WO2019026912A1 - Light source device and laser light irradiation device - Google Patents
Light source device and laser light irradiation device Download PDFInfo
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- WO2019026912A1 WO2019026912A1 PCT/JP2018/028683 JP2018028683W WO2019026912A1 WO 2019026912 A1 WO2019026912 A1 WO 2019026912A1 JP 2018028683 W JP2018028683 W JP 2018028683W WO 2019026912 A1 WO2019026912 A1 WO 2019026912A1
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
- H01S3/00—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
- H01S3/05—Construction or shape of optical resonators; Accommodation of active medium therein; Shape of active medium
- H01S3/06—Construction or shape of active medium
- H01S3/063—Waveguide lasers, i.e. whereby the dimensions of the waveguide are of the order of the light wavelength
- H01S3/067—Fibre lasers
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
- H01S3/00—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
- H01S3/10—Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating
Definitions
- One aspect of the present invention relates to a light source device and a laser beam irradiation device provided with the light source device.
- a linearly polarized light source described in Patent Document 1 includes a light source having a reflecting mirror, a polarization beam splitter that splits a light flux from the light source into two light fluxes whose polarization directions are orthogonal to each other, and between the light source and the polarization beam splitter And a luminous flux reflecting element for reflecting any one of the two luminous fluxes to make the light incident on a reflecting mirror of a light source.
- the linearly polarized light source described in Patent Document 1 is intended to efficiently generate linearly polarized light.
- a fiber laser that emits laser light of randomly polarized light may be used from the viewpoint of low price, high output, and high distribution.
- the fiber laser there are the following problems caused by the fiber laser. That is, in the laser light of random polarization, the polarization direction is not constant but changes. Therefore, when laser light is branched for each polarization component using a polarization beam splitter to obtain linearly polarized laser light, the ratio of each laser light after branching is not constant but fluctuates. As a result, the laser output of the linearly polarized laser light obtained may also fluctuate (become unstable).
- An object of one aspect of the present invention is to stably obtain linearly polarized laser light in a light source device and a laser light irradiation device using a fiber laser that emits randomly polarized laser light.
- a light source device branches a fiber laser that emits laser light of random polarization, and a laser light emitted by the fiber laser into a first branch laser light and a second branch laser light for each polarization component.
- a half mirror that multiplexes the second branched laser beam whose polarization direction has been changed and outputs it as a multiplexed laser beam.
- laser light of random polarization emitted from the fiber laser is branched for each polarization component by the polarization beam splitter.
- the polarization direction of the second branch laser beam is changed by the wave plate so as to be the same as the polarization direction of the first branch laser beam.
- the first and second split laser beams having the same polarization direction are multiplexed and output by the half mirror. Therefore, even when using a fiber laser that emits laser light of randomly polarized light, it is possible to stably obtain linearly polarized laser light regardless of the polarization characteristics of the fiber laser.
- the fiber laser has a main body that amplifies seed light, and a laser head that is connected to the main body via a light guide fiber and emits laser light.
- the fiber laser constitutes a so-called head separation type fiber laser.
- the polarization of the laser light emitted from the fiber laser is likely to be affected by the bending of the light guide fiber or the like. Therefore, the above-mentioned effect of stably obtaining linearly polarized laser light regardless of the polarization characteristics of the fiber laser used is particularly effective.
- the optical path difference between the optical path of the first branched laser beam and the optical path of the second branched laser beam may be longer than the coherence length of the fiber laser. According to this configuration, it is possible to suppress interference of the first and second branched laser beams combined by the half mirror.
- the combined laser beam includes the first combined laser beam coaxial with the first branched laser beam and the second combined laser beam coaxial with the second branched laser beam. It may be. According to this configuration, two linearly polarized laser beams can be obtained, which facilitates application to various specifications and the like.
- a laser beam irradiation apparatus is a laser beam irradiation apparatus including the above light source device, wherein a first polarization element to which a first combined laser beam is incident and a second combined laser beam are An optical system having a second polarizing element to be incident is provided.
- this laser beam irradiation apparatus includes the above-described light source device, the above-described effect of stably obtaining linearly polarized laser light when using a fiber laser that emits randomly polarized laser light is exhibited. Moreover, in this laser beam irradiation apparatus, it becomes possible to perform laser beam irradiation using both of the two linearly polarized laser beams obtained by multiplexing by the half mirror.
- the laser beam irradiation apparatus is a laser beam irradiation apparatus including the above light source device, and is a polarizing element to which any one of the first combined laser beam and the second combined laser beam is incident. And an optical system having a beam damper for blocking either the first combined laser beam or the second combined laser beam.
- this laser beam irradiation apparatus includes the above-described light source device, the above-described effect of stably obtaining linearly polarized laser light when using a fiber laser that emits randomly polarized laser light is exhibited. Moreover, in this laser beam irradiation apparatus, it becomes possible to perform laser beam irradiation using only one of two linearly polarized laser beams obtained by multiplexing by the half mirror.
- the present invention it is possible to stably obtain linearly polarized laser light in a light source device and a laser light irradiation device using a fiber laser that emits randomly polarized laser light.
- FIG. 1 is a schematic configuration view showing a laser beam irradiation apparatus according to the first embodiment.
- FIG. 2 is a graph for explaining the laser light emitted from the fiber laser of FIG.
- FIG. 3 is a graph for explaining the combined laser light output from the light source device of FIG.
- FIG. 4 is a schematic configuration view showing a laser beam irradiation apparatus according to the second embodiment.
- FIG. 1 is a schematic configuration view showing a laser beam irradiation apparatus 100 according to the first embodiment.
- the laser beam irradiation apparatus 100 is an apparatus for irradiating the laser light L of linearly polarized light to the object T, and includes the light source device 1 and the optical system 30.
- Linear polarization means a polarization state in which the vibration direction of the electric field (and the magnetic field) is constant.
- the light source device 1 includes a fiber laser 10 and a polarization adjustment unit 20.
- the fiber laser 10 emits laser light L0 of randomly polarized light. Random polarization means linearly polarized light, but a polarization state in which the polarization direction is not constant but changes with time.
- the fiber laser 10 has a main body 11 for amplifying seed light, and a laser head 13 connected to the main body 11 via a light guide fiber 12.
- the fiber laser 10 is a solid-state laser using an optical fiber as an amplification medium.
- the fiber laser 10 here is a so-called head separation type fiber laser.
- the main body 11 includes a laser diode 14 that oscillates seed light, and an amplification unit 15 that amplifies and outputs the seed light.
- the laser head unit 13 emits laser light L0 of random polarization.
- the polarization adjustment unit 20 includes a polarization beam splitter 21, a mirror 22, a half wave plate (wave plate) 23, a mirror 24, and a half mirror 25.
