Optical transmitter comprising a stepwise tunable laser

• US 6,611,546 B1
• Filed: 08/15/2001
• Issued: 08/26/2003
• Est. Priority Date: 08/15/2001
• Status: Active Grant

• Current Assignee: Blue Leaf IP Incorporated (CNH Industrial N.V.)
• Original Assignee: BlueLeaf, Inc.
• Inventors: Paldus, Barbara, Richman, Bruce, Romanini, Daniele, Katchanov, Alexandre, Knippels, Guido, Rella, Christopher, Garnache, Arnaud, Stoeckel, Frederic, Levenson, Marc
• Primary Examiner(s): Ip, Paul
• Assistant Examiner(s): Vy, Hung T
• Application Number:
  US09/930,841
• Time in Patent Office: 741 Days
• Field of Search: 372/92, 372/35, 372/103, 372/20, 372/99, 359/845
• US Class Current: 372/92
• CPC Class Codes: H01S 3/1062 using a controlled passive interferometer, e.g. a Fabry-Perot etalon
• CPC Class Codes: H01S 5/0217 Removal of the substrate
• CPC Class Codes: H01S 5/02253 using lenses
• CPC Class Codes: H01S 5/041 Optical pumping
• 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
• CPC Class Codes: H01S 5/18361 Structure of the reflectors, e.g. hybrid mirrors
• CPC Class Codes: H01S 5/18375 based on metal reflectors
• CPC Class Codes: H01S 5/18377 comprising layers of different kind of materials, e.g. combinations of semiconducting with dielectric or metallic layers

Abstract

An optical fiber transmitter for emitting an information-carrying laser beam comprises an optically or electrically pumped single mode MQW (multi quantum well) semiconductor amplifying mirror as a gain medium and a separate external reflector to form a cavity. The external cavity length defines a comb of optical modes, all or a subset of which corresponding to channel wavelengths of an optical telecommunications system having plural optical channels. The semiconductor gain element has a homogeneously broadened gain region; a tuning arrangement tunes the laser from mode to mode across the gain region thereby selecting each one of the plural optical channels. When the maximum gain bandwidth is less than mode-to-mode spacing defined by the cavity, that tuning arrangement comprises a means of altering the temperature of the amplifying mirror, thereby translating the frequency of the gain peak from one mode to another. An optical modulator adds modulation to a beam emitting from the laser to provide the information-carrying laser beam, and a coupler couples the information-carrying laser beam into an optical fiber of the optical telecommunications system. A calibration method based on detecting inter-mode optical transitions (mode hopping) is described. The parameters of the amplifying mirror and tuning arrangement can be adjusted during operation to switch quickly from one cavity mode to another in stepwise fashion.

Claims

1. A stepwise tunable external cavity laser, comprising an optical resonator, the resonator comprising:

a semiconductor amplifying mirror having a selected gain wavelength band and forming a first end of an optical resonator;

an external mirror forming a second end of the optical resonator, the external mirror being positioned such that a frequency comb of the optical resonator provides is aligned to a predetermined optical channel spacing arrangement; and

an electronically-actuated, frequency selective element, positioned within the optical resonator and having a control input to select an emission wavelength, of an optical beam emitted by the laser.

2. The laser of claim 1, wherein said amplifying mirror comprises an epitaxially grown monolithic semiconductor structure having a surface emitting gain region, the gain region including a plurality of active layers spaced apart by spacer layers, arranged to provide optical gain, and overlying a region of said amplifying mirror, the semiconductor structure comprising at least first and second layers of materials having different indices of refraction and selected to provide reflectivity greater than 95 percent over said gain wavelength band.

3. The laser of claim 1, wherein said amplifying mirror is excited to produce gain by radiation focused onto a selected region of said amplifying mirror.

4. The laser of claim 1, wherein said amplifying mirror is excited to produce gain by an electrical current.

5. The laser of claim 1, wherein said amplifying mirror is attached to a heat sink means that allows control of a temperature of said amplifying mirror.

6. The laser of claim 1, wherein said external mirror has a concave surface, with a radius of curvature that maintains a single transverse mode of oscillation over a selected range of optical pumping power, the concave surface being coated with at least first and second layers of dielectric materials having different indices of refraction and being selected to provide a reflectivity greater than 95 percent over said gain wavelength band.

7. The laser of claim 1, wherein said external mirror is planar, said laser further comprising a focusing element positioned within said optical resonator so that said optical resonator is centered within a selected resonator stability range.

8. The laser of claim 1, wherein said optical resonator further comprises at least one optical element, positioned between said amplifying mirror and said frequency selective element, to reduce angular divergence of an optical beam as the optical beam enters said frequency selective element.

