KR20140074788A - Apparatus and Method for emitting light - Google Patents
Apparatus and Method for emitting light Download PDFInfo
- Publication number
- KR20140074788A KR20140074788A KR1020120145716A KR20120145716A KR20140074788A KR 20140074788 A KR20140074788 A KR 20140074788A KR 1020120145716 A KR1020120145716 A KR 1020120145716A KR 20120145716 A KR20120145716 A KR 20120145716A KR 20140074788 A KR20140074788 A KR 20140074788A
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- light
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- optical fiber
- laser diode
- pulse
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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
- H01S3/06704—Housings; Packages
-
- 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
- H01S3/06754—Fibre amplifiers
-
- 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
- H01S3/08—Construction or shape of optical resonators or components thereof
- H01S3/08018—Mode suppression
- H01S3/08022—Longitudinal modes
- H01S3/08027—Longitudinal modes by a filter, e.g. a Fabry-Perot filter is used for wavelength setting
-
- 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
- H01S3/10061—Polarization control
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- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Engineering & Computer Science (AREA)
- Plasma & Fusion (AREA)
- Optics & Photonics (AREA)
- Microelectronics & Electronic Packaging (AREA)
- Lasers (AREA)
- Optical Modulation, Optical Deflection, Nonlinear Optics, Optical Demodulation, Optical Logic Elements (AREA)
Abstract
Description
A method for outputting light, and an optical output apparatus.
Utilizing the properties of light with monochromaticity, coherence, and directionality, light is currently being utilized in various fields. In the biotechnology and medical fields, light is being utilized in a variety of ways such as observation of tissues and cells, diagnosis of diseases, or laser procedures.
Especially in the medical field, since the internal structure of the human body can be observed without directly cutting the human body with the light characteristics as described above, the cause, position and progress of various diseases can be easily and safely detected by using light. In addition to the development of technologies for generating light such as high power, continuous wave, and wavelength sweeping, the depth of light transmission is improved and tomographic images of living tissue or cells can be acquired in high resolution in real time have.
SUMMARY OF THE INVENTION The present invention has been made in view of the above problems, and it is an object of the present invention to provide a method of outputting light and an optical output device. The present invention also provides a computer-readable recording medium on which a program for causing the computer to execute the method is provided. The method of outputting light and the technical object to be achieved by the optical output device are not limited to the above-described technical problems, and other technical problems may exist.
An optical output apparatus according to an aspect of the present invention includes: a first laser diode for generating pulsed light of a first wavelength whose intensity, width, and repetition rate are controlled according to an applied current; A second laser diode for generating pulsed light of a second wavelength whose intensity, width, and repetition rate are controlled according to the applied current; A laser diode control unit for controlling a current applied to the first laser diode and the second laser diode; An amplifying unit for amplifying multi-wavelength light in which the first pulse light and the second pulse light are combined; And a nonlinear gain medium in which a wavelength conversion characteristic is changed by the incident light, wherein the wavelength conversion characteristic of the nonlinear gain medium is changed based on the wavelength conversion characteristic of the nonlinear gain medium changed by the multi- And an optical fiber for outputting light obtained as a result of pumping of the optical fiber.
According to another aspect of the present invention, there is provided a method of outputting light in an optical output apparatus including at least two laser diodes, comprising: controlling a current applied to the at least two laser diodes; Generating pulse lights having different wavelengths whose intensity, width, and repetition rate are controlled in accordance with the currents applied to the at least two laser diodes; Amplifying multi-wavelength light in which pulse lights generated from the at least two laser diodes are combined; Linear gain medium, the wavelength conversion characteristic of the nonlinear gain medium being changed by the amplified multi-wavelength light in an optical fiber including a nonlinear gain medium whose wavelength conversion characteristic is changed by the incident light, And outputting the output signal.
An optical coherent tomography apparatus for photographing a single layer by irradiating light on a target according to another aspect of the present invention includes a first laser diode and a second laser diode for controlling a current applied to the first laser diode, A second pulse of a second wavelength having a controlled intensity, a width, and a repetition rate according to a current applied to the second laser diode, A nonlinear gain medium including a nonlinear gain medium which emits a pulse light and amplifies the multiwavelength light in which the first pulse light and the second pulse light are combined and whose wavelength conversion characteristic changes according to the amplified multiwavelength light, An optical output device for outputting light obtained as a result of pumping of the nonlinear gain medium by the amplified multi-wavelength light based on a wavelength conversion characteristic of the gain medium; An interferometer for separating the output light into measurement light and reference light, irradiating the measurement light to the object, and receiving the response light reflected from the object; A detector for detecting an interference signal generated by the response light and the reference light; And a video signal processor for generating a tomographic image of the object using the detected interference signal.