- the polarization beam splitter 21 splits the laser beam L0 emitted by the fiber laser 10 into a first split laser beam L1 and a second split laser beam L2 for each polarization component.
- the polarization beam splitter 21 divides the optical path P0 of the laser beam L0 into a first optical path P1 which is an optical path of the first branched laser light L1 and a second optical path P2 which is an optical path of the second branched laser light L2. Branch.
- the polarization directions of the first branched laser light L1 and the second branched laser light L2 are orthogonal to each other.
- the first branched laser beam L1 is a P-polarized laser beam, and has, for example, the vertical direction in the drawing as the polarization direction.
- the second branched laser beam L2 is an S-polarized laser beam, and has, for example, a direction perpendicular to the paper surface as a polarization direction.
- P-polarization is linear polarization in which an electric field vibrates in the incident plane.
- the s-polarized light is linearly polarized light in which the electric field oscillates perpendicularly to the incident plane.
- the mirror 22 is disposed in the second optical path P2.
- the mirror 22 reflects the second branched laser light L2 toward the half-wave plate 23.
- the half-wave plate 23 is disposed downstream of the mirror 22 in the second optical path P2.
- the half-wave plate 23 rotates the polarization component of the second branched laser beam L2 to change the polarization direction of the second branched laser beam L2 to be the same as the polarization direction of the first branched laser beam L1.
- the mirror 24 is disposed downstream of the half wave plate 23 in the second optical path P2.
- the mirror 24 reflects the second branched laser beam L2 toward the half mirror 25.
- the half mirror 25 is disposed at the junction of the downstream side of the first optical path P1 and the downstream side of the second optical path P2.
- the half mirror 25 combines the first split laser beam L1 split by the polarization beam splitter 21 and the second split laser beam L2 whose polarization direction is changed by the half wave plate 23, and combines the combined laser beam L3.
- Output as The half mirror 25 is a cube-shaped non-polarization half mirror.
- the half mirror 25 has a transmittance of 50% and a reflectance of 50%.
- the combined laser beam L3 is a linearly polarized laser beam, and here. P-polarized laser light.
- the combined laser beam L3 includes a first combined laser beam L31 coaxial with the first branched laser beam L1, and a second combined laser beam L32 coaxial with the second branched laser beam L2.
- the first combined laser beam L31 is a laser beam formed by combining a part of the first branched laser beam L1 transmitted through the half mirror 25 and a part of the second branched laser beam L2 reflected by the half mirror 25. is there.
- the second combined laser beam L32 is a laser beam formed by combining a part of the first branched laser beam L1 reflected by the half mirror 25 and a part of the second branched laser beam L2 transmitted through the half mirror 25. is there.
- the second optical path P2 includes a third optical path P21 from the polarization beam splitter 21 to the mirror 22, a fourth optical path P22 from the mirror 24 to the half mirror 25, and a fifth optical path P23 from the mirror 22 to the mirror 24.
- the fifth optical path P23 has the same optical path length as the first optical path P1.
- the optical path difference between the first optical path P1 and the second optical path P2 (that is, the optical path lengths of the third optical path P21 and the fourth optical path P22) is longer than the coherence length of the fiber laser 10.
- the coherence length is the upper limit of the distance in which the light interference phenomenon appears when the first branched laser light L1 and the second branched laser light L2 are combined.
- the optical system 30 includes a spatial light modulator (first polarizing element) 31 and 4 f optical system 32, a condensing lens 33, a spatial light modulator (second polarizing element) 35 and 4 f optical system 36, and a condensing lens 37.
- the spatial light modulators 31 and 35 are, for example, spatial light modulators (SLM: Spatial Light Modulator) of a reflective liquid crystal (LCOS: Liquid Crystal on Silicon).
- SLM Spatial Light Modulator
- LCOS Liquid Crystal on Silicon
- the spatial light modulator 31 is a polarizing element on which the first combined laser beam L31 is incident.
- the spatial light modulator 31 modulates and reflects the incident first combined laser beam L31.
- the spatial light modulator 35 is a polarizing element on which the second combined laser beam L32 is incident.
- the spatial light modulator 35 modulates and reflects the incident second combined laser beam L32.
- the spatial light modulators 31 and 35 have a display unit capable of displaying a modulation pattern.
- the spatial light modulator 31 adjusts the wavefront of the first combined laser beam L31 according to the modulation pattern by causing the first combined laser beam L31 to be incident on the modulation pattern.
- the spatial light modulator 35 adjusts the wavefront of the second combined laser beam L32 according to the modulation pattern by causing the second combined laser beam L32 to be incident on the modulation pattern.
- modulation of each of the first and second combined laser beams L31 and L32 for example, intensity, amplitude, phase, polarization, etc.
- the 4f optical system 32 is an adjustment optical system that adjusts the wavefront shape (wavefront adjustment) of the first combined laser light L31 modulated by the spatial light modulator 31.
- the 4f optical system 32 is disposed on the optical path between the spatial light modulator 31 and the condensing lens 33.
- the 4f optical system 36 is an adjustment optical system that adjusts the wavefront shape of the second combined laser light L32 modulated by the spatial light modulator 35.
- the 4f optical system 36 is disposed on the optical path between the spatial light modulator 35 and the condenser lens 37.
- the condensing lens 33 condenses the first combined laser beam L31 on the object T.
- the condensing lens 37 condenses the second combined laser beam L32 on the object T.
- Each of the condenser lenses 33 and 37 may be configured to include a plurality of lenses.
- the laser beam L0 of random polarization emitted from the fiber laser 10 in the light source device 1 is branched by the polarization beam splitter 21 for each polarization component.
- the half-wave plate 23 rotates the polarization component of the second split laser beam L2 so that the polarization direction of the second split laser beam L2 becomes the same (parallel) as the polarization direction of the first split laser beam L1. be changed.
- the first and second branched laser beams L1 and L2 having the same polarization direction are multiplexed by the half mirror 25, and finally output as a multiplexed laser beam L3 aligned with a single linearly polarized light. Ru.
- the first combined laser beam L31 in the combined laser beam L3 is incident on the spatial light modulator 31 in the optical system 30, and is modulated according to the modulation pattern displayed on the display unit of the spatial light modulator 31. Thereafter, the wavefront is adjusted by the 4f optical system 32.
- the first combined laser beam L31 whose wavefront is adjusted by the 4f optical system 32 is condensed by the condenser lens 33 and is irradiated as the laser beam L on the object T.
- the second combined laser beam L32 of the combined laser beam L3 is incident on the spatial light modulator 35, and is modulated according to the modulation pattern displayed on the display unit of the spatial light modulator 35.
- the wavefront is adjusted by the 4f optical system 36.
- the second combined laser beam L32 whose wavefront is adjusted by the 4f optical system 36 is condensed by the condenser lens 37 and is emitted as the laser beam L to the object T.
