CN109672078B - Pulse seed source and laser system with same - Google Patents
Pulse seed source and laser system with same Download PDFInfo
- Publication number
- CN109672078B CN109672078B CN201811390574.9A CN201811390574A CN109672078B CN 109672078 B CN109672078 B CN 109672078B CN 201811390574 A CN201811390574 A CN 201811390574A CN 109672078 B CN109672078 B CN 109672078B
- Authority
- CN
- China
- Prior art keywords
- port
- output
- beam combiner
- isolator
- saturable absorber
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Active
Links
- 230000007246 mechanism Effects 0.000 claims abstract description 55
- 239000006096 absorbing agent Substances 0.000 claims abstract description 45
- 239000013307 optical fiber Substances 0.000 claims abstract description 34
- 239000000835 fiber Substances 0.000 claims abstract description 30
- 230000010354 integration Effects 0.000 claims abstract description 22
- 238000005086 pumping Methods 0.000 claims abstract description 6
- 230000003287 optical effect Effects 0.000 claims description 30
- 238000012423 maintenance Methods 0.000 abstract description 6
- 230000010287 polarization Effects 0.000 description 5
- 239000004065 semiconductor Substances 0.000 description 5
- 230000003321 amplification Effects 0.000 description 4
- 230000000694 effects Effects 0.000 description 4
- 238000003199 nucleic acid amplification method Methods 0.000 description 4
- 238000005516 engineering process Methods 0.000 description 3
- 238000000034 method Methods 0.000 description 3
- 230000002411 adverse Effects 0.000 description 2
- 230000009286 beneficial effect Effects 0.000 description 2
- 239000013078 crystal Substances 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 230000004927 fusion Effects 0.000 description 2
- 238000012545 processing Methods 0.000 description 2
- 230000004044 response Effects 0.000 description 2
- 239000007787 solid Substances 0.000 description 2
- OKTJSMMVPCPJKN-UHFFFAOYSA-N Carbon Chemical compound [C] OKTJSMMVPCPJKN-UHFFFAOYSA-N 0.000 description 1
- 239000011358 absorbing material Substances 0.000 description 1
- 230000007547 defect Effects 0.000 description 1
- 238000013461 design Methods 0.000 description 1
- 238000011161 development Methods 0.000 description 1
- 229910021389 graphene Inorganic materials 0.000 description 1
- 230000006872 improvement Effects 0.000 description 1
- 238000002955 isolation Methods 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 230000008569 process Effects 0.000 description 1
- 238000011160 research Methods 0.000 description 1
- 239000000126 substance Substances 0.000 description 1
Classifications
-
- 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
- H01S3/10084—Frequency control by seeding
-
- 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
- H01S3/06708—Constructional details of the fibre, e.g. compositions, cross-section, shape or tapering
- H01S3/06716—Fibre compositions or doping with active elements
-
- 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
- H01S3/10038—Amplitude control
- H01S3/10046—Pulse repetition rate control
-
- 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
- H01S3/11—Mode locking; Q-switching; Other giant-pulse techniques, e.g. cavity dumping
- H01S3/1106—Mode locking
- H01S3/1112—Passive mode locking
- H01S3/1115—Passive mode locking using intracavity saturable absorbers
Abstract
The invention provides a pulse seed source and a laser system with the same, wherein the pulse seed source comprises a pumping source, a beam splitter, a first beam combiner, a resonant cavity component and an output mechanism; the output end of the pump source is connected with the input end of the beam splitter, the first output port of the beam splitter is connected with the input port of the first beam combiner, and the first output port of the first beam combiner is connected with the input port of the resonant cavity component; the second output port of the beam splitter and the second output port of the first beam combiner are both connected with the input port of the output mechanism; the resonant cavity component comprises a reflection grating, a first gain fiber and a saturable absorber integration mechanism; one port of the reflection grating is connected with a first output port of the first beam combiner, the other port of the reflection grating is connected with one port of the first gain optical fiber, and the other port of the first gain optical fiber is connected with the saturable absorber integration mechanism. The invention has simple structure and low maintenance cost.
