Direct entangled triplet-photon sources and methods for their design and fabrication

Patent metadata

Field	Value
Publication number	US-9971228-B2
Application number	US-201615130482-A
Country	US
Kind code	B2
Filing date	Apr 15, 2016
Priority date	Oct 31, 2013
Publication date	May 15, 2018
Grant date	May 15, 2018

Abstract

In one aspect, a device for generating triplet photons is disclosed, which includes a waveguide extending from a proximal end for receiving pump radiation to a distal end through which triplet photons generated via nonlinear interaction of the pump radiation with the waveguide exit the waveguide, where the waveguide is configured such that the triplet photons generated within the waveguide reach its distal end at a rate in a range of about 0.05 triplet photons/second/mW and 0.3 triplet photons/second/mW, e.g., in a range of about 0.1 triplet photons/second/mW to about 0.2 triplet photons/second/mW.

First claim

The invention claimed is:

1. A device for generating triplet photons, comprising:
a waveguide comprising a core and at least one cladding and extending from a proximal end for receiving pump radiation to a distal end through which triplet photons generated via nonlinear interaction of the pump radiation within the waveguide exit the waveguide, wherein the waveguide is configured such that the triplet photons are generated within the waveguide and reach said distal end at a rate in a range of about 0.05 triplet photons/second/mW and 0.3 triplets/second/mW,
wherein said length of the waveguide is equal to or less than (L opt ) defined by the following relation:
wherein α p and α s denote loss coefficients for the pump radiation photons and the triplet photons within said waveguide, respectively.

2. The device of claim 1 , wherein said rate is in a range of about 1 triplet photons/second/mW to about 0.2 triplet photons/second/mW.

3. The device of claim 1 , wherein said waveguide is configured to provide phase matching between at least one propagating mode of said pump radiation and at least one propagating mode suitable for generation of said triplet photons.

4. The device of claim 3 , wherein said waveguide is configured to provide phase matching between a higher-order propagating mode of said pump radiation and at least one mode suitable for propagation of said triplet photons.

5. The device of claim 1 , wherein said waveguide exhibits values of core and cladding thickness, height, etch fraction, sidewall angle and length that result in the waveguide supporting said rate for the triplet photons generated within the waveguide that reach its distal end.

6. The device of claim 5 , wherein any of said thickness and height are in the range of about 100 nm to about 2000 nm, fully etched fraction is in the range of 0.25 to 1 (fully etched), sidewall angle is in the range of 45-degrees to 90-degrees (vertical sidewalls) and length is in range of about 100 μm to about 10 cm.

7. The device of claim 1 , wherein said waveguide core comprises any of anatase TiO 2 , amorphous TiO 2 , brookite TiO 2 , silicon nitride, diamond, silicon nitride, silicon carbide, strontium titanate, or zinc oxide.

8. The device of claim 7 , wherein said waveguide core comprises rutile TiO 2 .

9. The device of claim 1 , wherein said at least one cladding comprises any of SiO 2 , CYTOP, SU-8, a low-index polymer, aluminum oxide, sapphire, air or vacuum.

10. The device of claim 1 , wherein said waveguide core comprises a polycrystalline material.

11. The device of claim 10 , wherein said polycrystalline material has grain sizes less than about 50 nm.

12. The device of claim 1 , wherein said polycrystalline material has grains having a size of about ⅕ th of the pump wavelength.

13. The device of claim 1 , wherein said waveguide has a non-circular cross section.

14. The device of claim 13 , wherein said waveguide has a rectangular or trapezoidal cross section.

15. The device of claim 1 , wherein said waveguide comprises a ring resonator.

16. A device for generating triplet photons, comprising
a waveguide extending from a proximal end for receiving pump radiation to a distal end through which triplet photons generated via nonlinear interaction of the pump radiation within the waveguide exit the waveguide,
wherein the waveguide is configured such that the triplet photons are generated within the waveguide and reach said distal end at a rate in a range of about 0.05 triplet photons/second/mW and 0.3 triplet photons/second/mW,
wherein said waveguide length is greater than a length (L min ) satisfying the following relation:

Δ
PPM

=

4
⁢
π

L
min

⁢



D
s



wherein λ PPM denotes the bandwidth of triplet photons at a phase matching point and

D
s

=

∂
2

⁢

k
s

∂
2

⁢

ω
s

 evaluated at ω s =ω s 0 is group velocity dispersion (GVD) of the triplet photons at the phase matching point.

17. The device of claim 16 , wherein said waveguide comprises a core and at least one cladding.

18. The device of claim 17 , wherein said waveguide core comprises any of anatase TiO 2 , amorphous TiO 2 , brookite TiO 2 , silicon nitride, diamond, silicon carbide, strontium titanate, or zinc oxide.

19. The device of claim 17 , wherein said waveguide core comprises rutile TiO 2 .

20. The device of claim 17 , wherein said cladding comprises any of SiO 2 , CYTOP, SU-8, a low-index polymer, aluminum oxide, sapphire, air or vacuum.

21. The device of claim 17 , wherein said waveguide core comprises a polycrystalline material.

22. The device of claim 21 , wherein said polycrystalline material has grain sizes less than about 50 nm.

23. A method of generating direct triplet photons, comprising
introducing pump radiation into a waveguide configured to provide phase matching between a higher order mode of said pump radiation and at least one mode suitable for propagation of direct triplet photons generated as a result of a non-linear interaction between the pump radiation and the waveguide,
wherein the waveguide is configured such that the triplet photons are generated within the waveguide and reach said distal end at a rate in a range of about 0.05 triplet photons/second/mW and 0.3 triplet photons/second/mW,
wherein a rate at which pump photons are applied to the waveguide is less than a threshold as defined by the following relation:

N
P

<

ρ
T

ρ
fl
3

⁢

Δτ
correlation
2

where ρ T and ρ fl represent, respectively, the rate at which pump photons are converted to photon triplets and fluorescence pho

Assignees

• Harvard College

Inventors

• Mazur Eric
• Evans Christopher Courtney
• Moebius Michael Gerhard
• Reshef Orad
• Griesse-Nascimento Sarah E

Classifications

• G02F1/353 Primary

  Frequency conversion, i.e. wherein a light beam is generated with frequency components different from those of the incident light beams · CPC title

• G02F1/3501

  Constructional details or arrangements of non-linear optical devices, e.g. shape of non-linear crystals · CPC title

• G02F1/3544

  Particular phase matching techniques · CPC title

• G02F1/395

  in optical waveguides · CPC title

• G02F1/365

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