Laser having a passive pulse modulator and method of making same

• US 5,666,373 A
• Filed: 02/06/1996
• Issued: 09/09/1997
• Est. Priority Date: 02/06/1996
• Status: Expired due to Fees

• Current Assignee: Raytheon Company (Rtx Corporation)
• Original Assignee: Raytheon Company (Rtx Corporation)
• Inventors: Pan, Noren, Spock, Derek E., Sharp, Richard C.
• Primary Examiner(s): Healy, Brian
• Application Number:
  US08/597,330
• Time in Patent Office: 581 Days
• Field of Search: 372/6, 372/7, 372/9, 372/10, 372/11, 372/18, 372/19, 372/21, 372/22, 372/23, 372/25, 372/26, 372/28, 372/30, 372/43, 372/50, 372/92, 372/98, 372/99, 372/96, 372/108, 437/51, 437/126, 437/129
• US Class Current: 372/18
• CPC Class Codes: G02F 1/3523 Non-linear absorption changing by light, e.g. bleaching
• CPC Class Codes: H01S 2303/00 Pumping wavelength
• CPC Class Codes: H01S 3/067 Fibre lasers
• CPC Class Codes: H01S 3/0675 Resonators including a grating structure, e.g. distributed Bragg reflectors [DBR] or distributed feedback [DFB] fibre lasers
• CPC Class Codes: H01S 3/08059 Constructional details of the reflector, e.g. shape mirrors in general G02B5/08; mountings for mirrors G02B7/18
• CPC Class Codes: H01S 3/09415 the pumping beam being parallel to the lasing mode of the pumped medium, e.g. end-pumping
• CPC Class Codes: H01S 3/1118 Semiconductor saturable absorbers, e.g. semiconductor saturable absorber mirrors [SESAMs]; Solid-state saturable absorbers, e.g. carbon nanotube [CNT] based
• CPC Class Codes: H01S 3/1616 thulium

Abstract

A laser having a gain medium disposed in a resonant cavity having a pair of end reflectors. One of such reflectors has a reflectivity lower than the reflectivity of the other one of the reflectors. The reflectors are arranged to provide a single ended output for the cavity through the one of the reflectors having the lower reflectivity. A saturable absorber is formed on the one of the reflectors having the lower reflectivity. With such an arrangement, fabrication of the saturable absorber on the single ended output coupler is greatly simplified. The gain medium is a doped fiber and the saturable absorber formed on the one of the reflectors having the lower reflectivity is affixed to an end of the doped fiber gain medium. With such an arrangement, a highly efficient, relatively low cost, mode locked laser is provided.

Claims

1. A laser, comprising:

a pair of end reflectors;

a resonant cavity having a gain medium disposed therein between the pair of end reflectors;

one of such reflectors having a reflectivity lower than the reflectivity of the other one of the reflectors;

the reflectors being arranged to provide a single ended output for the cavity through the one of the reflectors having the lower reflectivity; and

a saturable absorber integrally formed on the one of the reflectors having the lower reflectivity. affixed to an end of the doped fiber gain medium.

2. The laser recited in claim 1 wherein the gain medium is a doped fiber and the saturable absorber formed on the one of the reflectors having the lower reflectivity is affixed to an end of the doped fiber gain medium.

3. The laser recited in claim 2 wherein the gain medium comprises a thulium-doped silica fiber.

4. The laser recited in claim 3 including a diode pump laser arranged to pump the laser gain medium into spontaneous emission.

5. The laser recited in claim 4 wherein the diode laser is single-frequency diode laser.

6. The laser recited in claim 5 wherein the diode laser emits light having a wavelength in the order of 786 nm.

7. The laser recited in claim 6 wherein the diode laser produced light having a power level in the order of 50 mW.

8. The laser recited in claim 6 including a microlens attached to an output end of the diode laser.

9. The laser recited in claim 3 wherein the fiber is here fabricated by modified chemical deposition (MCVD) and has the central 25% of the core thulium-doped to 19000 ppm.

10. The laser recited in claim 9 wherein the fiber has a numerical aperture of 0.37, cutoff wavelength of 1.37 μ

m, core diameter of 2.8 μ

m, ³ F₄ fluorescence lifetime of 1 ms, and a small signal absorption coefficient of 0.5 dB/cm at 786 nm.

11. A laser, comprising:

a pair of end reflectors;

a resonant cavity having a gain medium disposed therein between the pair of end reflectors;

one of such reflectors having a reflectivity lower than the reflectivity of the other one of the reflectors to provide a output coupler for the laser;

a saturable absorber integrally formed with the output coupler as a single monolithic structure.

12. The laser recited in claim 11 wherein the gain medium is a doped fiber and the monolithic structure is affixed directly to an end of the doped fiber gain medium.

13. The laser recited in claim 12 wherein the output coupler comprises a distributed Bragg reflector.

14. The laser recited in claim 13 wherein the distributed Bragg reflector comprises:

an InP substrate;

a plurality of pairs of quarter-wave thick layers of alternating lattice-matched In_x Ga_1-x As, where x=0.53, and InP.

15. The laser recited in claim 14 wherein the saturable absorber comprises:

a plurality of pairs of a layers of strained In_y Ga_1-y As quantum wells and lattice matched barrier layers epitaxially deposited on the distributed Bragg reflector.

16. The laser recited in claim 15 where y=0.70.

17. The laser recited in claim 16 wherein the laser emits pulses of light having a wavelength between 1.8-2.0 μ

m and wherein the band edge of the superlattice of the saturable absorber is very near the wavelength of the pulses emitted by the laser.

18. The laser recited in claim 17 including anti-reflection coatings at 1.8 to 2 μ

m disposed on the monolithic structure.

25. The laser recited in claim 13 wherein the distributed Bragg reflector comprises:

a substrate;

a plurality of pairs of quarter-wave thick layers of alternating layers of material lattice-matched to the substrate; and

wherein the saturable absorber comprises;

a plurality of pairs of layers, each one of the pairs including a quantum well layer and a barrier layer, such plurality of layers being epitaxially deposited on the distributed Bragg reflector.

26. The laser recited in claim 25 wherein one of the layers in each one of the pairs of layers of the saturable absorer is a crystallographically strained layer.

19. A method of forming an output structure and saturable absorber, comprising the steps of:

providing a semiconductor substrate;

epitaxially growing substrate a plurality of pairs of layers of material lattice matched to the substrate to provide a distributed Bragg reflector output structure;

epitaxially forming on the distributed Bragg reflector output structure a plurality of pairs of layers of material to form a saturable absorber integrally with the distributed Bragg reflector output structure.

20. The method recited in claim 19 including additionally the step of affixing, in abutment to, a laser gain medium.

21. The method recited in claim 20 wherein the gain medium is a doped silica fiber.

22. The method recited in claim 21 wherein the substrate is III-V material.

23. The method recited in claim 22 wherein the doped fiber is thulium doped.

24. The method recited in claim 19 wherein at least one of the layers is crystallographically strained with respect to the substrate.