System and method for high-power, pulsed ring fiber oscillator

• US 9,653,872 B2
• Filed: 06/04/2014
• Issued: 05/16/2017
• Est. Priority Date: 10/24/2005
• Status: Active Grant

• Current Assignee: Lockheed Martin Aculight Corp. (Martin Marietta Corporation)
• Original Assignee: Lockheed Martin Corporation (Martin Marietta Corporation)
• Inventors: Di Teodoro, Fabio, Vatter, Tracy W., Brooks, Christopher D., Savage-Leuchs, Matthias P., Royse, Robert W.
• Primary Examiner(s): VAN ROY, TOD THOMAS
• Application Number:
  US14/295,919
• Publication Number:
  US 20160204564A1
• Time in Patent Office: 1,077 Days
• CPC Class Codes: G02F 1/37 for second-harmonic generation G02F1/3532 takes precedence
• CPC Class Codes: H01S 3/0057 Temporal shaping, e.g. pulse compression, frequency chirping soliton generation and propagation G02F1/3513, H01S3/063 and H01S3/108
• CPC Class Codes: H01S 3/0092 Nonlinear frequency conversion, e.g. second harmonic generation [SHG] or sum- or difference-frequency generation outside the laser cavity nonlinear frequency conversion per se G02F1/35
• CPC Class Codes: H01S 3/06708 Constructional details of the fibre, e.g. compositions, cross-section, shape or tapering optical fibres as passive waveguides G02B6/02
• CPC Class Codes: H01S 3/06712 Polarising fibre; Polariser
• CPC Class Codes: H01S 3/06791 Fibre ring lasers fibre laser gyrometers G01C19/72
• CPC Class Codes: H01S 3/08027 by a filter, e.g. a Fabry-Perot filter is used for wavelength setting
• CPC Class Codes: H01S 3/094011 with bidirectional pumping, i.e. with injection of the pump light from both two ends of the fibre
• CPC Class Codes: H01S 3/09408 Pump redundancy
• CPC Class Codes: H01S 3/1103 Cavity dumping
• CPC Class Codes: H01S 3/115 using intracavity electro-optic devices
• CPC Class Codes: H01S 3/1618 ytterbium
• CPC Class Codes: H01S 3/2308 Amplifier arrangements, e.g. MOPA

Abstract

A ring laser includes a large-core rare-earth-doped fiber ring-connected with a free-space path having an electro-optic switch, output coupler, and intracavity band-pass filter to enforce lasing operation in narrow wavelength range. In some cavity-dumped modes, the laser is configured in a similar manner, except that an output coupler is omitted since the optical power is extracted from the laser cavity by the electro-optic switch itself. The same laser can be configured to operate in Q-switched and/or cavity-dumping modes as well as in hybrid modes (e.g., partial Q-switch, followed by cavity dumping, or even CW). In some embodiments, the laser can be used as, or inject laser light into, a regenerative solid-state amplifier, or a Raman laser, or can be also used to generate visible, ultra-violet, mid-infrared, and far-infrared (THz) radiation via nonlinear wavelength conversion processes. The various embodiments can use a power oscillator or seed-plus-amplifier MOPA configuration.

Claims

1. A method comprising:

providing a rare-earth doped first fiber gain medium;

configuring a ring optical signal path that extends through the first fiber gain medium;

Q-switching a ring signal laser beam in the ring optical signal path, wherein the Q-switched ring signal laser beam has a pulse repetition rate that is independent of the ring optical signal path'"'"'s length during normal operation of the Q-switching, and wherein the Q-switched ring signal laser beam has a first wavelength and propagates in the ring optical signal path in a first direction, wherein the Q-switching is one of a plurality of operational modes that are electrically switchable from one to another, and wherein the plurality of operational modes includes both a continuous-wave mode and a Q-switched mode;

extracting a first optical signal beam from the Q-switched ring signal laser beam in a free-space portion of the ring optical signal path;

separating from the free-space portion of the ring optical signal path at least a portion of any light counter-propagating in the ring optical signal path in a second direction other than the first direction, wherein the separating from the ring optical signal path is spatially separate from the extracting of the first optical signal beam; and

forcing a majority of the Q-switched ring signal laser beam to lase in the first direction around the ring optical signal path by reflecting at least a portion of any light separated from the ring optical signal path by the separating to propagate in the ring optical signal path in the first direction.

2. The method of claim 1, further comprising:

amplifying the first signal beam in a second fiber gain medium to form an amplified second output beam;

wavelength converting the amplified second output beam to form a wavelength-converted output beam that has a second wavelength different from the first wavelength.

3. The method of claim 1, wherein the extracting of the first optical signal beam from the Q-switched ring signal laser beam includes beam splitting light of a first polarization into the first optical signal beam while passing light of another polarization into a ring-feedback signal beam.

4. The method of claim 1, further comprising wavelength filtering the Q-switched ring signal laser beam to limit a linewidth of the Q-switched ring signal laser beam.

5. The method of claim 1, further comprising preferentially amplifying signal light having only a first linear polarization direction in the first fiber gain medium.

6. The method of claim 1, wherein the Q-switching includes polarizing the Q-switched ring signal laser beam, rotating an angle of polarization of the polarized Q-switched ring signal laser beam, and again polarizing the polarization-rotated Q-switched ring signal laser beam.

