Modulation suppression in fiber lasers and associated devices

Patent metadata

Field	Value
Publication number	US-10193299-B2
Application number	US-201715473924-A
Country	US
Kind code	B2
Filing date	Mar 30, 2017
Priority date	Mar 30, 2017
Publication date	Jan 29, 2019
Grant date	Jan 29, 2019

Abstract

A system and method for an active Q-switched fiber laser cavity may include a pump source for emitting a laser beam at a wavelength along an optical path including an active optical medium. A modulation device may be configured to introduce tunable losses into the optical path. The tunable losses may be achieved through modulation of the transmissivity of an optical element within the optical path, the modulation of said optical element being performed over (i) a first period of time in which a cavity Q curve increases from a first percentage value to a second percentage value of a maximum Q value and (ii) a second period of time in which the cavity Q curve increases from a third percentage value to a fourth percentage value of the maximum Q value. The cavity Q curve may non-linearly and smoothly transition between (i) the first and second percentage values and (ii) the third and fourth percentage values.

First claim

What is claimed:

1. A system for an actively Q-switched fiber laser cavity, said system comprising:
an optical resonator (cavity);
a pump source for emitting a laser beam at a wavelength along an optical path;
an active optical medium disposed in the optical cavity along the optical path;
an electronic circuit configured to:
first low-pass filter a square wave to form a first low-pass filtered signal; and
second low-pass filter the first low-pass filtered signal to create a smooth rise wave in the first low-pass filtered signal to form a second low-pass filtered signal, the second low-pass filtered signal being an input signal to control the modulation of the laser beam; and

a modulation device in electrical communication with said electronic circuit to receive the second low-pass filtered signal as an input signal, and configured to introduce tunable losses into the optical path, the tunable losses inducing a modulation as a function of the second low-pass filtered signal of the cavity Q, the modulation of the cavity Q being performed over (i) a first period of time in which a cavity Q curve increases from a first percentage value to a second percentage value of a maximum Q value and (ii) a second period of time in which the cavity Q curve increases from a third percentage value to a fourth percentage value of the maximum Q value, the cavity Q curve non-linearly and smoothly transitioning between (i) the first and second percentage values and (ii) the third and fourth percentage values.

2. The system according to claim 1 , wherein the first percentage value is approximately zero percent, wherein the second percent value is approximately twenty percent, wherein the third percent value is approximately ten percent, and wherein the fourth percentage value is approximately ninety percent.

3. The system according to claim 1 , wherein the modulation device is a radiofrequency (RF) driven device.

4. The system according to claim 3 , wherein the modulation device is an acousto-optic modulator.

5. The system according to claim 4 , wherein said circuit is configured to apply an input signal into said modulation device to cause said modulation device to modulate the laser beam.

6. The system according to claim 4 , wherein said circuit is configured to shape the input signal, and including:
a first low-pass filter circuit; and
a second low-pass filter circuit serially connected to the output of the first low-pass filter circuit.

7. The system according to claim 1 , comprising a first highly reflective Fiber Bragg Grating (FBG) in the optical path interposed between the pump source and the active optical medium, the first FBG configured to reflect the laser at a first filtered wavelength.

8. The system according to claim 7 , further comprising a second partly reflective Fiber Bragg Grating (FBG) optically coupled to the output of the modulation device, the second FBG configured to partly transmit the laser at the same first filtered wavelength, the second FBG further configured to be an output coupler of the laser cavity.

9. The system according to claim 1 , wherein the active optical medium is an Ytterbium-doped active fiber.

10. The system according to claim 1 , wherein the first period of time is approximately the same as a laser cavity round-trip time.

11. The system according to claim 1 , wherein the second period of time is approximately the same as a laser cavity round-trip time.

12. A method for suppressing amplitude modulation in an actively Q-switched fiber laser cavity, the method comprising:
emitting a pump laser beam at a wavelength into an optical path;
first low-pass filtering a square wave to form a first low-pass filtered signal;
second low-pass filtering the first low-pass filtered signal to create a smooth rise wave in the first low-pass filtered signal to form a second low-pass filtered signal, the second low-pass filtered signal being an input signal to control the modulation of the laser beam;
modulating the transmissivity of an optical component in the optical path as a function of the second low-pass filtered signal to cause tunable losses, the modulation of the transmissivity of said optical component being performed over a first period of time during which a cavity Q curve increases from a first percentage value to a second percentage value of a maximum Q value and over a second period of time in which the cavity Q curve increases from a third percentage value to a fourth percentage value of the maximum Q value, the cavity Q curve non-linearly and smoothly transitioning between (i) the first and second percentage values and (ii) the third and fourth percentage values, thereby producing a modulated first filtered laser beam; and
reflecting the modulated first filtered laser beam at a second filtered wavelength to output a second filtered laser beam.

13. The method according to claim 12 , wherein the first percentage value is approximately zero percent, wherein the second percent value is approximately twenty percent, wherein the third percent value is approximately ten percent, and wherein the fourth percentage value is approximately ninety percent.

14. The method according to claim 12 , wherein the first period of time is approximately the same as a laser cavity round-trip time.

15. The method according to claim 14 , wherein the second period of time is approximately the same as the laser cavity round-trip time.

16. A method for suppressing amplitude modulation in an actively Q-switched fiber laser cavity, said method comprising:
first low-pass filtering a square wave to form a first low-pass filtered signal;
creating a smooth rise wave in the first low-pass filtered signal to form a second low-pass filtered signal; and
applying the second low-pass filtered signal to a modulator within an optical path of the actively Q-switched fiber laser cavity to introduce tunable losses into the actively Q-switched fiber laser cavity.

17. The method according to claim 16 , further comprising emitting a laser beam at a wavelength along an optical path within the Q-switched fiber laser cavity.

18. The method according to claim 16 , wherein introducing tunable losses into the active Q-switched fiber laser cavity includes modulating the cavity Q by introducing tunable losses, the modulation of the cavity Q being performed over a first period of time in which a cavity Q curve increases from a first percentage value to a second percentage value of a maximum Q value and over a second period of time in which the cavity Q curve increases from a third percentage value to a fourth percentage value of the maximum Q value, the cavity Q curve non-linearly and smoothly transitioning between (i) the first and second percentage values and (ii) the third and fourth percentage values in response to the third low-pass filtered signal being applied to the modulator.

19. The method according to claim 18 , wherein the first period of time is approximately the same as a laser cavity round-trip time.

Assignees

• Datalogic IP Tech Srl

Inventors

• Arcangeli Andrea
• Hammouda Mihamed

Classifications

• H01S3/169

  Nanoparticles, e.g. doped nanoparticles acting as a gain material · CPC title

• H01S3/0675

  Resonators including a grating structure, e.g. distributed Bragg reflectors [DBR] or distributed feedback [DFB] fibre lasers · CPC title

• H01S3/117 Primary

  using intracavity acousto-optic devices · CPC title

• G02F1/113

  Circuit or control arrangements · CPC title

• H01S3/10046

  Pulse repetition rate control (H01S3/11 takes precedence) · CPC title