Apparatus and methods for generating nonlinear effects in centrosymmetric materials

Patent metadata

Field	Value
Publication number	US-10133149-B2
Application number	US-201615359149-A
Country	US
Kind code	B2
Filing date	Nov 22, 2016
Priority date	Nov 25, 2015
Publication date	Nov 20, 2018
Grant date	Nov 20, 2018

Abstract

A waveguide includes an array of p-i-n junctions formed by ions implanted into the waveguide. The p-i-n junctions concentrate electric fields applied on the waveguide to convert the third order susceptibility χ (3) into the second order susceptibility χ (2) and induce the DC Kerr effect. The periodic electrical fields concentrated by the p-i-n junctions effectively create a wave vector, which together with the wave vectors of optical beams in the waveguide satisfies phase matching conditions for nonlinear optical effects. The phase matching can significantly enhance the efficiency of the nonlinear optical effects, such as second harmonic generation, sum frequency generation, difference frequency generation, and four-wave mixing. Waveguides with arrays of PIN junctions can also be used in phase modulators, amplitude modulators, and filters.

First claim

The invention claimed is:

1. An apparatus comprising:
a waveguide comprising a centrosymmetric material to guide at least one light beam, the waveguide comprising:
a plurality of p-type regions comprising a p-doped centrosymmetric material on a first side of the waveguide; and
a plurality of n-type regions comprising an n-doped centrosymmetric material on a second side, opposite the first side, of the waveguide;

a first electrode in electrical communication with the plurality of p-type regions;
a second electrode, in electrical communication with the plurality of n-type regions, to apply a voltage between the first electrode and the second electrode so as to increase a second order susceptibility of the centrosymmetric material; and
a first light source, in optical communication with the waveguide, to emit the at least one light beam comprising a first light beam at a first frequency ω 1 and having a first wave vector k ω1 in the waveguide,
wherein the waveguide is further configured to guide a second light beam at a second frequency ω 2 and having a second wave vector k ω2 in the waveguide, and
wherein the plurality of the p-regions and the plurality of the n-regions are arrayed with a period Λ based at least in part on the first wave vector k ω1 of the first light beam and the second wave vector k ω2 of the second light beam.

2. The apparatus of claim 1 , wherein the centrosymmetric material comprises at least one of silicon or germanium.

3. The apparatus of claim 1 , wherein each p-type region in the plurality of the p-type regions and each n-type region in the plurality of n-type regions forms a PIN junction with a corresponding portion of the waveguide.

4. The apparatus of claim 1 , wherein the second frequency ω 2 =2ω 1 , and the period Λ=2π/(2k ω1 −k ω2 ).

5. The apparatus of claim 4 , wherein the second light beam has a wavelength of about 0.9 μm to about 10 μm.

6. The apparatus of claim 1 , further comprising:
a second light source, in optical communication with the waveguide, to emit the second light beam, the first light beam and the second light beam interacting in the waveguide to generate a third light beam at a third frequency ω 3 =(ω 1 −ω 2 ) and having a third wave vector k ω3 in the waveguide,
wherein the period Λ=2π/((k ω1 +k ω2 )−k ω3 ).

7. The apparatus of claim 1 , further comprising:
a second light source, in optical communication with the waveguide, to provide the second light beam so as to generate a third light beam at a third frequency ω 3 =(ω 1 −ω 2 ) and having a third wave vector k ω3 in the waveguide.

8. The apparatus of claim 1 , further comprising:
a voltage source, in electrical communication with the first electrode and the second electrode, to apply an alternating current voltage having an electrical frequency electrical so as to generate the second light beam,
wherein ω 2 =(ω 1 +ω electrical ) and Λ=2π/((k ω1 +k electrical )−k ω2 ).

9. The apparatus of claim 1 , wherein the period Λ is about 100 nm to about 10 mm.

10. The apparatus of claim 1 , wherein the plurality of p-type regions comprises a first periodic array of p-type regions having a first period and a second periodic array of p-type regions having a second period.