According to still another aspect of the present invention, there is provided a computer-readable recording medium having recorded thereon a program for causing a computer to execute a method of outputting light.
According to the above, optical pumping is performed by using multi-wavelength light combined with pulse light generated in the laser diodes, and intensity, width, repetition rate, and the like of each pulse light in the optical output device outputting the obtained light The spectrum of the light output from the optical output device can be shaped into a desired shape by controlling at least one of the polarized light and the polarized light.
The optical output device outputs light having an extended bandwidth in a predetermined wavelength range by controlling at least one of the intensity, the width, the repetition rate, and the polarization of each of the pulse lights generated in the laser diodes can do.
By controlling at least one of the intensity, the width, the repetition rate, and the polarization of each of the pulse light beams generated in the laser diodes, the optical output device can generate light having any type of optical spectrum including a Gaussian shape in a predetermined wavelength region Can be output.
1 is a block diagram illustrating an optical output apparatus according to an embodiment of the present invention.
2 is a block diagram illustrating an optical output apparatus according to another embodiment of the present invention.
3 is a view illustrating an optical output apparatus according to an embodiment of the present invention.
4 is a view illustrating an optical output apparatus according to another embodiment of the present invention.
5 is a view illustrating an optical output apparatus according to another embodiment of the present invention.
FIG. 6 is a graph showing a change in optical spectrum of the light output from the optical output device under the control of the laser diode control unit shown in FIG. 1;
FIG. 7 is a diagram illustrating an optical coherence tomography apparatus including the optical output apparatus shown in FIG. 1 according to an embodiment of the present invention. Referring to FIG.
8 is a flowchart illustrating a method of outputting light by an optical output apparatus according to an embodiment of the present invention.
Hereinafter, preferred embodiments of the present invention will be described in detail with reference to the drawings.
1 is a block diagram illustrating an optical output apparatus according to an embodiment of the present invention. Referring to FIG. 1, an
The
The
The
Accordingly, the
The laser
Accordingly, the laser
For example, in order for the
According to one embodiment, the laser
According to another embodiment, the laser
According to another embodiment, the laser
The laser
The amplifying
The
The
For example, in order for the
The
At this time, the nonlinear gain medium of the
Accordingly, the
The wavelength conversion characteristics of the nonlinear gain medium of the
For example, in order for the
According to one embodiment, the
According to another embodiment, the
Alternatively, the
According to an embodiment, the
According to another embodiment, the
2 is a block diagram illustrating an optical output apparatus according to another embodiment of the present invention. 2, the
The laser
The
The
The
The
The amplifying
The
The
The nonlinear gain medium of the
The
According to an embodiment, the
Accordingly, the
3 is a view illustrating an optical output apparatus according to an embodiment of the present invention. 3, the
The
The
The
The first laser
The second laser
The
The
The optical attenuator (VA) 220 additionally adjusts the ratio of the output of the first pulse light output from the
The amplifying
The
The
The
The optical fiber bundle (TFB) 234 couples the pump light output from the
The ytterbium-doped optical fiber (YDF) 235 amplifies the multi-wavelength light input to the
The
The
The
The
Accordingly, the
4 is a view illustrating an optical output apparatus according to another embodiment of the present invention. 4, the
The
The amplifying unit 230 'amplifies the multi-wavelength light in which the first pulse light generated in the
The amplification unit 230 'shown in FIG. 4 amplifies the multi-wavelength light in which the first pulse light and the second pulse light are combined, in two stages, as compared with the
The
The
The
The first
The first ytterbium-doped optical fiber (YDF) 2305 transmits the multi-wavelength light input to the amplification unit 230 'through the first Yb doped
The
The
The
The
The second optical fiber bundle (TFB) 2314 is formed by coupling the pump light output from the
The second ytterbium-doped optical fiber (YDF) 2315 transmits the multi-wavelength light amplified by the first ytterbium-doped
For convenience of explanation, the optical fiber for amplifying the multi-wavelength light in the predetermined wavelength region in the amplification unit 230 'is represented by Y-doped optical fiber (YDF) 235, but the present invention is not limited thereto. Instead of the Yb doped optical fiber (YDF), the amplifying unit 230 'may include an optical fiber doped with Erbium Doped Fiber (EDF) or another material in accordance with the wavelength band of the multi-wavelength light input to the amplifying unit 230' Can be used. As described above, the amplifying unit 230 'can amplify the multi-wavelength light in two stages of the first Yb doped optical fiber (YDF) 2305 and the second Yb doped optical fiber (YDF) 2315. In the present embodiment, the optical fibers for amplifying the multi-wavelength light in the first and second steps are represented by the same type of Yb doped optical fiber, but the present invention is not limited thereto and optical fibers doped with different materials can be used.
