Method and apparatus for wavelength conversion and switching

US 6,433,919 B1
Filed: 05/19/2000
Issued: 08/13/2002
Est. Priority Date: 05/19/2000
Status: Expired due to Fees

First Claim

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1. Apparatus for simultaneous wavelength interchange of two optical signals of selected carrier frequencies ω

₁and ω

₂comprising;

(a) a lattice body comprising sensitized regions arranged in a two-dimensional array in a matrix material, the sensitized regions differing from the matrix material in the sign of the second order susceptibility, the spacing and pattern of the sensitized regions in the array selected to provide wavelength interchange for two optical signals at frequencies ω

₁and ω

₂;

(b) at least one input optical waveguide coupled to the lattice body by which the input signals at the frequencies ω

₁and ω

₂and a pump signal at a frequency ω

_pmay be coupled into the lattice body; and

(c) at least one output waveguide coupled to the lattice body in position to receive from the lattice body wavelength interchanged components of the input signals at least one of the frequencies ω

₁and ω

₂.

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Abstract

A two-dimensional second order nonlinear lattice formed in a lattice body is utilized for performing a one-step optical carrier wavelength interchange between pairs of input optical signals. The lattice body includes sensitized regions arranged in a two-dimensional array in a matrix material with the sensitized regions differing from the matrix material in the sign of the second order susceptibility. When an optical pump signal is coupled to the lattice body at a frequency corresponding to the sum of the frequencies of the two input signals, nonlinear interactions in the lattice body produce wavelength interchange between the input signals, resulting in angularly deflected optical signals exiting the lattice body in which the signal information on the input signals is interchanged between the carrier frequencies of the two input signals. The apparatus can be utilized to provide switching of optical signals and wavelength interchange for applications such as in wavelength division multiplexed communication systems.

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20 Claims

1. Apparatus for simultaneous wavelength interchange of two optical signals of selected carrier frequencies ω
- ₁and ω
  
  ₂comprising;
  
  (a) a lattice body comprising sensitized regions arranged in a two-dimensional array in a matrix material, the sensitized regions differing from the matrix material in the sign of the second order susceptibility, the spacing and pattern of the sensitized regions in the array selected to provide wavelength interchange for two optical signals at frequencies ω
  
  ₁and ω
  
  ₂;
  
  (b) at least one input optical waveguide coupled to the lattice body by which the input signals at the frequencies ω
  
  ₁and ω
  
  ₂and a pump signal at a frequency ω
  
  _pmay be coupled into the lattice body; and
  
  (c) at least one output waveguide coupled to the lattice body in position to receive from the lattice body wavelength interchanged components of the input signals at least one of the frequencies ω
  
  ₁and ω
  
  ₂.
- View Dependent Claims (2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12)
- - 2. The apparatus of claim 1 including a pump signal source coupled to an input waveguide to selectively provide an optical pump signal at a frequency ω
    - _p=ω
      
      ₁+ω
      
      ₂.
  - 3. The apparatus of claim 1 wherein the lattice body is formed of LiNbO₃and the sensitized regions are formed in the lattice body by periodic poling of the material of the lattice body to provide an opposite sign of the second order susceptibility in the sensitized regions from that of the matrix material surrounding the sensitized regions.
  - 4. The apparatus of claim 1 wherein there are at least two output waveguides coupled to the lattice body to receive from the lattice body spatially diverging wavelength interchanged components of the input signals at the frequencies ω
    - ₁and ω
      
      ₂.
  - 5. The apparatus of claim 1 including lateral waveguide regions formed on lateral sides of the lattice body to receive and guide light that has been deflected from the longitudinal direction of the incoming light by interaction with the lattice.
  - 6. The apparatus of claim 1 wherein the input waveguide comprises a fiber optic cable and the output waveguides comprise fiber optic cables.
  - 7. The apparatus of claim 6, including a pump source that selectively provides light at the pump wavelength ω
    - _p=ω
      
      ₁+ω
      
      ₂to a fiber optic cable and thence to a coupler the output of which is connected to a fiber optic cable comprising the input waveguide and wherein the coupler also is connected to a fiber optic cable on which is transmitted a pair of optical signals at carrier frequencies ω
      
