Fiber laser system, fiber laser system production method, and processing method

Patent metadata

Field	Value
Publication number	US-10522967-B2
Application number	US-201715450224-A
Country	US
Kind code	B2
Filing date	Mar 6, 2017
Priority date	Jan 26, 2016
Publication date	Dec 31, 2019
Grant date	Dec 31, 2019

Abstract

The present invention achieves a fiber laser having a high reflection resistance. A length of an optical fiber MMF is set so that a condition is satisfied at each point on an individual optical path of a fiber laser (FL 2 ), the condition being that a difference between time at which a power of a forward Stokes beam (SF) is at a maximum value and time at which a power of a backward Stokes beam (SB) is at a maximum value is greater than a sum of a half width at half maximum of the power of the forward Stokes beam (SF) and a half width at half maximum of the power of the backward Stokes beam (SB).

First claim

The invention claimed is:

1. A fiber laser system comprising:
a plurality of fiber lasers which generates respective laser beams;
a combiner which combines the laser beams together, so that a combined laser beam is obtained;
an output section; and
an optical fiber which (i) has an input end part and an output end part that are connected to the combiner and the output section, respectively and (ii) guides the combined laser beam from the combiner to the output section,
the fiber laser system having
(a) individual optical paths in which the respective laser beams generated by the plurality of fiber lasers are not yet combined together and
(b) a common optical path in which the respective laser beams generated by the plurality of fiber lasers have been combined together and which has an optical path length,

wherein the optical path length of the common optical path is set so that a first condition is satisfied at each point on any of the individual optical paths,
wherein the first condition is that a difference between a time at which a power of a forward Stokes beam is at a maximum value and a time at which a power of a backward Stokes beam is at a maximum value is greater than a sum of a half width at half maximum of the power of the forward Stokes beam and a half width at half maximum of the power of the backward Stokes beam with a reflector being in contact with an exit surface of the output section.

2. The fiber laser system as set forth in claim 1 , wherein
the optical path length of the common optical path is set so that a second condition is further satisfied at the each point on any of the individual optical paths,
the second condition being that, in the case where the reflector is in contact with the exit surface of the output section, a difference between the time at which the power of the forward Stokes beam is at a maximum value and time at which a power of a backward laser beam is at a maximum value is greater than a sum of the half width at half maximum of the power of the forward Stokes beam and a half width at half maximum of the power of the backward laser beam.

3. The fiber laser system as set forth in claim 1 , wherein
the optical path length of the common optical path is set so that a third condition is further satisfied at the each point on any of the individual optical paths,
the third condition being that, in the case where the reflector is in contact with the exit surface of the output section, a difference between time at which a power of a forward laser beam is at a maximum value and the time at which the power of the backward Stokes beam is at a maximum value is greater than a sum of a half width at half maximum of the power of the forward laser beam and the half width at half maximum of the power of the backward Stokes beam.

4. The fiber laser system as set forth in claim 1 , wherein
the optical path length of the common optical path is set so that a fourth condition is further satisfied at the each point on any of the individual optical paths,
the fourth condition being that, in the case where the reflector is in contact with the exit surface of the output section, a difference between the time at which the power of the forward laser beam is at a maximum value and the time at which the power of the backward laser beam is at a maximum value is greater than a sum of the half width at half maximum of the power of the forward laser beam and the half width at half maximum of the power of the backward laser beam.

5. A method of producing a fiber laser system,
the fiber laser system comprising:
a plurality of fiber lasers which generates respective laser beams;
a combiner which combines the laser beams together, so that a combined laser beam is obtained;
an output section; and
an optical fiber which (i) has an input end part and an output end part that are connected to the combiner and the output section, respectively and (ii) guides the combined laser beam from the combiner to the output section,
the fiber laser system having
(a) individual optical paths in which the respective laser beams generated by the plurality of fiber lasers are not yet combined together and
(b) a common optical path in which the respective laser beams generated by the plurality of fiber lasers have been combined together and Which has an optical path length,

the method comprising the step of:
setting the optical path length of the common optical path so that a first condition is satisfied at each point on any of the individual optical paths,
wherein the first condition is that, when a reflector is in contact with an exit surface of the output section, then a difference between a time at which a power of a forward Stokes beam is at a maximum value and a time at which a power of a backward Stokes beam is at a maximum value is greater than a sum of a half width at half maximum of the power of the forward Stokes beam and a half width at half maximum of the power of the backward Stokes beam.

6. A method of processing an object with use of a fiber laser system,
the fiber laser system comprising:
a plurality of fiber lasers which generates respective laser beams;
a combiner which combines the laser beams together, so that a combined laser beam is obtained;
an output section; and
an optical fiber which (i) has an input end part and an output end part that are connected to the combiner and the output section, respectively and (ii) guides the combined laser beam from the combiner to the output section,
the fiber laser system having
individual optical paths in which the respective laser beams generated by the plurality of fiber lasers are not yet combined together,

the method comprising the step of:
setting a distance from the output section to the object so that a first condition is satisfied at each point on any of the individual optical paths,
wherein the first condition is that a difference between a time at which a power of a forward Stokes beam is at a maximum value and a time at which a power of a backward Stokes beam is at a maximum value is greater than a sum of a half width at half maximum of the power of the forward Stokes beam and a half width at half maximum of the power of the backward Stokes beam.

Assignees

• Fujikura Ltd

Inventors

• Kashiwagi Masahiro

Classifications

• B23K26/707

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