The
The
The
The
As described above, the amplifier 230 'of the
5 is a view illustrating an optical output apparatus according to another embodiment of the present invention. 5, the
The
The first laser
The second laser
The first pulse light and the second pulse light, respectively, whose polarization is controlled by the
The
The multi-wavelength light whose polarization is controlled by the
The
The
The nonlinear gain medium of the
The
FIG. 6 is a graph showing a change in optical spectrum of the light output from the optical output device under the control of the laser diode control unit shown in FIG. 1 to FIG.
The horizontal axis represents the wavelength (nm) and the vertical axis represents the relative spectral output (dB). The
Accordingly, the
The
The
The
According to an embodiment, the
According to another embodiment, the
The
The
The
The
The
8 is a flowchart illustrating a method of outputting light in accordance with an embodiment of the present invention. Referring to FIG. 8, the method shown in FIG. 8 is composed of steps that are processed in a time-series manner in the optical output devices shown in FIGS. 1 to 5 and FIG. Therefore, even if the contents are omitted in the following description, it can be understood that the above description about the optical output devices shown in Figs. 1 to 5 and Fig. 7 also applies to the method shown in Fig.
In
According to one embodiment, the laser
According to another embodiment, the laser
In
In
In
Meanwhile, the above-described method can be implemented in a general-purpose digital computer that can be created as a program that can be executed by a computer and operates the program using a computer-readable recording medium. In addition, the structure of the data used in the above-described method can be recorded on a computer-readable recording medium through various means. The computer-readable recording medium includes a storage medium such as a magnetic storage medium (e.g., ROM, floppy disk, hard disk, etc.), optical reading medium (e.g., CD ROM,
It will be understood by those skilled in the art that various changes in form and details may be made therein without departing from the spirit and scope of the invention as defined by the appended claims. Therefore, the disclosed methods should be considered from an illustrative point of view, not from a restrictive point of view. The scope of the present invention is defined by the appended claims rather than by the foregoing description, and all differences within the scope of equivalents thereof should be construed as being included in the present invention.
100 ... optical output device
110 ... first laser diode
120 ... second laser diode
130 ... laser diode control unit
140 ... amplifying unit
150 ... optical fiber
Claims (25)
A first laser diode for generating pulsed light of a first wavelength whose intensity, width, and repetition rate are controlled in accordance with an applied current;
A second laser diode for generating pulsed light of a second wavelength whose intensity, width, and repetition rate are controlled according to the applied current;
A laser diode control unit for controlling a current applied to the first laser diode and the second laser diode;
An amplifying unit for amplifying multi-wavelength light in which the first pulse light and the second pulse light are combined; And
A nonlinear gain medium in which a wavelength conversion characteristic is varied by an incident light, wherein the wavelength conversion characteristic of the nonlinear gain medium is changed based on the wavelength conversion characteristic of the nonlinear gain medium modified by the multiwavelength light amplified by the amplification unit, And an optical fiber for outputting light obtained as a result of the pumping.
Further comprising at least one polarization controller for controlling at least one polarization of the first pulse light, the second pulse light, the multi-wavelength light, and the amplified multi-wavelength light.
Wherein the position of the at least one polarization controller can be changed according to a shape of a spectrum of light to be output from the optical output device.
Wherein the laser diode control unit controls at least one of intensity, width, and repetition rate of each of the first pulse light and the second pulse light, or the at least one polarization controller controls the first pulse light, Wherein the optical output device shapes the spectrum of light output from the optical fiber by controlling one of polarized light of the multi-wavelength light and the amplified multi-wavelength light.
