. The device according to claim 6, wherein the elements providing the reflection present a progressive change of index of refraction or material composition.

15. The device according to claim 6, wherein at least a part of the refractive index or material composition distribution of the elements providing the reflection presents an apodization along the direction locally perpendicular to the diffraction grating or along the direction of the length of the elements.

16. The device according to claim 6 based on the Rowland configuration, where light input and light output locations are substantially on the Rowland circle and where the grating front is tangent to the Rowland circle and has a radius of curvature substantially twice the Rowland circle radius.

17. A planar waveguide grating device comprising at least an input channel waveguide or at least an input location and a plurality of output channel waveguides or a plurality of output locations, wherein the grating element that spatially separates wavelengths supplied by the input channel waveguide comprises the device according to claim 6.

18. The planar waveguide grating device according to claim 17, based on geometrical configuration which allows the light emanating from the input location or channel waveguide extremity to be collected by the output locations or channel waveguides extremities.

19. The planar waveguide grating device according to claim 17 such that a mean penetration depth of light into the grating corresponds substantially to the position of a regular grating front.

20. The planar waveguide grating device according to claim 17, where the channel waveguides have a free orientation, in particular the one to maximize the light efficiency coupling into them.

21. The planar waveguide grating device according to claim 17, used for integrated spectrometers or for spectral measurement on a lab on a chip.

22. The planar waveguide grating device according claim 17 that is used for wavelength selection of an optical source, wherein the output or input channel waveguides could be used for, or replaced by, selective elements operating reflection, transmission, absorption, or other light manipulation.

23. The device according to claim 6, wherein at least two materials having different indices of reference are used in fabricating the device.

24. The device according to claim 6, wherein at least a part of the diffraction grating has a non-constant period.