Laser-beam combination with dual-substrate dichroic filters
A dual-substrate dichroic beam combiner includes two substrates, and a dichroic thin-film filter coated at a nominally planar interface between the substrates. The filter is configured to combine, into a combined laser beam, two input laser beams that are incident on the filter of the combiner from opposite respective sides thereof. One input beam is transmitted by the combiner, while the other input beam is reflected. The substrates are configured to, when heated by absorption of the input laser beams in the filter, form a lens for each of the input laser beams. The lens is either (a) a negative lens for each of the input laser beams or (b) a positive lens for each of the input laser beams. The combiner thereby reduces or eliminates focusing discrepancies between the two input beams, in the combined beam, as compared to a conventional single-substrate dichroic beam combiner.
1 . A system for generating a spectrally-combined laser beam, comprising:
a first laser configured to generate a first laser beam;
a second laser configured to generate the second laser beam, at least one of the first laser and the second laser is configured to generate the corresponding laser beam with an average power of at least 2.5 kilowatts; and
a dichroic beam combiner comprising
two substrates; and
a dichroic thin-film filter coated at a nominally planar interface between the substrates, the dichroic thin-film filter being transmissive in a transmission-wavelength-range and reflective in a reflection-wavelength-range, wherein the dichroic thin-film filter is configured to combine, into a combined laser beam, the first and second input laser beams that (a) have wavelengths in the transmission-wavelength-range and reflection-wavelength-range, respectively, and (b) are incident on the dichroic thin-film filter of the dichroic beam combiner from opposite respective sides thereof;
wherein the substrates are configured to, when heated by absorption of the first laser beam and the second laser beam in the dichroic thin-film filter, form a first lens for the first input laser beam and a second lens for the second input laser beam, the first and second lenses being either (a) both negative or (b) both positive.
2 . The system of claim 1 , wherein each of the first laser and the second laser is configured to generate the corresponding input laser beam with an average power of at least 2.5 kilowatts.
3 . The system of claim 1 , wherein the first and second lenses have the same optical power.
4 . The system of claim 3 , wherein each of the first and second lenses has positive optical power.
5 . The system of claim 1 , wherein the first and second lenses are at least partly caused by bulging of surfaces of the two substrates facing away from the planar interface.
6 . The system of claim 1 , wherein the two substrates are nominally planar in a dimension parallel to the planar interface.
7 . The dichroic beam combiner of claim 6 , wherein the two substrates are made of the same material and have the same nominal thickness orthogonally to the nominally planar interface.
8 . The system of claim 7 , wherein outlines of respective projections of the two substrates onto the nominally planar interface therebetween are identical in both shape and location at the same position.
9 . A system for combining three or more collimated laser beams, comprising:
a series of instances of a dichroic beam combiner comprising:
two substrates; and
a dichroic thin-film filter coated at a nominally planar interface between the substrates, the dichroic thin-film filter being transmissive in a transmission-wavelength-range and reflective in a reflection-wavelength-range, whereby the dichroic thin-film filter is configured to combine, into a combined laser beam, first and second input laser beams that (a) have wavelengths in the transmission-wavelength-range and reflection-wavelength-range, respectively, and (b) are incident on the dichroic thin-film filter of the dichroic beam combiner from opposite respective sides thereof;
wherein the substrates are configured to, when heated by absorption of the input laser beams in the dichroic thin-film filter, form a first lens for the first input laser beam and a second lens for the second input laser beam, the first and second lenses being either (a) both negative or (b) both positive; and
for each pair of dichroic beam combiners adjacent to each other in the series, a respective reflector arranged to (a) collimate the combined laser beam produced by a first dichroic beam combiner of the pair and (b) reflect the combined laser beam toward a second dichroic beam combiner of the pair, whereby the combined laser beam produced by the first dichroic beam combiner of the pair forms one of the first and second input laser beams for the second dichroic beam combiner of the pair.
10 . The system of claim 9 , wherein at least one of the reflectors includes:
a substrate having a front surface facing the combined laser beam incident on the reflector; and
a reflective coating disposed on the front surface, the reflective coating being partly absorptive to the combined laser beam incident thereon, whereby an optical power of the reflector, caused by thermal expansion of the substrate induced by absorption of the combined laser beam in the reflective coating, is passively adaptable to a power of the combined laser beam.
11 . The system of claim 9 , wherein at least one of the reflectors has actively adjustable optical power.
12 . The system of claim 9 , wherein for each dichroic beam combiner of the series, the first and second lenses are positive lenses having the same optical power, whereby the first and second lenses are configured to focus the first and second input laser beams by the same amount when the dichroic beam combiner is heated by absorption of the first and second input laser beams in the dichroic thin-film filter.
13 . The system of claim 12 , wherein, for each pair of dichroic beam combiners adjacent to each other in the series, a propagation distance of the combined laser beam from the first dichroic beam combiner of the pair to the reflector is less than a focal length of the positive lenses formed by the non-last dichroic beam combiner when heated by the absorption of the first and second input laser beams in the dichroic thin-film filter thereof.
14 . The system of claim 9 , wherein each non-first dichroic beam combiner of the series is configured to reflect the combined laser beam produced by the immediately preceding dichroic beam combiner of the series.
15 . A system for generating a spectrally-combined laser beam, comprising:
the system of claim 9 ;
two laser sources configured to generate the first and second input laser beams for the first dichroic beam combiner of the series; and
for each non-first dichroic beam combiner of the series, an additional laser source configured to generate the one of the corresponding first and second input laser beams that is not the combined laser beam produced by an immediately preceding dichroic beam combiner of the series.
16 . The system of claim 15 , wherein the combined laser beam produced by a last dichroic beam combiner of the series has an average power of more than 15 kilowatts.
17 . The system of claim 15 , wherein each of the laser sources is configured to generate the corresponding laser beam with a power of at least 2.5 kilowatts.
18 . The system of claim 9 , wherein in each beam combiner the first and second lenses have the same optical power.
19 . The system of claim 9 , wherein in each beam combiner the two substrates are nominally planar.
20 . The system of claim 19 , wherein the two substrates are made of the same material and have the same nominal thickness orthogonally to the nominally planar interface.