Divided pulse lasers
Methods, systems, and devices are disclosed for divided-pulse lasers. In one aspect, a pulsed laser is provided to include a laser cavity including an optical amplifier and a plurality of optical dividing elements and configured to direct a laser pulse of linearly polarized light into the plurality of optical dividing elements to divide the light of the laser pulse into a sequence of divided pulses each having a pulse energy being a portion of the energy of the laser pulse before entry of the optical dividing elements, to subsequently direct the divided pulses into the optical amplifier to produce amplified divided pulses. The laser cavity is configured to direct the amplified divided pulses back into the plurality of optical dividing elements for a second time in an opposite direction to recombine the amplified divided pulses into a single laser pulse with greater pulse energy as an output pulse of the laser cavity.
1. A pulsed laser that generates high energy pulses by dividing laser pulses and recombining laser pulses within a laser cavity, comprising:
an optical cavity including a first mirror, and a second mirror to direct light to travel between the first mirror and the second mirror;
a set of optical dividing/combining elements positioned between the first mirror and the second mirror within the optical cavity and having a first side and second side;
an optical amplifier positioned within the optical cavity on the second side of the set of optical dividing/combining elements;
wherein the optical cavity is configured to:
direct a laser pulse of linearly polarized light into the set of optical dividing/combining elements from the first side to divide the laser pulse into a sequence of temporally spaced sub-pulses, wherein each sub-pulse has a lower pulse energy than an input laser pulse; and
direct the sequence of sub-pulses into the optical amplifier to produce a sequence of amplified sub-pulses;
wherein the first mirror is configured to direct the sequence of amplified sub-pulses back into the set of optical dividing/combining elements from the second side to recombine the sequence of amplified sub-pulses into a single amplified laser pulse having a greater pulse energy than the laser pulse; and
wherein the optical cavity is configured to output a portion of the single amplified laser pulse as the output pulse of the pulsed laser.
2. The pulsed laser of claim 1 , wherein each of the set of optical dividing/combining elements is configured to divide an input pulse into two temporally spaced sub-pulses in a first direction from the first side to the second side and combine two input pulses into a single pulse in a second direction from the second side to the first side.
3. The pulsed laser of claim 1 , wherein the pulsed laser is a soliton laser that includes a dispersive delay module for providing anomalous dispersion.
4. The pulsed laser of claim 3 , wherein the dispersive delay module includes a grating pair.
5. The pulsed laser of claim 1 , wherein the second mirror is saturable absorber mirror (SAM).
6. The pulsed laser of claim 5 , wherein the second mirror is semiconductor saturable absorber mirror (SESAM).
7. The pulsed laser of claim 1 , wherein the optical amplifier includes a fiber gain medium.
8. The pulsed laser of claim 7 , wherein the fiber gain medium includes a ytterbium (Yb)-doped fiber.
9. The pulsed laser of claim 7 , wherein the optical cavity includes a Faraday rotator positioned between the first mirror and the fiber gain medium.
10. The pulsed laser of claim 9 , wherein the Faraday rotator and the first mirror together serve as a retro-reflector and are configured to cancel an effect due to a birefringence of the fiber gain medium.
11. The pulsed laser of claim 1 , wherein the optical dividing/combining elements include yttrium vanadate crystals.
12. The pulsed laser of claim 1 , wherein the set of optical dividing/combining elements are arranged as a set of successive dividing stages along the light path, and the input laser pulse is divided in each successive dividing stage.
13. The pulsed laser of claim 1 , wherein the optical amplifier is in a double-pass configuration to pass and amplify the sequence of sub-pulses once in each direction.
14. The pulsed laser of claim 1 , wherein the single amplified laser pulse at the first side of the set of optical dividing/combining elements is polarized substantially orthogonal to the polarization of the input laser.
15. The pulsed laser of claim 1 , wherein the number of pulses in the sequence of sub-pulses is N, and the number of elements in the set of optical dividing/combining elements is M, wherein N=2 M .
16. The pulsed laser of claim 1 , wherein the pulse energy of the single amplified laser pulse is 2 M × of the pulse energy of the input laser pulse.
17. A method for operating a pulsed laser by dividing laser pulses and recombining laser pulses within a laser cavity, comprising:
inside a laser cavity, directing a laser pulse of linearly polarized light to divide the laser pulse into a sequence of temporally spaced sub-pulses, wherein each sub-pulse has a lower pulse energy than an input laser pulse;
amplifying the sequence of sub-pulses in an optical amplifier in the laser cavity to produce a sequence of amplified sub-pulses; and
recombining, inside the laser cavity, the sequence of amplified sub-pulses into a single amplified laser pulse with a greater pulse energy than the input laser pulse; and
redirecting a portion of the single amplified laser pulse as the output pulse of the pulsed laser.
18. The method as in claim 17 , wherein the single amplified laser pulse is polarized orthogonally to the input laser pulse.
19. The method as in claim 17 , comprising using a set of optical dividing/combining elements inside the laser cavity to divide the laser pulse into the sequence of temporally spaced sub-pulses.
20. The method as in claim 17 , wherein the set of optical dividing/combining elements include yttrium vanadate crystals.