The laser diode control unit controls the intensity, width, and repetition rate of each of the first pulse light and the second pulse light so that the light output from the optical fiber has a Gaussian shape optical spectrum in a third wavelength range. Wherein the at least one polarization controller controls at least one of the first pulse light, the second pulse light, the multi-wavelength light, and the amplified multi-wavelength light, Output device.
Wherein the laser diode control unit controls the intensity and width of the first pulse light and the second pulse light so that the light output from the optical fiber has a flat optical spectrum in a third wavelength range, Or at least one of the polarization controllers controls one of the first pulse light, the second pulse light, the multi-wavelength light, and the amplified multi-wavelength light, Device.
Wherein the wavelength conversion characteristic of the nonlinear gain medium can be changed by changing at least one of a type and a composition ratio of materials included in the nonlinear gain medium and a geometry and a length of the optical fiber.
Wherein the optical fiber is a high non-linear fiber (HNLF).
Wherein the optical fiber is a high-birefringent optical fiber (Hi-Bi fiber).
The nonlinear gain medium includes materials included in a nonlinear gain medium of a high nonlinear optical fiber (HNLF) and a high birefringent optical fiber (Hi-Bi fiber) according to a predetermined component ratio Wherein the light output device comprises:
The amplifying unit
An optical fiber for increasing an output gain of the multi-wavelength light in a predetermined wavelength region according to characteristics of a gain medium to be pumped;
A fourth laser diode for emitting light of a fourth wavelength that promotes pumping of the gain medium of the optical fiber; And
And a tapered fiber bundle (TFB) for coupling the multi-wavelength light and the fourth wavelength light so that the light of the fourth wavelength is incident on the optical fiber.
A first optical fiber for increasing an output gain of the multi-wavelength light in a predetermined wavelength region according to characteristics of a gain medium included therein;
A fourth laser diode for emitting light of a fourth wavelength that promotes pumping of the gain medium contained in the first optical fiber;
A first optical fiber bundle (TFB) for coupling the multi-wavelength light and the fourth wavelength light so that light of the fourth wavelength is incident on the first optical fiber;
A second optical fiber for increasing the output gain of the multi-wavelength light amplified by the first optical fiber in a predetermined wavelength region according to characteristics of the included gain medium;
A fifth laser diode that emits light of a fifth wavelength that promotes pumping of the gain medium included in the second optical fiber; And
And a second optical fiber bundle (TFB) that combines the multi-wavelength light amplified by the first optical fiber and the light of the fifth wavelength so that light of the fifth wavelength is incident on the second optical fiber Wherein the optical output device comprises:
Further comprising: at least one laser diode for generating pulsed light whose intensity, width, and repetition rate are controlled in accordance with an applied current,
Wherein the amplifying unit amplifies the multi-wavelength light in which the first pulse light, the second pulse light, and the pulse light generated from the at least one laser diode are combined,
Wherein the laser diode control unit controls a current applied to the first laser diode, the second laser diode, and the at least one laser diode.
At least one polarization controller for controlling at least one polarization of the first pulse light, the second pulse light, the pulse lights generated from the at least one laser diode, the multi-wavelength light, and the amplified multi-wavelength light; Further comprising a light source for emitting light.
Controlling a current applied to the at least two laser diodes;
Generating pulse lights having different wavelengths whose intensity, width, and repetition rate are controlled in accordance with the currents applied to the at least two laser diodes;
Amplifying multi-wavelength light in which pulse lights generated from the at least two laser diodes are combined;
Linear gain medium, the wavelength conversion characteristic of the nonlinear gain medium being changed by the amplified multi-wavelength light in an optical fiber including a nonlinear gain medium whose wavelength conversion characteristic is changed by the incident light, / RTI >
The amplifying step
Receiving pulse lights generated from the at least two laser diodes;
Adjusting the polarization of each of the pulsed light beams generated from the at least two laser diodes;
Combining the pulsed light with the polarization control to generate one multi-wavelength light; And
And amplifying the multi-wavelength light.
The amplifying step
Receiving pulse lights generated from the at least two laser diodes;
Combining the pulse lights generated from the at least two laser diodes to generate one multi-wavelength light;
Adjusting the polarization of the multi-wavelength light; And
And amplifying the polarization-controlled multi-wavelength light.
The amplifying step
Receiving pulse lights generated from the at least two laser diodes;
Combining the pulse lights generated from the at least two laser diodes to generate one multi-wavelength light;
Emitting a fourth wavelength of light that promotes pumping of the gain medium contained in the first optical fiber;
Coupling the multi-wavelength light and the fourth wavelength light so that the light of the fourth wavelength is incident on the first optical fiber; And
And increasing an output gain of the multi-wavelength light in a predetermined wavelength region by the light of the fourth wavelength and the gain medium included in the first optical fiber.