- FIG. 2 is a graph for explaining the laser beam L0 emitted from the fiber laser 10.
- the vertical axis is the normalized laser output obtained by dividing the laser output by the reference output value.
- the horizontal axis is time (hour).
- the data label value of “P polarization” indicates the normalized laser output of the polarization component of P polarization formed by separating the laser light L 0 emitted by the fiber laser 10 with a polarizer or the like.
- the data label value of “S polarization” indicates the normalized laser output of the polarization component of S polarization formed by separating the laser light L 0 emitted by the fiber laser 10 with a polarizer or the like.
- the “total” data label value indicates the sum of the polarization component of the P polarization and the polarization component of the S polarization.
- the total laser output is stable after a predetermined time, while the P-polarized and S-polarized laser outputs have larger fluctuations than the total.
- the laser light L0 emitted from the fiber laser 10 has randomly polarized light, and the ratio of the p-polarized light component to the s-polarized light component fluctuates.
- the laser output of P-polarization and S-polarization is affected by the polarization characteristic of the fiber laser 10 and becomes unstable.
- the fiber laser 10 when a fiber such as the light guide fiber 12 is bent or crushed, the polarization of the emitted laser light L0 may be affected. While moving the light guiding fiber 12, the polarization may fluctuate while moving.
- the randomly polarized laser beam L0 emitted from the fiber laser 10 is split into the first and second split laser beams L1 and L2.
- the polarization direction of the second split laser beam L2 is changed by the half-wave plate 23 to be the same as the polarization direction of the first split laser beam L1, and the first and second split laser beams L1 and L2 are half mirrors
- the light is combined at 25 and output as combined laser light L3. Therefore, even when using the fiber laser 10 for emitting the laser light L0 of random polarization, the laser light L (multiplexing laser light L3) of linear polarization can be stably obtained regardless of the polarization characteristic of the fiber laser 10 It becomes possible. It is possible to obtain a high-power light source device 1 that is cheaper than the existing light source device.
- FIG. 3 is a graph for explaining the combined laser light L3 output from the light source device 1.
- the vertical axis is the normalized laser output obtained by dividing the laser output by the reference output value.
- the horizontal axis is time (min).
- the data label value of “original output” indicates the normalized laser output of the laser light L0 of random polarization emitted by the fiber laser 10.
- the data label value of the “first branched laser beam” indicates the normalized laser output of the first branched laser beam L1 which is obtained by just branching the randomly polarized laser beam L0 by the polarization beam splitter 21.
- the data label value of the “first branched laser light” here is the polarization adjustment (that is, the second branched laser light whose polarization direction is changed by the first branched laser light L1 and the half wavelength plate 23 by the half mirror 25). It is a normalized laser output of the 1st branch laser beam L1 of P polarization in front of combining with L2.
- the data label value of “combined laser light” indicates the normalized laser output of the combined laser light L3.
- the data label value of “multiplexed laser light” here is a normalized laser output of the first multiplexed laser light L31 of P-polarization after the polarization adjustment. According to the results shown in FIG. 3, it can be confirmed that the laser output of the combined laser light L3 after the polarization adjustment has an output fluctuation equal to that of the stable laser output of the original output.
- the fiber laser 10 constitutes a so-called head separation type fiber laser having a main body portion 11 and a laser head portion 13.
- the polarization of the laser beam L0 emitted from the fiber laser 10 is likely to be affected by the bending or the like of the light guide fiber 12. Therefore, the above-mentioned effect of stably obtaining linearly polarized laser light L regardless of the polarization characteristic of the fiber laser 10 used is particularly effective.
- the optical path difference between the first optical path P1 of the first branched laser light L1 and the second optical path P2 of the second branched laser light L2 is longer than the coherence length of the fiber laser 10. According to this configuration, it is possible to suppress interference of the first and second split laser beams L1 and L2 combined by the half mirror 25.
- the combined laser light L3 having the same beam profile as the laser light L0 emitted from the fiber laser 10 can be output.
- the combined laser beam L3 includes a first combined laser beam L31 coaxial with the first split laser beam L1, and a second combined laser beam L32 coaxial with the second split laser beam L2. According to this configuration, since the two linearly polarized first and second combined laser beams L31 and L32 can be obtained, application to various specifications and the like can be facilitated.
- the laser beam irradiation apparatus 100 when the fiber laser 10 emitting the laser beam L0 of random polarization is used by the light source device 1, the above-described effect of stably obtaining the linearly polarized laser beam L is exerted. Further, in the laser beam irradiation apparatus 100, laser beam irradiation can be performed using both of the two first and second combined laser beams L31 and L32 obtained by multiplexing by the half mirror 25. It is possible to obtain a laser beam irradiation apparatus 100 having a specification having two ports of laser output (using two beams).
- FIG. 4 is a schematic configuration view showing a laser beam irradiation apparatus 200 according to the second embodiment.
- the laser beam irradiation apparatus 200 differs from the first embodiment in that an optical system 40 is provided instead of the optical system 30 (see FIG. 1).
- the optical system 40 includes a spatial light modulator (polarization element) 31, a 4 f optical system 32, a condenser lens 33, and a beam damper 44.
- the beam damper 44 blocks the second combined laser beam L32.
- the first combined laser beam L31 of the combined laser beam L3 is incident on the spatial light modulator 31 in the optical system 30, and displayed on the display unit of the spatial light modulator 31. After being modulated according to the modulation pattern, the wavefront is adjusted by the 4f optical system 32.
- the first combined laser beam L31 whose wavefront is adjusted by the 4f optical system 32 is condensed by the condenser lens 33 and is irradiated as the laser beam L on the object T.
- the second combined laser beam L32 of the combined laser beam L3 is blocked by the beam damper 44 and terminated.
- the laser beam irradiation apparatus 200 when the fiber laser 10 emitting the randomly polarized laser beam L0 is used by the light source device 1, the above-described effect of stably obtaining the linearly polarized laser beam L is exhibited. Further, in the laser beam irradiation apparatus 200, laser beam irradiation can be performed using only one of the two first and second combined laser beams L31 and L32 obtained by multiplexing by the half mirror 25. It is possible to obtain a laser light irradiation apparatus 200 having a specification having one port of laser output (using one beam).
- the said embodiment is equipped with the spatial light modulators 31 and 35 as a polarizing element
- the polarizing element applied to the laser beam irradiation apparatuses 100 and 200 is not specifically limited, It replaces with the spatial light modulators 31 and 35.
- other polarization elements may be provided.
- the first combined laser beam L31 is made incident on the spatial light modulator 31, and the second combined laser beam L32 is made incident on the beam damper 44.
