Athermal external cavity laser

• US 7,580,441 B2
• Filed: 12/05/2006
• Issued: 08/25/2009
• Est. Priority Date: 12/07/2005
• Status: Active Grant

• Current Assignee: Electronics and Telecommunications Research Institute
• Original Assignee: Electronics and Telecommunications Research Institute
• Inventors: Jeong, Geon, Kim, Byoung Whi, Lee, Woo Ram, Cho, Seung Hyun, Lee, Jie Hyun, Park, Mahn Yong, Kim, Chul Young
• Primary Examiner(s): Nguyen; Dung T
• Application Number:
  US11/634,792
• Publication Number:
  US 20070127538A1
• Time in Patent Office: 994 Days
• Field of Search: 372/34, 372/92, 372/6
• US Class Current: 372/92
• CPC Class Codes: G02B 6/0218 using mounting means, e.g. by using a combination of materials having different thermal expansion coefficients
• CPC Class Codes: G02B 6/0219 based on composition of fibre materials
• CPC Class Codes: G02B 6/4206 Optical features G02B6/4207, G02B6/421 take precedence
• CPC Class Codes: H01S 5/02251 using optical fibres
• CPC Class Codes: H01S 5/02253 using lenses
• CPC Class Codes: H01S 5/0654 Single longitudinal mode emission
• CPC Class Codes: H01S 5/141 using a wavelength selective device, e.g. a grating or etalon H01S5/146 takes precedence
• CPC Class Codes: H01S 5/142 which comprises an additional resonator
• CPC Class Codes: H01S 5/146 using a fiber as external cavity

Abstract

Provided is an athermal external cavity laser (ECL), whose output optical power and output wavelength can be kept regular irrespective of temperature changes without using additional temperature controlling components. The ECL comprises: a semiconductor amplifier; an optical fiber comprising a core in which a Bragg grating is formed and a cladding surrounding the core; and a thermosetting polymer that fixes the optical fiber to a ferrule and has a negative thermooptical coefficient, wherein the thickness of the cladding surrounding the core in which the Bragg grating is formed is smaller than the portion of the cladding surrounding the portion of the core where the Bragg grating is not formed, and the thermosetting polymer the negative thermooptical coefficient surrounds the cladding. The ECL does not need additional temperature controlling components and thus can be manufactured compact and at low cost, and thus can be used as a light source of a dense wavelength division multiplexing (DWDM) system in designing economical WDM passive optical networks (PON).

Claims

1. An athermal external cavity laser (ECL) comprising:

a semiconductor amplifier;

an optical fiber comprising a core in which a Bragg grating is formed and a cladding surrounding the core; and

a thermosetting polymer that fixes the optical fiber to a ferrule and has a negative thermooptical coefficient,

wherein the thickness of the cladding surrounding the core in which the Bragg grating is formed is smaller than that of the cladding surrounding region of the core in which the Bragg grating is not formed, and the thermosetting polymer surrounds the cladding.

2. The athermal ECL of claim 1, wherein reflection spectrums of the Bragg grating are kept athermal by the thermosetting polymer.

3. The athermal ECL of claim 2, wherein the output optical power of the ECL is athermal.

4. The athermal ECL of claim 1, wherein the thickness of the cladding around the Bragg grating is 0.2 to 0.4 μ

m, the thermooptical coefficient of the thermosetting polymer is −

1×

10<sup>−

4</sup>/deg to −

1.6×

10<sup>−

4</sup>/deg, and the refractive index of the thermosetting polymer is 1.43 to 1.445.

5. The athermal ECL of claim 1, further comprising an optical path compensator between the semiconductor amplifier and the optical fiber.

6. The athermal ECL of claim 5, wherein the ECL is a single-mode ECL, and the optical path compensator makes the length of the optical path in which the external cavity is formed athermal, so as to make the output wavelength of the ECL athermal.

7. The athermal ECL of claim 5, wherein the thermooptical coefficient of the optical path compensator is −

1×

10<sup>−

4</sup>/deg to −

2.5×

10^{31 4}/deg, and the length of the optical path of the optical path compensator is 500 to 2000 μ

m.

8. The athermal ECL of claim 7, wherein the ECL is formed in a TO-CAN package and comprises a focusing lens for improving the optical combination efficiency of the semiconductor amplifier and the optical fiber;

and

when a length of the optical path of the semiconductor amplifier is 600 μ

m, a thermooptical coefficient is 2.2×

10<sup>−

4</sup>/deg, a length of the optical path of the focusing lens is 1000 μ

m, a length of the Bragg grating is 4000 μ

m, and a thermooptical coefficient of the Bragg grating is 0.1×

10<sup>−

4</sup>/deg, the thermooptical coefficient of the optical path compensator is −

1.0×

10<sup>−

4</sup>/deg and the length of the optical path is 1200 μ

m.

9. The athermal ECL of claim 5, wherein a front surface and a rear surface of the optical path compensator are anti-reflection (AR) coated, and

the front surface and the rear surface are inclined at a predetermined angle with respect to the perpendicular of the optical path.

10. The athermal ECL of claim 9, wherein the inclination angle is 1 to 3°

.

11. The athermal ECL of claim 1, wherein a cross-section of the optical fiber is coated AR-coated;

or inclined at 8°

to the perpendicular of the optical path;

or is AR-coated and inclined at 8°

to the perpendicular of the optical path.

12. The athermal ECL of claim 1, wherein the ECL is a multi-mode ECL, and the reflection bandwidth of the Bragg grating and the length of the external cavity are controlled.