The amplifying step
Receiving pulse lights generated from the at least two laser diodes;
Combining the pulse lights generated from the at least two laser diodes to generate one multi-wavelength light;
Emitting a fourth wavelength of light that promotes pumping of the gain medium contained in the first optical fiber;
Coupling the multi-wavelength light and the fourth wavelength light so that the light of the fourth wavelength is incident on the first optical fiber;
Increasing an output gain of the multi-wavelength light in a predetermined wavelength region by the light of the fourth wavelength and the gain medium included in the first optical fiber;
Emitting light of a fifth wavelength that promotes pumping of the gain medium contained in the second optical fiber;
Combining the multi-wavelength light amplified by the first optical fiber and the light of the fifth wavelength so that the light of the fifth wavelength is incident on the second optical fiber; And
And increasing an output gain of the multi-wavelength light amplified by the first optical fiber in a predetermined wavelength region by the gain medium included in the light of the fifth wavelength and the gain medium included in the second optical fiber.
Wherein the controlling step controls at least one of an intensity, a width, and a repetition rate of each of the pulse lights in order to shape a spectrum of light output from the optical output device.
Wherein the optical output device controls at least one of an intensity, a width, and a repetition rate of each of the pulse lights to adjust a polarization of each of the pulse lights to shape a spectrum of light output from the optical fiber.
Wherein the wavelength conversion characteristic of the nonlinear gain medium is changed by changing at least one of a type and a composition ratio of materials included in the nonlinear gain medium and a geometry and a length of the optical fiber.
The first laser diode and the second laser diode are controlled to emit pulsed light of a first wavelength whose intensity, width, and repetition rate are controlled in accordance with the current applied to the first laser diode And emits a second pulse light of a second wavelength whose intensity, width, and repetition rate are controlled in accordance with the current applied to the second laser diode, and outputs the second pulse light of the second wavelength controlled by the multi- Linear gain medium of the optical fiber including a nonlinear gain medium in which the wavelength conversion characteristic is changed according to the amplified multi-wavelength light, amplifies the nonlinear gain medium by pumping the nonlinear gain medium by the amplified multi- An optical output device for outputting light obtained as a result of the light;
An interferometer for separating the output light into measurement light and reference light, irradiating the measurement light to the object, and receiving the response light reflected from the object;
A detector for detecting an interference signal generated by the response light and the reference light; And
And an image signal processor for generating a tomographic image of the object using the detected interference signal.
Wherein the optical output device controls at least one of intensity, width, repetition rate, and polarization of each of the first pulse light and the second pulse light in order to shape a spectrum of light output from the optical output device The optical coherence tomography apparatus.
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Cited By (2)
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KR102255317B1 (en) * | 2020-11-04 | 2021-05-24 | 국방과학연구소 | Apparatus and method for amplification of laser, computer-readable storage medium and computer program |
KR102392830B1 (en) * | 2020-11-19 | 2022-04-29 | 광주과학기술원 | Optical fiber laser device controlling beam shape and operating method there of |
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JP2010140047A (en) * | 2002-11-21 | 2010-06-24 | Furukawa Electric Co Ltd:The | Light source, waveform shaper, sbs suppressor, and pulse light source |
KR20120122102A (en) * | 2011-04-28 | 2012-11-07 | 광주과학기술원 | Method of flexible burst mode operation of pulse laser system with multiple seed and laser system with flexible burst mode operation |
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JP2010140047A (en) * | 2002-11-21 | 2010-06-24 | Furukawa Electric Co Ltd:The | Light source, waveform shaper, sbs suppressor, and pulse light source |
KR20120122102A (en) * | 2011-04-28 | 2012-11-07 | 광주과학기술원 | Method of flexible burst mode operation of pulse laser system with multiple seed and laser system with flexible burst mode operation |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
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KR102255317B1 (en) * | 2020-11-04 | 2021-05-24 | 국방과학연구소 | Apparatus and method for amplification of laser, computer-readable storage medium and computer program |
KR102392830B1 (en) * | 2020-11-19 | 2022-04-29 | 광주과학기술원 | Optical fiber laser device controlling beam shape and operating method there of |
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