- the second combined laser beam L32 is made second
- the wave laser light L32 may be made incident on the spatial light modulator 31, and the first combined laser light L31 may be made incident on the beam damper 44.
- the first combined laser beam L31 is shielded and terminated by the beam damper 44, while the second combined laser beam L32 is modulated according to the modulation pattern displayed on the display unit of the spatial light modulator 31.
- the wavefront is adjusted by the 4f optical system 32, and the light is condensed by the condensing lens 33 and irradiated as the laser light L on the object T.
- SYMBOLS 1 Light source device, 10 ... Fiber laser, 11 ... Main-body part, 12 ... Light guide fiber, 13 ... Laser head part, 21 ... Polarization beam splitter, 23 ... 1/2 wavelength plate (wave plate), 25 ... Half mirror, Reference Signs List 30 optical system 31 spatial light modulator (polarization element, first polarization element) 35 spatial light modulator (second polarization element) 40 optical system 44 beam damper 100, 200 laser light Irradiation device, P1 ... first light path (light path of first branched laser light), P2 ... second light path (light path of second branched laser light).
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Abstract
Description
本発明の一側面は、光源装置及びそれを具備するレーザ光照射装置に関する。 One aspect of the present invention relates to a light source device and a laser beam irradiation device provided with the light source device.
従来、光源装置に関する技術として、例えば特許文献1に記載された直線偏光光源が知られている。特許文献1に記載された直線偏光光源は、反射鏡を有する光源と、光源からの光束を偏光方向が互いに直交する2つの光束に分離する偏光ビームスプリッタと、光源と偏光ビームスプリッタとの間に配置された1/4波長板と、2つの光束の何れか一方を反射して光源の反射鏡に入射させる光束反射素子と、を備える。特許文献1に記載された直線偏光光源では、効率よく直線偏光光を発生することが図られている。
Conventionally, as a technique related to a light source device, for example, a linearly polarized light source described in
上述したような光源装置では、例えば価格の安さ、出力の高さ、及び流通の多さ等から、ランダム偏光のレーザ光を出射するファイバレーザを用いる場合がある。この場合、当該ファイバレーザに起因する次の課題が存在する。すなわち、ランダム偏光のレーザ光では、偏光方向が一定ではなく変化する。よって、直線偏光のレーザ光を得るべく、偏光ビームスプリッタを用いて偏光成分ごとにレーザ光を分岐すると、分岐後の各レーザ光の比率が一定ではなく変動する。その結果、得られた直線偏光のレーザ光のレーザ出力についても、変動する(不安定になる)おそれがある。 In the light source device as described above, for example, a fiber laser that emits laser light of randomly polarized light may be used from the viewpoint of low price, high output, and high distribution. In this case, there are the following problems caused by the fiber laser. That is, in the laser light of random polarization, the polarization direction is not constant but changes. Therefore, when laser light is branched for each polarization component using a polarization beam splitter to obtain linearly polarized laser light, the ratio of each laser light after branching is not constant but fluctuates. As a result, the laser output of the linearly polarized laser light obtained may also fluctuate (become unstable).
本発明の一側面は、ランダム偏光のレーザ光を出射するファイバレーザを用いた光源装置及びレーザ光照射装置において、安定して直線偏光のレーザ光を得ることを課題とする。 An object of one aspect of the present invention is to stably obtain linearly polarized laser light in a light source device and a laser light irradiation device using a fiber laser that emits randomly polarized laser light.
本発明の一側面に係る光源装置は、ランダム偏光のレーザ光を出射するファイバレーザと、ファイバレーザで出射したレーザ光を、偏光成分ごとに第1分岐レーザ光と第2分岐レーザ光とへ分岐する偏光ビームスプリッタと、第2分岐レーザ光の偏光方向を第1分岐レーザ光の偏光方向と同じになるように変える波長板と、偏光ビームスプリッタで分岐された第1分岐レーザ光と波長板で偏光方向を変えた第2分岐レーザ光とを、合波して合波レーザ光として出力するハーフミラーと、を備える。 A light source device according to one aspect of the present invention branches a fiber laser that emits laser light of random polarization, and a laser light emitted by the fiber laser into a first branch laser light and a second branch laser light for each polarization component. Polarization beam splitter, a wavelength plate for changing the polarization direction of the second branch laser beam to be the same as the polarization direction of the first branch laser beam, and a first branch laser beam and a wavelength plate branched by the polarization beam splitter And a half mirror that multiplexes the second branched laser beam whose polarization direction has been changed and outputs it as a multiplexed laser beam.
この光源装置では、ファイバレーザから出射されたランダム偏光のレーザ光は、偏光ビームスプリッタで偏光成分ごとに分岐される。第2分岐レーザ光の偏光方向が、第1分岐レーザ光の偏光方向と同じになるように波長板により変えられる。そして、ハーフミラーによって、互いに同じ偏光方向となった第1及び第2分岐レーザ光が合波されて出力される。したがって、ランダム偏光のレーザ光を出射するファイバレーザを用いた場合でも、当該ファイバレーザの偏光特性によらずに、安定して直線偏光のレーザ光を得ることが可能となる。 In this light source device, laser light of random polarization emitted from the fiber laser is branched for each polarization component by the polarization beam splitter. The polarization direction of the second branch laser beam is changed by the wave plate so as to be the same as the polarization direction of the first branch laser beam. Then, the first and second split laser beams having the same polarization direction are multiplexed and output by the half mirror. Therefore, even when using a fiber laser that emits laser light of randomly polarized light, it is possible to stably obtain linearly polarized laser light regardless of the polarization characteristics of the fiber laser.
本発明の一側面に係る光源装置では、ファイバレーザは、種光を増幅する本体部と、本体部に導光ファイバを介して接続され、レーザ光を出射するレーザヘッド部と、を有していてもよい。この構成では、ファイバレーザは、いわゆるヘッド分離型のファイバレーザを構成する。この場合、導光ファイバの曲げ等により、ファイバレーザから出射するレーザ光の偏光に影響が出やすい。よって、用いたファイバレーザの偏光特性によらずに安定して直線偏光のレーザ光を得るという上記効果は、特に有効である。 In the light source device according to one aspect of the present invention, the fiber laser has a main body that amplifies seed light, and a laser head that is connected to the main body via a light guide fiber and emits laser light. May be In this configuration, the fiber laser constitutes a so-called head separation type fiber laser. In this case, the polarization of the laser light emitted from the fiber laser is likely to be affected by the bending of the light guide fiber or the like. Therefore, the above-mentioned effect of stably obtaining linearly polarized laser light regardless of the polarization characteristics of the fiber laser used is particularly effective.