      ₂and ω
      
      ₂that are to be interchanged.
  - 8. The apparatus of claim 6 further including a third output fiber optic cable coupled to the lattice body to receive the light from the input fiber optic cable that passes longitudinally through the lattice body without being deflected.
  - 9. The apparatus of claim 1 wherein the centers of the sensitized regions have spacings r_Aand r_Bin the two dimensions of the lattice given by the relation:
    - $r_{A, B} = \frac{2 π}{\langle \vec{G_{A, B}} \rangle \sin (φ)}$
10. The apparatus of claim 1 wherein the sensitized regions and the matrix material have the same first order susceptibility.
11. The apparatus of claim 1 wherein the pairs of input optical signals have carrier wavelengths in the 1.0 to 1.6 μ
- m wavelength range and the spacing between centers of sensitized regions in the lattice in the lattice body are in the range of about 5 to 10 μ
  
  m.
12. The apparatus of claim 1 wherein a single input optical waveguide is coupled to the lattice body by which the input signals at the frequencies ω
- ₁and ω
  
  ₂and the pump signal may be coupled into the lattice body collinear with one another.

13. A method for carrying out simultaneous wavelength interchange between two modulated optical signals at different carrier wavelengths comprising:
- (a) providing a lattice body comprising sensitized regions arranged in a two-dimensional array in a matrix material, the sensitized regions differing from the matrix material in the sign of the second order susceptibility, the spacing and pattern of the sensitized regions in the array selected to provide wavelength interchange for two optical signals at frequencies ω
  
  ₁and ω
  
  ₂;
  
  (b) coupling two input optical signals at the carrier frequencies ω
  
  ₁and ω
  
  ₂into the lattice body and coupling a third pump optical signal into the lattice body, the pump optical signal having a frequency ω
  
  _pselected to cause wavelength interchange in the lattice body between the two input optical signals;
  
  (c) receiving an output optical signal exiting from the lattice body angularly displaced from the direction of propagation of the input optical signals that comprises an optical signal at a carrier frequency ω
  
  ₂that carries the information on the input signal at the carrier frequency ω
  
  ₁, and receiving an output optical signal exiting from the lattice body angularly displaced from the direction of propagation of the input signals that comprises an optical signal at a carrier frequency ω
  
  ₁that carries the information on the input signal at the carrier frequency ω
  
  ₂.
- View Dependent Claims (14, 15, 16, 17)
- - 14. The method of claim 13 further including turning the pump signal on and off to switch on and off the signals exiting from the lattice body at an angle to the direction of propagation of the input signals to the lattice body.
  - 15. The method of claim 13 wherein the optical signals at the carrier frequencies ω
    - ₁and ω
      
      ₂and the pump signal at the frequency cop are coupled into the lattice body collinear with one another.
  - 16. The method of claim 13 wherein the pump signal has a frequency ω
    - _p=ω
      
      ₁+ω
      
      ₂, and wherein in the step of receiving an optical signal at a carrier frequency ω
      
      ₁that optical signal is angularly displaced from the direction of propagation of the output signal at the carrier frequency ω
      
      ₂.
  - 17. The method of claim 13 wherein the sensitized regions in the lattice body have the same first order susceptibility as the matrix material.

18. Apparatus for simultaneous wavelength interchange of two optical signals of selected carrier frequencies ω
- ₁and ω
  
  ₂comprising;
  
  (a) a lattice body comprising sensitized regions arranged in a two-dimensional array in a matrix material, the sensitized regions differing from the matrix material in the sign of the second order susceptibility and having the same first order susceptibility, the spacing and pattern of the sensitized regions in the array selected to provide wavelength interchange for two optical signals at frequencies ω
  
  ₁and ω
  
  ₂and wavelengths λ
  
  _Aand λ
  
  _B, respectively;
  
  (b) at least one input optical waveguide coupled to the lattice body by which the input signals at the frequencies ω
  
  ₁and ω
  
  ₂and a pump signal at a frequency ω
  
  _p=ω
  
  ₁+ω
  
  ₂and wavelength λ
  
  _pmay be coupled into the lattice body collinear with one another;
  
  (c) at least one output waveguide coupled to the lattice body in position to receive from the lattice body wavelength interchanged components of the input signals at least one of the frequencies ω
  
  ₁and ω
  
  ₂; and
  
  (d) wherein the centers of the sensitized regions in the lattice body have spacings r_Aand r_Bin the two dimensions of the lattice given by the relation;
  