9. The laser of claim 8, wherein said optical element comprises a lens.

10. The laser of claim 8, wherein said optical element comprises a concave mirror with a multi-layer dielectric coating.

11. The laser of claim 8, wherein said optical element comprises an off-axis parabolic mirror.

12. The laser of claim 1, wherein said frequency selective element comprises an intra-cavity etalon having an electronically-actuated control means to alter an angle between a normal to an etalon surface and a direction of propagation of an intra-cavity laser beam, whereby an emission wavelength of said laser is tunable.

13. The laser of claim 1, wherein said frequency selective element comprises a monolithic planar, air-spaced etalon comprising a free-standing dielectric film mirror, wherein a frequency of maximum transmission of the etalon is tunable by application of a variable voltage to the etalon.

14. The laser of claim 1, wherein said frequency selective element comprises a planar etalon, including a spacer medium comprising an electro-optically active material, wherein a frequency of maximum transmission of the etalon is tunable by application of a variable voltage to the spacer medium.

15. The laser of claim 14, wherein said spacer medium comprises a nematic or smectic liquid crystal.

16. The laser of claim 1, wherein said frequency selective element comprises:

a polarization selective element having a high transmission axis;

a birefringent electro-optical medium with an ordinary axis and an extraordinary axis oriented at substantially +45° and

at −

45°

respectively, with respect to the high transmission axis of the polarization selective element; and

voltage means for applying a selected voltage to the electro-optical medium, and for varying the selected voltage over a range of values that includes said gain wavelength band.

17. The laser of claim 1, wherein said frequency selective element comprises:

a polarization selective element having a high transmission axis;

a first birefringent electro-optical medium with an ordinary axis and an extraordinary axis oriented at substantially +45° and

−

45°

, respectively, with respect to the high transmission axis of the polarization selective element;

a second birefringent electro-optical medium with an ordinary axis and an extraordinary axis oriented so that the extraordinary axis of the second electro-optic medium is substantially aligned with the ordinary axis of the first electro-optic medium, and the ordinary axis of the second electro-optic medium is substantially aligned with the extraordinary axis of the first electro-optic medium; and

voltage means for applying a first selected voltage to the first electro-optical medium, for applying a second selected voltage to the second electro-optical medium, and for varying at least one of the first and second selected voltages over a range of values that includes said gain wavelength band,

whereby a total length of electro-optic media in said laser can be increased without reducing a laser tuning range, thereby allowing use of at least one of a reduced first selected voltage and a reduced second selected voltage.

18. The laser of claim 1, wherein said frequency selective element comprises:

a polarization selective element having a high transmission axis;

a first birefringent electro-optical medium with an ordinary axis and an extraordinary axis oriented at substantially +45° and

at −

45°

, respectively, with respect to the high transmission axis of the polarization selective element;

a second birefringent electro-optical medium with an ordinary axis and an extraordinary axis oriented such that the extraordinary axis of the second electro-optic medium is substantially aligned with the extraordinary axis of the first electro-optic medium, and the ordinary axis of the second electro-optic medium is substantially aligned with the ordinary axis of the first electro-optic medium;

a half-wave plate, positioned between the first electro-optic medium and the second electro-optic medium, oriented such that light polarized along an ordinary axis of the first electro-optical medium is substantially converted to light polarized along an extraordinary axis of the second electro-optical medium, and light polarized along an extraordinary axis of the first electro-optical medium is substantially converted to light polarized along an ordinary axis of the second electro-optical medium, in transmission through the half wave plate; and

voltage means for applying a first selected voltage to the first electro-optical medium and for applying a second selected voltage to the second electro-optical medium, and for varying at least one of the first and second selected voltages over a range of values that includes said gain wavelength band,

whereby an angular bandwidth of said frequency selective element is enhanced, and a total length of the electro-optic media in said laser can be increased without reducing a laser tuning range, thereby allowing use of at least one of a reduced first selected voltage and a reduced second selected voltage.

19. The laser of claim 1, wherein said frequency selective element comprises:

a polarization selective element having a high transmission axis;

a birefringent medium with an ordinary axis and an extraordinary axis oriented at substantially +45° and

−

45°

, respectively, with respect to the high transmission axis of the selective element;

a birefringent electro-optical medium with an ordinary axis and an extraordinary axis oriented at substantially −

45° and

+45°

, respectively, with respect to a high transmission axis of the polyarization selective element; and

voltage means for applying a selected voltage to said electro-optical medium and for varying the selected voltage over a range of values that includes said gain wavelength band.

20. The laser of claim 19, wherein said electro-optic medium comprises a nematic or smectic liquid crystal.