本発明の一側面に係る光源装置では、第1分岐レーザ光の光路と第2分岐レーザ光の光路との光路差が、ファイバレーザの可干渉距離よりも長くてもよい。この構成によれば、ハーフミラーによって合波する第1及び第2分岐レーザ光が干渉するのを抑制することが可能となる。 In the light source device according to one aspect of the present invention, the optical path difference between the optical path of the first branched laser beam and the optical path of the second branched laser beam may be longer than the coherence length of the fiber laser. According to this configuration, it is possible to suppress interference of the first and second branched laser beams combined by the half mirror.
本発明の一側面に係る光源装置では、合波レーザ光は、第1分岐レーザ光と同軸の第1合波レーザ光、及び、第2分岐レーザ光と同軸の第2合波レーザ光を含んでいてもよい。この構成によれば、2つの直線偏光のレーザ光が得られることから、種々の仕様等に適用させ易くなる。 In the light source device according to one aspect of the present invention, the combined laser beam includes the first combined laser beam coaxial with the first branched laser beam and the second combined laser beam coaxial with the second branched laser beam. It may be. According to this configuration, two linearly polarized laser beams can be obtained, which facilitates application to various specifications and the like.
本発明の一側面に係るレーザ光照射装置は、上記光源装置を具備するレーザ光照射装置であって、第1合波レーザ光が入射される第1偏光素子、及び第2合波レーザ光が入射される第2偏光素子を有する光学系を備える。 A laser beam irradiation apparatus according to one aspect of the present invention is a laser beam irradiation apparatus including the above light source device, wherein a first polarization element to which a first combined laser beam is incident and a second combined laser beam are An optical system having a second polarizing element to be incident is provided.
このレーザ光照射装置は、上記光源装置を具備することから、ランダム偏光のレーザ光を出射するファイバレーザを用いた場合に安定して直線偏光のレーザ光を得るという上記効果を奏する。また、このレーザ光照射装置では、ハーフミラーによって合波されることで得られた2つの直線偏光のレーザ光の双方を利用したレーザ光照射が可能となる。 Since this laser beam irradiation apparatus includes the above-described light source device, the above-described effect of stably obtaining linearly polarized laser light when using a fiber laser that emits randomly polarized laser light is exhibited. Moreover, in this laser beam irradiation apparatus, it becomes possible to perform laser beam irradiation using both of the two linearly polarized laser beams obtained by multiplexing by the half mirror.
本発明の一側面に係るレーザ光照射装置は、上記光源装置を具備するレーザ光照射装置であって、第1合波レーザ光及び第2合波レーザ光の何れか一方が入射される偏光素子、及び、第1合波レーザ光及び第2合波レーザ光の何れか他方を遮蔽するビームダンパーを有する光学系を備える。 The laser beam irradiation apparatus according to one aspect of the present invention is a laser beam irradiation apparatus including the above light source device, and is a polarizing element to which any one of the first combined laser beam and the second combined laser beam is incident. And an optical system having a beam damper for blocking either the first combined laser beam or the second combined laser beam.
このレーザ光照射装置は、上記光源装置を具備することから、ランダム偏光のレーザ光を出射するファイバレーザを用いた場合に安定して直線偏光のレーザ光を得るという上記効果を奏する。また、このレーザ光照射装置では、ハーフミラーによって合波されることで得られた2つの直線偏光のレーザ光の何れか一方のみを利用したレーザ光照射が可能となる。 Since this laser beam irradiation apparatus includes the above-described light source device, the above-described effect of stably obtaining linearly polarized laser light when using a fiber laser that emits randomly polarized laser light is exhibited. Moreover, in this laser beam irradiation apparatus, it becomes possible to perform laser beam irradiation using only one of two linearly polarized laser beams obtained by multiplexing by the half mirror.
本発明の一側面によれば、ランダム偏光のレーザ光を出射するファイバレーザを用いた光源装置及びレーザ光照射装置において、安定して直線偏光のレーザ光を得ることが可能となる。 According to one aspect of the present invention, it is possible to stably obtain linearly polarized laser light in a light source device and a laser light irradiation device using a fiber laser that emits randomly polarized laser light.
以下、実施形態について、図面を参照して詳細に説明する。なお、各図において同一又は相当部分には同一符号を付し、重複する説明を省略する。 Hereinafter, embodiments will be described in detail with reference to the drawings. In the drawings, the same or corresponding parts are denoted by the same reference numerals and redundant description will be omitted.
[第1実施形態]
図1は、第1実施形態に係るレーザ光照射装置100を示す概略構成図である。レーザ光照射装置100は、対象物Tに直線偏光のレーザ光Lを照射する装置であって、光源装置1及び光学系30を備える。直線偏光とは、電場(及び磁場)の振動方向が一定である偏光状態を意味する。
First Embodiment
FIG. 1 is a schematic configuration view showing a laser
光源装置1は、ファイバレーザ10と、偏光調整ユニット20と、を備える。ファイバレーザ10は、ランダム偏光のレーザ光L0を出射する。ランダム偏光とは、直線偏光ではあるが、偏光方向が一定ではなく時間と共に変化する偏光状態を意味する。ファイバレーザ10は、種光を増幅する本体部11と、本体部11に導光ファイバ12を介して接続されたレーザヘッド部13と、を有する。ファイバレーザ10は、増幅媒質に光ファイバを使った固体レーザである。ここでのファイバレーザ10は、いわゆるヘッド分離型のファイバレーザである。本体部11は、種光を発振するレーザダイオード14と、種光を増幅して出力する増幅部15と、含む。レーザヘッド部13は、ランダム偏光のレーザ光L0を出射する。
The
偏光調整ユニット20は、偏光ビームスプリッタ21と、ミラー22と、1/2波長板(波長板)23と、ミラー24と、ハーフミラー25と、を有する。偏光ビームスプリッタ21は、ファイバレーザ10で出射したレーザ光L0を、偏光成分ごとに第1分岐レーザ光L1と第2分岐レーザ光L2とへ分岐する。換言すると、偏光ビームスプリッタ21は、レーザ光L0の光路P0を、第1分岐レーザ光L1の光路である第1光路P1と、第2分岐レーザ光L2の光路である第2光路P2と、に分岐する。
The
第1分岐レーザ光L1と第2分岐レーザ光L2とは、偏光方向が互いに直交する。第1分岐レーザ光L1は、P偏光のレーザ光であり、例えば紙面上下方向を偏光方向として有する。第2分岐レーザ光L2は、S偏光のレーザ光であり、例えば紙面垂直方向を偏光方向として有する。P偏光とは、入射面内で電界が振動する直線偏光である。S偏光とは、S偏光は、入射面に垂直に電界が振動する直線偏光である。 The polarization directions of the first branched laser light L1 and the second branched laser light L2 are orthogonal to each other. The first branched laser beam L1 is a P-polarized laser beam, and has, for example, the vertical direction in the drawing as the polarization direction. The second branched laser beam L2 is an S-polarized laser beam, and has, for example, a direction perpendicular to the paper surface as a polarization direction. P-polarization is linear polarization in which an electric field vibrates in the incident plane. The s-polarized light is linearly polarized light in which the electric field oscillates perpendicularly to the incident plane.
