Continuously variable attenuation of an optical signal using an optical isolator

1. A variable optical attenuation device, the device comprising:

an optical signal source generating an optical signal that is polarized in an original polarization direction D;

an optical isolator located to receive the optical signal, wherein the optical isolator includes:

a first polarizer that transmits only light that is substantially polarized in a first polarizer direction T 1 ;

a polarization rotator optically coupled to the first polarizer for rotating the optical signal by a predetermined angle; and

a second polarizer optically coupled to the polarization rotator, the second polarizer transmitting only light that is polarized in a second polarizer direction T 2 that is different from the first polarization direction T 1 ;

means for rotating at least one of the optical isolator and the optical signal source to adjust an angle θ, wherein the angle θ is the angle between the original polarization direction D and the polarizer direction T 1 ; and

wherein the predetermined angle is equal to the difference between the first polarizer direction T 1 and the second polarizer direction T 2 .

2. The device of claim 1 , wherein the predetermined angle is approximately 45°.

3. The device of claim 1 , wherein the polarization rotator is a Faraday rotator.

4. The device of claim 1 , further comprising a signal transfer medium optically coupled to the optical isolator, the signal transfer medium receiving the optical signal from the optical isolator.

5. The device of claim 4 , wherein the signal transfer medium is an optical fiber.

6. The device of claim 4 , wherein the signal transfer medium reflects a portion of the optical signal, forming a back-reflected light traveling from the input end toward the optical isolator, and wherein the optical isolator prevents substantially all of the back-reflected light from reaching the optical signal source.

7. The device of claim 6 , wherein the optical signal is rotated by approximately 45° in a direction A while propagating toward the signal transfer medium and the back-reflected light is also rotated by approximately 45° in the direction A so that the back-reflected light is polarized in a direction that is substantially orthogonal to the polarization direction T 1 .

8. The device of claim 4 , further comprising a focusing element for focusing the optical signal into the input end of the signal transfer medium.

9. The device of claim 1 , wherein the means for rotating allows the angle θ to be adjusted continuously.

10. The device of claim 1 , further comprising a module housing holding the optical isolator, wherein the module housing is positioned on a rotating surface that rotates the optical isolator relative to the optical signal source.

11. A method of controlling the intensity of an optical signal, the method comprising:

adjusting an angle θ, which is the difference between an original polarization direction D of the optical signal and a polarizer direction T 1 , wherein the optical signal is generated by an optical signal source and the polarizer is located inside an optical isolator; and

wherein the adjustment comprises rotating at least one of the optical signal source and the optical isolator comprising the steps of:

obtaining a module housing and placing the optical isolator therein;

inserting the optical signal source into the module housing such that the module housing is rotatable relative to the optical signal source;

and determining an orientation of the polarizer direction T 1 .

12. The method of claim 11 further comprising coupling the optical signal into a signal transfer medium that creates a back-reflected light traveling toward the optical signal source, wherein the optical isolator reduces the amount of back reflected light that reaches the optical signal source.

13. The method of claim 12 further comprising rotating the optical signal and the back-reflected light by a predetermined angle using a Faraday rotator that is a part of the optical isolator.

14. The method of claim 11 , wherein determining the orientation of the polarizer direction T 1 comprises at least one of:

maximizing a power level of an output exiting the optical isolator;

minimizing the power level of the output and rotating the optical isolator by 90° relative to the optical signal source;

and selecting an angle between two power level minima.

15. The method of claim 11 , wherein determining the orientation of the polarizer direction T 1 comprises:

adjusting the angle θ;

and measuring the transmission power as a function of θ.

16. The method of claim 11 further comprising:

rotating the optical signal coming out of the polarizer by approximately 45° in a direction A so that most of the optical signal has a polarization direction T 2 ;

allowing only the portion of the optical signal having the polarization direction T 2 to reach a signal transfer medium;

and rotating the portion of the optical signal that is reflected back toward the optical signal source by approximately 45° in the direction A so that most of the optical signal has a polarization direction that is orthogonal to T 1 and are blocked by the polarizer.

17. The method of claim 16 , wherein rotating the optical signal and rotating the portion of the optical signal that is reflected back both include using a Faraday rotator.

18. The method of claim 11 , wherein the adjustment is done continuously to achieve the desired intensity.

19. An optical transmitter module comprising:

a module housing;

an optical signal source generating a light that is substantially polarized in a direction D;

and an optical isolator located inside the module housing, the optical isolator including a polarizer that transmits only light that is substantially polarized in a polarizer direction T 1 and receiving the light generated by the optical signal source, wherein the optical isolator is rotatable to adjust an angle θ between the direction D and the polarizer direction T 1 to control a power level of the light exiting the optical isolator.