7. The method of claim 1, wherein the rare-earth doped first fiber gain medium is a large-mode-area (LMA) first fiber gain medium, the method further comprising providing a passive polarization-maintaining fiber, wherein the configuring of the ring optical signal path includes connecting an end of the LMA first fiber gain medium to the passive polarization-maintaining fiber.

8. An apparatus comprising:

a rare-earth doped first fiber gain medium;

means for configuring a ring optical signal path that extends through the first fiber gain medium;

means for Q-switching a signal laser beam in the ring optical signal path, wherein the Q-switched ring signal laser beam has a pulse repetition rate that is independent of the ring optical signal path'"'"'s length during normal operation of the means for Q-switching, and wherein the Q-switched ring signal laser beam has a first wavelength and propagates in the ring optical signal path in a first direction;

means for extracting a first optical signal beam from the Q-switched ring signal laser beam outside of the first fiber gain medium in a free-space portion of the ring optical signal path;

means for separating from the free-space portion of the ring optical signal path at least a portion of any light counter-propagating in the ring optical signal path in a second direction other than the first direction, wherein the means for separating is spatially separate from the means for extracting; and

means for forcing the Q-switched ring signal laser beam to lase in a single first direction around the ring optical signal path, including means for reflecting, to propagate in the ring optical signal path in the single first direction, at least a portion of any light separated from the ring optical signal path by the means for separating, wherein the means for Q-switching is operable in one of a plurality of operational modes that are electrically switchable from one to another, and wherein the plurality of operational modes includes both a continuous-wave mode and a Q-switched mode.

9. The apparatus of claim 8, wherein the means for extracting the first optical signal beam from the Q-switched ring signal laser beam includes means for beam splitting light of a first polarization into the first optical signal beam while passing light of another polarization into a ring-feedback signal beam.

10. The apparatus of claim 8, further comprising means for wavelength filtering the Q-switched ring signal laser beam to limit a linewidth of the Q-switched ring signal laser beam.

11. The apparatus of claim 8, wherein the means for configuring the ring optical signal path includes means for maintaining a polarization of the Q-switched ring signal laser beam in a portion of the ring optical signal path outside of the first fiber gain medium.

12. The apparatus of claim 8, further comprising means for preferentially amplifying signal light having only a first linear polarization direction in the first fiber gain medium.

13. The apparatus of claim 8, wherein the rare-earth doped first fiber gain medium is a large-mode-area (LMA) first fiber gain medium, the apparatus further comprising:

a passive polarization-maintaining fiber, wherein the means for configuring the ring optical signal path includes means for connecting an end of the LMA first fiber gain medium to the passive polarization-maintaining fiber.

14. An apparatus comprising:

a ring laser that has an optical signal ring path and generates a Q-switched ring signal laser beam that propagates along the optical signal ring path in the ring laser, wherein the Q-switched ring signal laser beam has a pulse repetition rate that is independent of the optical signal ring path'"'"'s length during normal Q-switched mode, wherein the Q-switched ring signal laser beam has a first wavelength and propagates in the optical signal ring path in a first direction, wherein the ring laser includes a first optical fiber that forms a first portion of the optical signal ring path, and wherein the first optical fiber includes an optically-pumped rare-earth-doped gain-fiber section;

first extraction optics configured to extract a first signal beam from the Q-switched ring signal laser beam in a free-space portion of the optical signal ring path;

second extraction optics, separate from the first extraction optics, that separates from the optical signal ring path at least a portion of any light that counter-propagates in the free-space portion of the optical signal ring path in a second direction other than the first direction; and

a first high-reflectivity mirror, wherein the first mirror is configured to reflect toward the first direction around the optical signal ring path at least a portion of any light separated from the optical signal ring path by the second extraction optics in order to control the Q-switched ring signal laser beam to lase in only the first direction around the optical signal ring path, wherein the ring laser operates in one of a plurality of operational modes that are electrically switchable from one to another, and wherein the plurality of operational modes includes both a continuous-wave mode and the Q-switched mode.

15. The apparatus of claim 14, further comprising:

a rare-earth-doped optical-fiber power amplifier that is optically coupled to receive the first signal beam and that has a power-gain-fiber section configured to generate an amplified second signal beam; and

a wavelength-conversion device optically coupled to receive the amplified second signal beam and configured to form a wavelength-converted output beam that has a second wavelength different from the first wavelength.

16. The apparatus of claim 15, wherein the optical-fiber power amplifier includes a passive polarization-maintaining delivery fiber that couples the amplified output beam out of a second end of the power-gain-fiber section.

17. The apparatus of claim 14, wherein the gain-fiber section of the first optical fiber includes a large-mode-area (LMA) gain-fiber section, wherein the first optical fiber further includes a passive polarization-maintaining fiber section connected to an end of the LMA gain-fiber section.

18. The apparatus of claim 14, wherein the gain-fiber section of the first optical fiber includes a large-mode-area (LMA) gain-fiber section.

19. The apparatus of claim 14, further comprising:

a rare-earth-doped optical-fiber power amplifier that is optically coupled to receive the first signal beam and that has a power-gain-fiber section configured to generate an amplified second output beam; and

a first pump port configured to guide pump light into the optical-fiber power amplifier.

20. The apparatus of claim 14, further comprising:

a first pump port optically coupled to inject pump light into the free-space portion of the optical signal ring path; and

a pump laser operatively coupled to launch pump light through the first pump port into the optical signal ring path in a direction counter-propagating to the Q-switched ring signal laser beam.