  $r_{A} = \frac{2 π}{\langle \vec{G_{A}} \rangle \sin (φ)} and r_{B} = \frac{2 π}{\langle \vec{G_{B}} \rangle \sin (φ)}$ where φ
  
  is the interior angle subtended by the vectors r_Aand r_Band where |G_A| and |G_B| are the magnitudes of the reciprocal lattice vectors and are determined in accordance with;
  
  $\langle G_{A} \rangle = \frac{2 π n_{A}}{λ_{A}} \sqrt{{[1 - (\frac{n_{p} λ_{B} - n_{B} λ_{p}}{n_{A} (λ_{B} - λ_{p})})]}^{2} + 4 (\frac{n_{p} λ_{B} - n_{B} λ_{p}}{n_{A} (λ_{B} - λ_{p})}) \sin^{2} (θ_{A})}$ $\langle G_{B} \rangle = \frac{2 π n_{B}}{λ_{B}} \sqrt{{[1 - (\frac{n_{p} λ_{A} - n_{B} λ_{p}}{n_{B} (λ_{A} - λ_{p})})]}^{2} + 4 (\frac{n_{p} λ_{A} - n_{B} λ_{p}}{n_{B} (λ_{A} - λ_{p})}) \sin^{2} (θ_{B})}$ $and$ $\sin (φ) = \langle \sqrt{{(\frac{\langle \vec{k_{A}} \rangle}{\langle \vec{G_{A}} \rangle} \sin (2 θ_{A}))}^{2} - {(\frac{\langle \vec{k_{A}} \rangle}{\langle \vec{G_{A}} \rangle} \sin (2 θ_{A}) \frac{\langle \vec{k_{B}} \rangle}{\langle \vec{G_{B}} \rangle} \sin (2 θ_{B}))}^{2}} \pm \sqrt{{(\frac{\langle \vec{k_{B}} \rangle}{\langle \vec{G_{B}} \rangle} \sin (2 θ_{B}))}^{2} - {(\frac{\langle \vec{k_{A}} \rangle}{\langle \vec{G_{A}} \rangle} \sin (2 θ_{A}) \frac{\langle \vec{k_{B}} \rangle}{\langle \vec{G_{B}} \rangle} \sin (2 θ_{B}))}^{2}} \rangle$ where n_pis the refractive index in the lattice body for the pump signal, n_Ais the refractive index in the lattice body for the signal at the wavelength λ
  
  _A, n_Bis the refractive index in the lattice body for the signal at the wavelength λ
  
  _B, θ
  
  _Ais a selected desired half exit angle with respect to a normal to an output face of the lattice body for the output signal at the wavelength λ
  
  _A, θ
  
  _Bis a selected desired half exit angle with respect to a normal to the output face of the lattice body for the output signal at the wavelength λ
  
  _B, $\langle \vec{k_{A}} \rangle = 2 π n_{A} / λ_{A}, and$ $\langle \vec{k_{B}} \rangle = 2 π n_{B} / λ_{B} .$
- View Dependent Claims (19, 20)
- - 19. The apparatus of claim 18 wherein the lattice body is formed of LiNbO₃and the sensitized regions are formed in the lattice body by periodic poling of the material of the lattice body to provide an opposite sign of the second order susceptibility in the sensitized regions from that of the matrix material surrounding the sensitized regions.
  - 20. The apparatus of claim 18 wherein the lattice body is formed of a semiconductor and the sensitized regions are formed therein by selective disordering.

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Current Assignee
Wisconsin Alumni Research Foundation (University of Wisconsin System)
Original Assignee
Wisconsin Alumni Research Foundation (University of Wisconsin System)
Inventors
Chowdhury, Aref, McCaughan, Leon
Primary Examiner(s)
Lee, John D.

Application Number

US09/575,040
Time in Patent Office

816 Days
Field of Search

359/326-332, 359/117, 359/127, 359/128, 385/122, 372/21-22
US Class Current

359/332
CPC Class Codes

G02F 1/3534 Three-wave interaction, e.g...

G02F 2/004 Transferring the modulation...

Method and apparatus for wavelength conversion and switching

First Claim

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Abstract

78 Citations

20 Claims

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Method and apparatus for wavelength conversion and switching

First Claim

2 Assignments

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Abstract

78 Citations

20 Claims

Specification

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