ミラー22は、第2光路P2に配置されている。ミラー22は、第2分岐レーザ光L2を1/2波長板23へ向かって反射する。1/2波長板23は、第2光路P2においてミラー22の下流側に配置されている。1/2波長板23は、第2分岐レーザ光L2の偏光成分を回転させ、第2分岐レーザ光L2の偏光方向を、第1分岐レーザ光L1の偏光方向と同じになるように変える。
The
ミラー24は、第2光路P2において1/2波長板23の下流側に配置されている。ミラー24は、第2分岐レーザ光L2をハーフミラー25へ向かって反射する。ハーフミラー25は、第1光路P1の下流側と第2光路P2の下流側との合流部分に配置されている。ハーフミラー25は、偏光ビームスプリッタ21で分岐された第1分岐レーザ光L1と1/2波長板23で偏光方向を変えた第2分岐レーザ光L2とを、合波して合波レーザ光L3として出力する。ハーフミラー25は、キューブ型の無偏光ハーフミラーである。ハーフミラー25は、50%の透過率及び50%の反射率を有する。
The
合波レーザ光L3は、直線偏光のレーザ光であり、ここでは。P偏光のレーザ光である。合波レーザ光L3は、第1分岐レーザ光L1と同軸の第1合波レーザ光L31、及び、第2分岐レーザ光L2と同軸の第2合波レーザ光L32を含む。第1合波レーザ光L31は、ハーフミラー25を透過した第1分岐レーザ光L1の一部とハーフミラー25で反射した第2分岐レーザ光L2の一部とが合波されてなるレーザ光である。第2合波レーザ光L32は、ハーフミラー25で反射した第1分岐レーザ光L1の一部とハーフミラー25を透過した第2分岐レーザ光L2の一部とが合波されてなるレーザ光である。
The combined laser beam L3 is a linearly polarized laser beam, and here. P-polarized laser light. The combined laser beam L3 includes a first combined laser beam L31 coaxial with the first branched laser beam L1, and a second combined laser beam L32 coaxial with the second branched laser beam L2. The first combined laser beam L31 is a laser beam formed by combining a part of the first branched laser beam L1 transmitted through the
第2光路P2は、偏光ビームスプリッタ21からミラー22までの第3光路P21と、ミラー24からハーフミラー25までの第4光路P22と、ミラー22からミラー24までの第5光路P23を含む。第5光路P23は、第1光路P1と同じ光路長を有する。第1光路P1と第2光路P2との光路差(つまり、第3光路P21及び第4光路P22の光路長)は、ファイバレーザ10の可干渉距離よりも長い。可干渉距離は、第1分岐レーザ光L1と第2分岐レーザ光L2とを合波するときに光の干渉現象が現れる距離の上限である。
The second optical path P2 includes a third optical path P21 from the
光学系30は、空間光変調器(第1偏光素子)31、4f光学系32、集光レンズ33、空間光変調器(第2偏光素子)35、4f光学系36、及び、集光レンズ37を有する。空間光変調器31,35は、例えば反射型液晶(LCOS:Liquid Crystal on Silicon)の空間光変調器(SLM:Spatial Light Modulator)である。空間光変調器31は、第1合波レーザ光L31が入射される偏光素子である。空間光変調器31は、入射した第1合波レーザ光L31を変調すると共に反射する。空間光変調器35は、第2合波レーザ光L32が入射される偏光素子である。空間光変調器35は、入射した第2合波レーザ光L32を変調すると共に反射する。
The
空間光変調器31,35は、変調パターンを表示可能な表示部を有する。空間光変調器31は、第1合波レーザ光L31を変調パターンに入射させることで、当該変調パターンに応じて第1合波レーザ光L31の波面を調整する。空間光変調器35は、第2合波レーザ光L32を変調パターンに入射させることで、当該変調パターンに応じて第2合波レーザ光L32の波面を調整する。空間光変調器31,35のそれぞれでは、表示させる各変調パターンを適宜設定することにより、第1及び第2合波レーザ光L31,L32それぞれの変調(例えば、強度、振幅、位相、偏光等の変調)が可能となる。
The spatial
4f光学系32は、空間光変調器31によって変調された第1合波レーザ光L31の波面形状を調整(波面調整)する調整光学系である。4f光学系32は、空間光変調器31と集光レンズ33との間の光路上に配置されている。4f光学系36は、空間光変調器35によって変調された第2合波レーザ光L32の波面形状を調整する調整光学系である。4f光学系36は、空間光変調器35と集光レンズ37との間の光路上に配置されている。
The 4f
集光レンズ33は、第1合波レーザ光L31を対象物Tに集光する。集光レンズ37は、第2合波レーザ光L32を対象物Tに集光する。集光レンズ33,37のそれぞれは、複数のレンズを含んで構成されていてもよい。
The condensing
以上に説明したレーザ光照射装置100では、光源装置1において、ファイバレーザ10から出射されたランダム偏光のレーザ光L0は、偏光ビームスプリッタ21で偏光成分ごとに分岐される。1/2波長板23により、第2分岐レーザ光L2の偏光成分が回転させられ、第2分岐レーザ光L2の偏光方向が第1分岐レーザ光L1の偏光方向と同じ(平行)になるように変えられる。そして、ハーフミラー25によって、互いに同じ偏光方向になった第1及び第2分岐レーザ光L1,L2が合波され、最終的に単一の直線偏光に揃えられた合波レーザ光L3として出力される。
In the laser
合波レーザ光L3のうちの第1合波レーザ光L31は、光学系30において、空間光変調器31に入射し、空間光変調器31の表示部に表示された変調パターンに応じて変調された後、4f光学系32により波面調整される。4f光学系32で波面調整された第1合波レーザ光L31は、集光レンズ33により集光されて対象物Tに対してレーザ光Lとして照射される。合波レーザ光L3のうちの第2合波レーザ光L32は、光学系30において、空間光変調器35に入射し、空間光変調器35の表示部に表示された変調パターンに応じて変調された後、4f光学系36により波面調整される。4f光学系36で波面調整された第2合波レーザ光L32は、集光レンズ37により集光されて対象物Tに対してレーザ光Lとして照射される。
The first combined laser beam L31 in the combined laser beam L3 is incident on the spatial
