Tuneable laser

• US 20050175044A1
• Filed: 03/19/2003
• Published: 08/11/2005
• Est. Priority Date: 03/19/2002
• Status: Abandoned Application

• Current Assignee: Bookham Incorporated (Oclaro (North America), Inc.)
• Original Assignee: Bookham Incorporated (Oclaro (North America), Inc.)
• Inventors: Holden, Anthony, Zakhleniuk, Nick
• Application Number:
  US10/508,386
• Publication Number:
  US 20050175044A1
• Time in Patent Office: Days
• US Class Current: 372/20
• CPC Class Codes: B82Y 20/00 Nanooptics, e.g. quantum optics or photonic crystals
• CPC Class Codes: H01S 5/06256 with DBR-structure
• CPC Class Codes: H01S 5/3412 quantum box or quantum dash

Abstract

A tuneable laser including a light creating section to generate light and a tuneable section formed of a semiconductor material which utilises the electro-optic effect to achieve a change in the refractive index of the material, Δn, under the influence of an applied field, F, in accordance with the equation: Δn=−½n₀³[rF+sF²]≡Δn_L+Δn_Q, where n_o is the refractive index at zero field and Δn_L and Δn_Q are the linear and quadratic contributions to the change in refractive index respectively, r is the linear electro-optic coefficient of the material and s is the quadratic electro-optic coefficient of the material, the tuning section including a waveguide and the material of the waveguide incorporating a plurality of quantum dots and operating in a wavelength region where the value of rF is sufficiently greater than the value of sF², so as to operate with the dominant effect on Δn being contributed by the linear effect.

Claims

1. A tuneable laser, comprising a light creating section to generate light and a tuneable section formed of a semiconductor material which utilizes the electro-optic effect to achieve a change in the refractive index of the material, Δ

n, under the influence of an applied field, F, in accordance with the equation;

Δ

n=−

½

n₀³[rF+sF²]≡

Δ

n_L+Δ

n_Q

where n_o is the refractive index at zero field and Δ

n_L and Δ

n_Q are the linear and quadratic contributions to the change in refractive index respectively, r is the linear electro-optic coefficient of the material and s is the quadratic electro-optic coefficient of the material, the material incorporating a plurality of quantum dots and operating in a wavelength region where the value of rF is sufficiently greater than the value of sF², so as to operate with the dominant effect on Δ

n being contributed by the linear effect.

2. A tuneable laser as claimed in claim 1, wherein tuning section comprises a waveguide and the material of the waveguide includes the plurality of quantum dots operating in the wavelength region where the value of rF is sufficiently greater than the value of sF², so as to operate with the dominant effect on Δ

n being contributed by the linear effect.

3. A tuneable laser as claimed in claim 1, wherein a band-gap wavelength λ

_g of the quantum dots is shorter than a wavelength of the photons emitted by the light creating section.

4. A tuneable laser as claimed in claim 1, wherein a band-gap wavelength λ

_g of the quantum dots in the tuneable section is typically 100 nm shorter than the wavelength of the photons emitted by the light creating section.

14. A tuneable laser as claimed in claim 1, wherein the tuneable section is the tuning section of the laser.

15. A tuneable laser as claimed in claim 14, wherein the tuneable section incorporates a distributed Bragg reflector.

16. A tuneable laser as claimed in claim 15, wherein the distributed Bragg reflector is formed between two layers of different refractive indices and a plurality of quantum dots is provided in either of the layers between which the Bragg grating is formed.

17. A tuneable laser as claimed in claim 1, wherein the tuneable laser incorporates a phase change section and the phase change section is a tuneable section.

20. A tuneable laser as claimed in claim 1, wherein the laser comprises at least three sections.

21. A tuneable laser as claimed in claim 1, wherein the quantum dots are self-assembled quantum dots.

22. A tuneable laser as claimed in claim 21, wherein the self-assembled quantum dots are formed of one of an InGaAs and an InAs based material in a host GaAs based semiconductor material formed on a GaAs substrate.

26. A tuneable laser as claimed in claim 21, wherein the self-assembled quantum dots are formed of one of an InGaAs and an InAs based material in a host In_xGa_1-xAs_yP_1-y based semiconductor material formed on an InP substrate.

31. A tuneable laser as claimed in claim 1, further comprising a plurality of layers of quantum dots.

5. A tuneable laser, comprising a light creating section to generate light of a wavelength λ

and a tuneable section;

the tuneable section being formed of a semiconducting material incorporating a plurality of quantum dots and exhibiting an electro-optic response thereby to permit variation of the refractive index;

the band-gap of the semiconducting material incorporating the quantum dots being such that the corresponding wavelength λ

_g is less than λ

.

6. A tuneable laser according to claim 5, wherein the tuneable section comprises a waveguide being formed of the semiconducting material incorporating the plurality of quantum dots and exhibiting the electro-optic response thereby to permit variation of the refractive index.

7. A tuneable laser according to claim 5, wherein the wavelength λ

_g is less than 1400 nm.

8. A tuneable laser according to claim 5, wherein the wavelength λ

_g is less than 90% of λ

.

9. A tuneable laser according to claim 5, wherein the difference between λ

_g and λ

is greater than 100 nm.

10. A tuneable laser, comprising a light creating section to generate light and a tuneable section for adjusting the wavelength thereof within the range λ

₁ and λ

₂;

the tuneable section being formed of a semiconducting material incorporating a plurality of quantum dots and exhibiting an electro-optic response thereby to permit variation of the refractive index;

the band-gap of the semiconducting material incorporating the quantum dots is such that a corresponding wavelength λ

g is less than both λ

1 and λ

2 by an amount sufficient that the change in refractive index at λ

1 and λ

2 is substantially the same.

11. A tuneable laser according to claim 10, wherein the tuneable section including a waveguide;

being formed of the semiconducting material incorporating the plurality of quantum dots and exhibiting the electro-optic response thereby to permit variation of the refractive index.

12. A tuneable laser according to claim 10, wherein the difference in refractive index at λ

₁ and λ

₂ is less than 0.1% per nanometre of wavelength change.

13. A tuneable laser according to claim 10, wherein the difference between λ

₁ and λ

₂ is greater than 1 nm.

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