Description
Technical Field
The present invention relates to laser technology, and more particularly, to a pulsed seed source and a laser system having the same.
Background
Ultrafast laser has extremely short pulse and extremely high peak power, so that laser cold processing in the true sense is realized when the ultrafast laser interacts with substances, and therefore, ultrafast laser technology is also popular in research of various countries at present, and represents the development direction of the laser technology at present. The ultra-fast picosecond and femtosecond seed source is a key component of the ultra-fast laser, and the reliability and stability of the laser are directly determined by the performance of the seed source.
Currently, there are three main methods for obtaining picosecond pulses from industrialized picosecond seed sources: 1. directly modulating a fast-response semiconductor laser; 2. the picosecond pulse output is realized by using nonlinear polarization rotation mode locking effect through some nonlinear crystals; 3. picosecond pulses are obtained by using a saturable absorbing material as an optical switch.
Picosecond pulses obtained by directly modulating a fast response semiconductor laser typically have a pulse width limit of hundreds picoseconds and a power of tens to hundreds microwatts, and cannot be used as a seed source for an ultrafast laser. The ultra-fast laser picosecond seed source used in the industrial market at present mainly uses nonlinear crystals, and uses nonlinear polarization rotation mode locking effect to realize pulse output with pulse width of tens of femtoseconds to tens of picoseconds. The solid seed source has the defects of complex structure, large volume, high cost, poor stability, high maintenance cost and the like due to the special spatial structure of the solid seed source.
Disclosure of Invention
First, the technical problem to be solved
The invention provides a pulse seed source and a laser system with the pulse seed source, which are used for solving the technical problems of complex structure, poor stability and high maintenance cost of the pulse seed source in the prior art.
(II) technical scheme
In order to solve the above technical problems, according to an aspect of the present invention, there is provided a pulse seed source, including a pump source, a beam splitter, a first beam combiner, a resonant cavity assembly, and an output mechanism; the output end of the pump source is connected with the input end of the optical splitter, the first output port of the optical splitter is connected with the input port of the first beam combiner, and the first output port of the first beam combiner is connected with the input port of the resonant cavity component; the second output port of the beam splitter and the second output port of the first beam combiner are both connected with the input port of the output mechanism;
the resonant cavity assembly comprises a reflection grating, a first gain fiber and a saturable absorber integration mechanism; one port of the reflection grating is connected with the first output port of the first beam combiner, the other port of the reflection grating is connected with one port of the first gain optical fiber, and the other port of the first gain optical fiber is connected with the saturable absorber integration mechanism.
Further, the saturable absorber integration mechanism comprises a saturable absorber; the saturable absorber is adhered to a jumper wire port of the saturable absorber integration mechanism, and the end face of the saturable absorber is perpendicular to an optical path projected onto the saturable absorber.
Further, the output mechanism comprises a second beam combiner and an output terminal; the second output port of the beam splitter is connected with the second output port of the first beam combiner, and the second output port of the beam splitter is connected with the input port of the second beam combiner;
the first isolator is arranged between the second beam combiner and the output terminal, an input port of the first isolator is connected with an output port of the second beam combiner, and an output port of the first isolator is connected with the output terminal.
Further, a second gain fiber is also included; and one port of the second gain optical fiber is connected with the output port of the second beam combiner, and the other port of the second gain optical fiber is connected with the input port of the first isolator.
Further, a second isolator is also included; the input port of the second isolator is connected with the second output port of the first beam combiner, and the output port of the second isolator is connected with the input port of the output mechanism.
Further, a second gain fiber is also included; one port of the second gain optical fiber is connected with a second output port of the first beam combiner, and the other port of the second gain optical fiber is connected with an input port of the output mechanism.
Further, a second isolator is also included; the input port of the second isolator is connected with the second output port of the first beam combiner, the output port of the second isolator is connected with one port of the second gain optical fiber, and the other port of the second gain optical fiber is connected with the input port of the output mechanism.