図2は、ファイバレーザ10から出射されるレーザ光L0を説明するためのグラフである。縦軸は、レーザ出力を基準出力値で除算して得た規格化レーザ出力である。横軸は、時間(hour)である。「P偏光」のデータラベル値は、ファイバレーザ10で出射されたレーザ光L0を偏光子等で分離してなるP偏光の偏光成分の規格化レーザ出力を示す。「S偏光」のデータラベル値は、ファイバレーザ10で出射されたレーザ光L0を偏光子等で分離してなるS偏光の偏光成分の規格化レーザ出力を示す。「合計」のデータラベル値は、当該P偏光の偏光成分と当該S偏光の偏光成分との合計を示す。
FIG. 2 is a graph for explaining the laser beam L0 emitted from the
図2に示されるように、合計のレーザ出力は、所定時間の経過後に安定している一方、P偏光及びS偏光のレーザ出力は、合計に比べて変動が大きい。これは、ファイバレーザ10から出射されるレーザ光L0は、ランダム偏光の偏光を有しており、P偏光の偏光成分とS偏光の偏光成分との比率が変動する。よって、P偏光及びS偏光のレーザ出力が、当該ファイバレーザ10の偏光特性に影響されて不安定になるためである。例えば、ファイバレーザ10では、導光ファイバ12等のファイバが曲がったり潰れたり等すると、出射したレーザ光L0の偏光に影響が発生する場合がある。導光ファイバ12を動かすと動かしている間、偏光が揺らぐ場合がある。したがって、一般的には、光源装置においてランダム偏光のレーザ光L0を出射するファイバレーザ10を用いると、得られる直線偏光のレーザ光に偏光素子(空間光変調器等)を利用することは困難であることがわかる。
As shown in FIG. 2, the total laser output is stable after a predetermined time, while the P-polarized and S-polarized laser outputs have larger fluctuations than the total. This is because the laser light L0 emitted from the
これに対して、本実施形態に係る光源装置1によれば、上述したように、ファイバレーザ10から出射されたランダム偏光のレーザ光L0が第1及び第2分岐レーザ光L1,L2に分岐され、第2分岐レーザ光L2の偏光方向が1/2波長板23で第1分岐レーザ光L1の偏光方向と同じになるように変えられ、第1及び第2分岐レーザ光L1,L2がハーフミラー25で合波されて合波レーザ光L3として出力される。よって、ランダム偏光のレーザ光L0を出射するファイバレーザ10を用いた場合でも、当該ファイバレーザ10の偏光特性によらずに、安定して直線偏光のレーザ光L(合波レーザ光L3)を得ることが可能となる。既存の光源装置よりも安価で高出力な光源装置1を得ることができる。
On the other hand, according to the
図3は、光源装置1から出力される合波レーザ光L3を説明するためのグラフである。縦軸は、レーザ出力を基準出力値で除算して得た規格化レーザ出力である。横軸は、時間(min)である。「元出力」のデータラベル値は、ファイバレーザ10で出射されたランダム偏光のレーザ光L0の規格化レーザ出力を示す。
FIG. 3 is a graph for explaining the combined laser light L3 output from the
「第1分岐レーザ光」のデータラベル値は、ランダム偏光のレーザ光L0を偏光ビームスプリッタ21で分岐しただけの第1分岐レーザ光L1の規格化レーザ出力を示す。ここでの「第1分岐レーザ光」のデータラベル値は、偏光調整(つまり、ハーフミラー25により、第1分岐レーザ光L1と1/2波長板23で偏光方向を変えた第2分岐レーザ光L2とを合波すること)の前におけるP偏光の第1分岐レーザ光L1の規格化レーザ出力である。「合波レーザ光」のデータラベル値は、合波レーザ光L3の規格化レーザ出力を示す。ここでの「合波レーザ光」のデータラベル値は、偏光調整の後におけるP偏光の第1合波レーザ光L31の規格化レーザ出力である。図3に示される結果によれば、偏光調整後の合波レーザ光L3のレーザ出力が、元出力の安定したレーザ出力と同等の出力変動になることを確認することができる。
The data label value of the “first branched laser beam” indicates the normalized laser output of the first branched laser beam L1 which is obtained by just branching the randomly polarized laser beam L0 by the
光源装置1では、ファイバレーザ10は、本体部11とレーザヘッド部13とを有する、いわゆるヘッド分離型のファイバレーザを構成する。この場合、その導光ファイバ12の曲げ等により、ファイバレーザ10から出射するレーザ光L0の偏光に影響が出やすい。よって、用いたファイバレーザ10の偏光特性によらずに安定して直線偏光のレーザ光Lを得るという上記効果は、特に有効である。
In the
光源装置1では、第1分岐レーザ光L1の第1光路P1と第2分岐レーザ光L2の第2光路P2との光路差が、ファイバレーザ10の可干渉距離よりも長い。この構成によれば、ハーフミラー25によって合波する第1及び第2分岐レーザ光L1,L2が干渉するのを抑制することが可能となる。ファイバレーザ10から出射されたレーザ光L0と同じビームプロファイルの合波レーザ光L3を出力できる。
In the
光源装置1では、合波レーザ光L3は、第1分岐レーザ光L1と同軸の第1合波レーザ光L31、及び、第2分岐レーザ光L2と同軸の第2合波レーザ光L32を含む。この構成によれば、2つの直線偏光の第1及び第2合波レーザ光L31,L32が得られることから、種々の仕様等に適用させ易くすることができる。
In the
レーザ光照射装置100においても、光源装置1により、ランダム偏光のレーザ光L0を出射するファイバレーザ10を用いた場合に安定して直線偏光のレーザ光Lを得るという上記効果を奏する。また、レーザ光照射装置100では、ハーフミラー25によって合波されることで得られた2つの第1及び第2合波レーザ光L31,L32の双方を利用したレーザ光照射が可能となる。レーザ出力を2ポート有する(2ビーム利用する)仕様のレーザ光照射装置100を得ることができる。
Also in the laser
[第2実施形態]
次に、第2実施形態のレーザ光照射装置について説明する。本実施形態の説明では、第1実施形態と異なる点について説明する。
Second Embodiment
Next, a laser beam irradiation apparatus according to a second embodiment will be described. In the description of the present embodiment, points different from the first embodiment will be described.