11. The apparatus of claim 1 , wherein the plurality of p-type regions further comprises at least one p-type region on the second side of the waveguide and the plurality of n-type regions further comprises at least one n-type region on the first side of the waveguide.

12. The apparatus of claim 1 , wherein the n-type material comprises the centrosymmetric material doped with an n-type dopant and the p-type material comprises the centrosymmetric material doped with a p-type dopant.

13. The apparatus of claim 12 , wherein at least one of the n-type dopant or the p-type dopant has a concentration of about 10 15 /cm 3 to about 10 20 cm 3 .

14. The apparatus of claim 1 , further comprising:
a voltage source, in electrical communication with the first electrode and the second electrode, to supply the voltage of about 1 V to about 100 V.

15. A method comprising:
guiding at least one light beam in a waveguide formed of centrosymmetric material, the waveguide comprising:
a plurality of p-type regions comprising a p-type material on a first side of the waveguide; and
a plurality of n-type regions comprising an n-type material on a second side, opposite the first side, of the waveguide;

applying a voltage between the plurality of p-type regions and the plurality of n-type regions to increase a second order susceptibility of the centrosymmetric material; and
wherein guiding the at least one light beam comprises:
guiding a first light beam at a first frequency ω 1 and having a first wave vector k ω1 in the waveguide; and
guiding a second light beam at a second frequency ω 2 and having a second wave vector k ω2 in the waveguide,
wherein at least one of the plurality of the p-type regions or the plurality of the n-type regions has a period Λ based at least in part on the first wave vector k ω1 of the first light beam and the second wave vector k ω2 of the second light beam.

16. The method of claim 15 , wherein the second frequency ω 2 =2ω 1 , the period Λ=2π/(2k ω1 −k ω2 ), and the method further comprises:
generating the second light beam from the first light beam via second harmonic generation within the waveguide.

17. The method of claim 16 , wherein generating the second light beam comprises generating light at a wavelength of about 1 μm to about 10 μm.

18. The method of claim 15 , further comprising:
generating a third light beam from the first light beam and the second light beam at a third frequency ω 3 =(ω 1 −ω 2 ) and having a third wave vector k ω3 in the waveguide via difference frequency generation, and
wherein the period Λ=2π/((k ω1 +k ω2 )−k ω3 ).

19. The method of claim 15 , further comprising:
generating the third light beam from the first light beam and the second light beam at a third frequency ω 3 =(ω 1 +ω 2 ) and having a third wave vector k ω3 in the waveguide via sum frequency generation with the period Λ of the at least one of the plurality of the p-regions or the plurality of the n-regions as Λ=2π/((k ω1 +k ω2 )−k ω3 ).

20. The method of claim 15 , wherein guiding the first light beam comprises:
guiding the first light beam through a first region of the waveguide including a first periodic array of p-type regions having a first period; and
guiding the first light beam through a second region of the waveguide including a second periodic array of p-type regions having a second period.

21. The method of claim 15 , wherein guiding the first light beam comprises:
guiding the first light beam through at least one portion of the waveguide including at least one second p-type region on the second side and at least one n-type region on the first side.

22. The method of claim 15 , wherein the n-type material comprises the centrosymmetric material doped with an n-type dopant and the p-type material comprises the centrosymmetric material doped with a p-type dopant, and the method further comprises:
changing at least one of a first doping concentration of the n-type dopant or a second doping concentration of the p-type dopant.

23. The method of claim 22 , wherein changing the at least one of the first doping concentration or the second doping concentration comprises changing the at least one of the first doping concentration or the second d

Assignees

• Massachusetts Inst Technology

Inventors

• Timurdogan Erman
• Watts Michael R

Classifications

• G02F1/3556

  Semiconductor materials, e.g. quantum wells · CPC title

• G02F1/3534

  Three-wave interaction, e.g. sum-difference frequency generation (G02F1/3532 takes precedence) · CPC title

• G02F2001/3548

  Physics · mapped topic

• G02F1/377

  in an optical waveguide structure · CPC title

• G02F1/365 Primary

  in an optical waveguide structure (G02F1/377, {G02F1/395} take precedence) · CPC title