21. The method as in claim 17 , wherein the set of optical dividing/combining elements are arranged as a set of successive dividing stages along the light path, so that the input laser pulse is divided in each successive dividing stage.
22. The method as in claim 17 , wherein the optical amplifier includes a ytterbium-doped fiber configured in a double-pass configuration, and wherein amplifying the sequence of sub-pulses includes directing the sequence of sub-pulses to pass through the fiber once in each direction, thereby amplifying sequence of sub-pulses twice through the fiber.
23. A method for operating a pulsed laser by dividing laser pulses and recombining laser pulses within a laser cavity, comprising:
inside a laser cavity, directing a laser pulse of linearly polarized light to divide the laser pulse into a sequence of temporally spaced sub-pulses, wherein each sub-pulse has a lower pulse energy than an input laser pulse;
amplifying the sequence of sub-pulses in an optical amplifier in the laser cavity to produce a sequence of amplified sub-pulses; and
recombining, inside the laser cavity, the sequence of amplified sub-pulses into a single amplified laser pulse with a greater pulse energy than the input laser pulse; and
redirecting a portion of the single amplified laser pulse as the output pulse of the pulsed laser
wherein recombining the sequence of amplified sub-pulses includes directing the sequence of amplified sub-pulses into the same set of optical dividing/combining elements in the opposite direction to the dividing process.
24. The method as in claim 23 , wherein the single amplified laser pulse is polarized orthogonally to the input laser pulse.
25. The method as in claim 23 , wherein the set of optical dividing/combining elements are arranged as a set of successive dividing stages along the light path, so that the input laser pulse is divided in each successive dividing stage.
26. The method as in claim 23 , wherein the optical amplifier includes a ytterbium-doped fiber configured in a double-pass configuration, and wherein amplifying the sequence of sub-pulses includes directing the sequence of sub-pulses to pass through the fiber once in each direction, thereby amplifying sequence of sub-pulses twice through the fiber.
27. A pulsed laser, comprising:
a laser cavity including an optical amplifier and a plurality of optical dividing elements and configured to direct a laser pulse of linearly polarized light into the plurality of optical dividing elements to divide the light of the laser pulse into a sequence of divided pulses each having a pulse energy being a portion of the energy of the laser pulse before entry of the optical dividing elements, to subsequently direct the divided pulses into the optical amplifier to produce amplified divided pulses,
wherein the laser cavity is configured to direct the amplified divided pulses back into the plurality of optical dividing elements for a second time in an opposite direction to recombine the amplified divided pulses into a single laser pulse with a greater pulse energy as an output pulse of the laser cavity.
28. The pulsed laser as in claim 27 , wherein the laser cavity is a fiber laser cavity having a segment of gain fiber as the optical amplifier.
29. The pulsed laser as in claim 27 , wherein the laser cavity includes a dispersive delay module.
30. A pulsed laser that generates high energy pulses, comprising:
an optical ring cavity including an optical path to allow laser light to circulate inside the optical ring cavity;
a set of optical dividing elements and a set of optical recombining elements positioned along the optical path of the optical ring cavity; and
an optical amplifier positioned along the optical path of the optical ring cavity between the set of optical dividing elements and the set of optical recombining elements;
wherein the optical ring cavity is configured to:
direct a laser pulse into the set of optical dividing elements to divide the laser pulse into a sequence of temporally spaced sub-pulses, wherein each sub-pulse has a lower pulse energy than an input laser pulse;
direct the sequence of sub-pulses into the optical amplifier to produce a sequence of amplified sub-pulses;
direct the sequence of amplified sub-pulses into the set of optical recombining elements to recombine the sequence of amplified sub-pulses into a single amplified laser pulse having a greater pulse energy than the laser pulse; and
direct a portion of the single amplified laser pulse out of the optical ring cavity as an output pulse of the pulsed laser.
31. The pulse laser of claim 30 , wherein the optical ring cavity includes an optical coupler configured to couple the portion of the single amplified laser pulse as the output pulse of the pulse laser.
32. The pulse laser of claim 30 , wherein the laser pulse is linearly polarized.
33. A pulsed laser that generates high energy pulses, comprising:
a linear optical cavity including an optical path;
a set of optical dividing elements and a set of optical recombining elements positioned along the optical path of the linear optical cavity; and
an optical amplifier positioned along the optical path of the linear optical cavity between the set of optical dividing elements and the set of optical recombining elements;
wherein the linear optical cavity is configured to:
direct a laser pulse into the set of optical dividing elements to divide the laser pulse into a sequence of temporally spaced sub-pulses, wherein each sub-pulse has a lower pulse energy than an input laser pulse;
direct the sequence of sub-pulses into the optical amplifier to produce a sequence of amplified sub-pulses;
direct the sequence of amplified sub-pulses into the set of optical recombining elements to recombine the sequence of amplified sub-pulses into a single amplified laser pulse having a greater pulse energy than the laser pulse; and
direct a portion of the single amplified laser pulse out of the linear optical cavity as an output pulse of the pulsed laser.
34. The pulsed laser of claim 33 , wherein the laser pulse travels from the set of optical dividing elements to the set of optical recombining elements in the same direction.
35. The pulse laser of claim 33 , wherein the laser pulse is linearly polarized.