図4は、第2実施形態に係るレーザ光照射装置200を示す概略構成図である。図4に示されるように、レーザ光照射装置200は、光学系30(図1参照)に代えて光学系40を備える点で、第1実施形態と異なる。光学系40は、空間光変調器(偏光素子)31、4f光学系32、及び、集光レンズ33及びビームダンパー44を有する。ビームダンパー44は、第2合波レーザ光L32を遮蔽する。
FIG. 4 is a schematic configuration view showing a laser
レーザ光照射装置200では、合波レーザ光L3のうちの第1合波レーザ光L31は、光学系30において、空間光変調器31に入射し、空間光変調器31の表示部に表示された変調パターンに応じて変調された後、4f光学系32により波面調整される。4f光学系32で波面調整された第1合波レーザ光L31は、集光レンズ33により集光されて対象物Tに対してレーザ光Lとして照射される。一方、合波レーザ光L3のうちの第2合波レーザ光L32は、ビームダンパー44により遮蔽されて終端させられる。
In the laser
以上、レーザ光照射装置200においても、光源装置1により、ランダム偏光のレーザ光L0を出射するファイバレーザ10を用いた場合に安定して直線偏光のレーザ光Lを得るという上記効果を奏する。また、レーザ光照射装置200では、ハーフミラー25によって合波されることで得られた2つの第1及び第2合波レーザ光L31,L32の一方のみを利用したレーザ光照射が可能となる。レーザ出力を1ポート有する(1ビーム利用する)仕様のレーザ光照射装置200を得ることができる。
As described above, also in the laser
以上、実施形態について説明したが、本発明の一態様は、上記実施形態に限られず、各請求項に記載した要旨を変更しない範囲で変形し、又は他のものに適用してもよい。 The embodiment has been described above, but one aspect of the present invention is not limited to the above-described embodiment, and may be modified or applied to other things without departing from the scope of the invention described in each claim.
上記実施形態は、偏光素子として空間光変調器31,35を備えているが、レーザ光照射装置100,200に適用される偏光素子は特に限定されず、空間光変調器31,35に代えて又は加えて、他の偏光素子を備えていてもよい。
Although the said embodiment is equipped with the spatial
上記第2実施形態では、第1合波レーザ光L31を空間光変調器31に入射させ、第2合波レーザ光L32をビームダンパー44に入射させたが、これとは逆に、第2合波レーザ光L32を空間光変調器31に入射させ、第1合波レーザ光L31をビームダンパー44に入射させてもよい。この場合、第1合波レーザ光L31はビームダンパー44により遮蔽されて終端させられる一方、第2合波レーザ光L32は、空間光変調器31の表示部に表示された変調パターンに応じて変調された後、4f光学系32により波面調整され、集光レンズ33により集光されて対象物Tに対してレーザ光Lとして照射される。
In the second embodiment, the first combined laser beam L31 is made incident on the spatial
1…光源装置、10…ファイバレーザ、11…本体部、12…導光ファイバ、13…レーザヘッド部、21…偏光ビームスプリッタ、23…1/2波長板(波長板)、25…ハーフミラー、30…光学系、31…空間光変調器(偏光素子,第1偏光素子)、35…空間光変調器(第2偏光素子)、40…光学系、44…ビームダンパー、100,200…レーザ光照射装置、P1…第1光路(第1分岐レーザ光の光路)、P2…第2光路(第2分岐レーザ光の光路)。
DESCRIPTION OF
Claims (6)
前記ファイバレーザで出射した前記レーザ光を、偏光成分ごとに第1分岐レーザ光と第2分岐レーザ光とへ分岐する偏光ビームスプリッタと、
前記第2分岐レーザ光の偏光方向を前記第1分岐レーザ光の偏光方向と同じになるように変える波長板と、
前記偏光ビームスプリッタで分岐された前記第1分岐レーザ光と前記波長板で偏光方向を変えた前記第2分岐レーザ光とを、合波して合波レーザ光として出力するハーフミラーと、を備える光源装置。 A fiber laser that emits randomly polarized laser light;
A polarization beam splitter that branches the laser beam emitted by the fiber laser into a first branch laser beam and a second branch laser beam for each polarization component;
A wavelength plate that changes the polarization direction of the second branched laser beam to be the same as the polarization direction of the first branched laser beam;
And a half mirror that multiplexes the first split laser beam split by the polarization beam splitter and the second split laser beam whose polarization direction is changed by the wavelength plate, and outputs the combined laser beam as a combined laser beam. Light source device.
種光を増幅する本体部と、
前記本体部に導光ファイバを介して接続され、前記レーザ光を出射するレーザヘッド部と、を有する、請求項1に記載の光源装置。 The fiber laser is
A main unit that amplifies seed light;
The light source device according to claim 1, further comprising: a laser head unit connected to the main body via a light guide fiber and configured to emit the laser light.
前記第1合波レーザ光が入射される第1偏光素子、及び前記第2合波レーザ光が入射される第2偏光素子を有する光学系を備える、レーザ光照射装置。 A laser beam irradiation apparatus comprising the light source apparatus according to claim 4, wherein
A laser beam irradiation apparatus comprising: an optical system having a first polarization element to which the first combined laser beam is incident, and a second polarization element to which the second combined laser beam is incident.
前記第1合波レーザ光及び前記第2合波レーザ光の何れか一方が入射される偏光素子、及び、前記第1合波レーザ光及び前記第2合波レーザ光の何れか他方を遮蔽するビームダンパーを有する光学系を備える、レーザ光照射装置。 A laser beam irradiation apparatus comprising the light source apparatus according to claim 4, wherein
A polarization element on which any one of the first combined laser beam and the second combined laser beam is incident, and the other one of the first combined laser beam and the second combined laser beam is blocked. Laser light irradiation apparatus provided with the optical system which has a beam damper.
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| JPH0385514A (en) * | 1989-08-30 | 1991-04-10 | Sumitomo Electric Ind Ltd | Circularly polarized light generator |
| JPH10170868A (en) * | 1996-12-10 | 1998-06-26 | Nec Corp | Optical filter module, and light amplifier using it |
| JP2009145429A (en) * | 2007-12-11 | 2009-07-02 | Univ Of Yamanashi | Optical wavelength filter device |
| JP2010204508A (en) * | 2009-03-05 | 2010-09-16 | V Technology Co Ltd | Optical switching device |
| JP2016051147A (en) * | 2014-09-02 | 2016-04-11 | 浜松ホトニクス株式会社 | Optical modulation device and optical system |
| US20170082494A1 (en) * | 2015-08-12 | 2017-03-23 | Government Of The United States As Represetned By The Secretary Of The Air Force | Photon entanglement router |
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| JPH0385514A (en) * | 1989-08-30 | 1991-04-10 | Sumitomo Electric Ind Ltd | Circularly polarized light generator |
| JPH10170868A (en) * | 1996-12-10 | 1998-06-26 | Nec Corp | Optical filter module, and light amplifier using it |
| JP2009145429A (en) * | 2007-12-11 | 2009-07-02 | Univ Of Yamanashi | Optical wavelength filter device |
| JP2010204508A (en) * | 2009-03-05 | 2010-09-16 | V Technology Co Ltd | Optical switching device |
| JP2016051147A (en) * | 2014-09-02 | 2016-04-11 | 浜松ホトニクス株式会社 | Optical modulation device and optical system |
| US20170082494A1 (en) * | 2015-08-12 | 2017-03-23 | Government Of The United States As Represetned By The Secretary Of The Air Force | Photon entanglement router |
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