Tunable laser and method for operating the same

• US 5,949,801 A
• Filed: 07/22/1998
• Issued: 09/07/1999
• Est. Priority Date: 07/22/1998
• Status: Expired due to Fees

• Current Assignee: Coretek, Inc. (Nortel Networks Corporation)
• Original Assignee: Coretek, Inc. (Nortel Networks Corporation)
• Inventors: Tayebati, Parviz
• Primary Examiner(s): Scott, Jr., Leon
• Application Number:
  US09/123,391
• Time in Patent Office: 412 Days
• Field of Search: 372/20, 372/19, 372/106, 372/98, 372/6
• US Class Current: 372/20
• CPC Class Codes: H01S 3/0064 Anti-reflection devices, e.g. optical isolaters absorbing layers for marking or protecting purposes in laser working B23K26/50; magneto-optical non-reciprocal devices G02F1/093, G02F1/0955
• CPC Class Codes: H01S 5/0687 Stabilising the frequency of the laser
• CPC Class Codes: H01S 5/141 using a wavelength selective device, e.g. a grating or etalon H01S5/146 takes precedence

Abstract

A tunable laser and method for operating the same, wherein the tunable laser utilizes a tunable Fabry-Perot filter as its wavelength-selective component. In one form of the invention, the tunable laser is characterized by the provision of optical elements (hereinafter referred to as "optical operators" or just "operators") on either side of the tunable Fabry-Perot filter, whereby the tunable Fabry-Perot filter can be set at a right angle to the optical path of the laser without introducing reflection problems interfering with the optimum lasing.

Claims

1. A tunable laser comprising:

a gain medium defining a first relatively high reflectivity coated facet and a second relatively low reflectivity coated facet, said gain medium being adapted to generate a beam of light emerging from said second relatively low reflectivity coated facet;

a mirror disposed adjacent to, but spaced from, said second relatively low reflectivity coated facet and in alignment with said beam of light, said mirror having an appropriate curvature so as to define a stable laser cavity between said first relatively high reflectivity coated facet and said mirror;

a tunable Fabry-Perot filter disposed between said second relatively low reflectivity coated facet and said mirror, said tunable Fabry-Perot filter being disposed perpendicular to said beam of light;

lens apparatus disposed between said second relatively low reflectivity coated facet and said tunable Fabry-Perot filter, said lens apparatus being adapted to transform the intensity profile of the beam of light emerging from said gain medium so that the transformed profile of the beam of light emerging from said gain medium matches the lateral and transverse mode of said tunable Fabry-Perot filter; and

optical operators disposed on either side of said tunable Fabry-Perot filter and in alignment with said beam of light, said optical operators being adapted to transform said beam of light emerging from said second relatively low reflectivity coated facet so that (1) the wavelengths of light which are to be selected by said tunable Fabry-Perot filter can pass from said gain medium through said tunable Fabry-Perot filter to reach said mirror, and then return off said mirror and pass back through said tunable Fabry-Perot filter to re-enter said gain medium 10, and (2) any wavelengths of light reflected off said tunable Fabry-Perot filter back towards said gain medium will be prevented from re-entering said gain medium.

2. A tunable laser according to claim 1 wherein said optical operators comprise:

is a polarizer disposed between said relatively low reflectivity coated facet and said tunable Fabry-Perot filter;

a first Faraday rotator disposed between said polarizer and said tunable Fabry-Perot filter; and

a second Faraday rotator disposed between said tunable Fabry-Perot filter and said mirror.

3. A tunable laser according to claim 2 wherein said first Faraday rotator is adapted to rotate the state of polarization of light entering said first Faraday rotator by 45 degrees, and wherein said second Faraday rotator is adapted to rotate the state of polarization of light entering said second Faraday rotator by 45 degrees.

4. A tunable laser according to claim 2 wherein a thick etalon is disposed between said Fabry-Perot filter and said second Faraday rotator.

5. A tunable laser according to claim 4 wherein said thick etalon is designed to have a transmittance mode separated by integer multiples of 12.5 GHz.

6. A tunable laser according to claim 4 wherein said laser further comprises an active feedback loop adapted to monitor the output of the tunable laser and adjust the tuning voltage of said tunable Fabry-Perot filter so as to adjust the transmittance wavelength of said tunable Fabry-Perot filter so as to minimize noise.

7. A tunable laser according to claim 6 wherein said active feedback loop comprises a detector, a high pass frequency filter, and an integrator/feedback voltage generator.

8. A method for generating a laser beam of a selected wavelength, said method comprising the steps of:

proving a tunable laser comprising;

a gain medium defining a first relatively high reflectivity coated facet and a second relatively low reflectivity coated facet, said gain medium being adapted to generate a beam of light emerging from said second relatively low reflectivity coated facet;

a mirror disposed adjacent to, but spaced from, said second relatively low reflectivity coated facet and in alignment with said beam of light, said mirror having an appropriate curvature so as to define a stable laser cavity between said first relatively high reflectivity coated facet and said mirror;

a tunable Fabry-Perot filter disposed between said second relatively low reflectivity coated facet and said mirror, said tunable Fabry-Perot filter being disposed perpendicular to said beam of light;

lens apparatus disposed between said second relatively low reflectivity coated facet and said tunable Fabry-Perot filter, said lens apparatus being adapted to transform the intensity profile of the beam of light emerging from said gain medium so that the transformed profile of the beam of light emerging from said gain medium matches the lateral and transverse mode of said tunable Fabry-Perot filter; and

optical operators disposed on either side of said tunable Fabry-Perot filter and in alignment with said beam of light, said optical operators being adapted to transform said beam of light emerging from said second relatively low reflectivity coated facet so that (1) the wavelengths of light which are to be selected by said tunable Fabry-Perot filter can pass from said gain medium through said tunable Fabry-Perot filter to reach said mirror, and then return off said mirror and pass back through said tunable Fabry-Perot filter to re-enter said grain medium, and (2) any wavelengths of light reflected off said tunable Fabry-Perot filter back towards said gain medium will be prevented from re-entering said gain medium; and

tuning said tunable Fabry-Perot filter so as to set the transmittance mode of said tunable Fabry-Perot filter so as to vary the wavelength of laser oscillation.

9. A method according to claim 8 wherein said tunable laser further comprises a thick etalon disposed between said tunable Fabry-Perot filter and said mirror, and further wherein said tunable Fabry-Perot filter is tuned so that its transmittance peak matches the transmittance peak of said thick etalon.

10. A method according to claim 9 wherein said laser further comprises an active feedback loop adapted to monitor the output of the tunable laser and adjust the tuning voltage of said tunable Fabry-Perot filter so as to adjust the transmittance wavelength of said tunable Fabry-Perot filter so as to minimize noise.