According to another aspect of the present invention, there is also provided a laser system comprising the above pulsed seed source.
(III) beneficial effects
The application provides a pulse seed source and have laser system of this pulse seed source, its beneficial effect mainly as follows:
dividing an optical signal emitted by a pumping source into two paths, wherein one path is directly output to a pumping leg of a second beam combiner, and the other path is processed by a resonant cavity component and then output to a signal leg of the second beam combiner, and amplified and then output as a laser signal; in addition, the saturable absorber of the saturable absorber integration mechanism in the resonant cavity assembly is stuck to the jumper wire port, and the saturable absorber is vertically arranged in the light path, so that the structure can be simplified, and the stability of the pulse seed source can be improved; in addition, through the two-stage gain optical fiber amplification treatment, the return light is isolated by the two isolators, so that the signal intensity can be further enhanced and the stable operation can be realized. The pulse seed source can be used for providing seed source laser with stable power and pulse width less than 10 ps.
Drawings
FIG. 1 is a schematic diagram of a pulsed seed source according to an embodiment of the present invention;
FIG. 2 is a schematic diagram of a pulsed seed source according to an embodiment of the present invention;
in the figure, the 1-saturable absorber integrating mechanism, the 2-first gain optical fiber, the 3-reflection grating, the 4-first beam combiner, the 5-second isolator, the 6-beam splitter, the 7-pump source, the 8-second beam combiner, the 9-first isolator, the 10-output terminal and the 11-second gain optical fiber.
Detailed Description
The following describes in further detail the embodiments of the present invention with reference to the drawings and examples. The following examples are illustrative of the invention and are not intended to limit the scope of the invention.
In the description of the invention, it should be noted that the terms "first," "second," and "second," are used for clarity in describing the numbering of product components and do not represent any substantial distinction, unless explicitly stated or defined otherwise. The terms "front" and "rear" are used in a conventional sense for the structure of the product. "last", "next" are described based on the arrangement order. The directions of the upper and the lower are all the directions shown in the drawings. The specific meaning of the above terms in the present invention can be understood by those of ordinary skill in the art according to the specific circumstances.
It should be noted that unless explicitly stated or limited otherwise, the term "coupled" is to be construed broadly, and may be, for example, fixedly coupled, detachably coupled, or integrally coupled; can be directly connected or indirectly connected through an intermediate medium. The specific meaning of the terms in the invention will be understood by those of ordinary skill in the art in a specific context.
Referring to fig. 1, the present embodiment provides a pulse seed source, which includes a pump source 7, a beam splitter 6, a first beam combiner 4, a resonant cavity assembly, and an output mechanism; the output end of the pump source 7 is connected with the input end of the beam splitter 6, the first output port of the beam splitter 6 is connected with the input port of the first beam combiner 4, and the first output port of the first beam combiner 4 is connected with the input port of the resonant cavity component; the second output port of the beam splitter 6 and the second output port of the first beam combiner 4 are both connected with the input port of the output mechanism;
the resonant cavity assembly comprises a reflection grating 3, a first gain optical fiber 2 and a saturable absorber integration mechanism 1; one port of the reflection grating 3 is connected to the first output port of the first beam combiner 4, the other port of the reflection grating 3 is connected to one port of the first gain fiber 2, and the other port of the first gain fiber 2 is connected to the saturable absorber integration mechanism 1.
The pump source 7 may be a semiconductor pump laser. The generated light source of the pump source 7 enters the optical splitter 6, and is split into two paths of optical signals by the optical splitter 6: a first optical signal and a second optical signal. The beam splitter's split ratio may be adjusted according to the actual situation, for example, it may be 3:7. The first path of optical signals enter the resonant cavity assembly through the first output port of the first beam combiner 4, and enter the output mechanism through the second output port of the first beam combiner 4 after the signal amplification processing and the frequency adjustment of the resonant cavity assembly. The first beam combiner 4 may be a wavelength division multiplexer or a (2+1) x 1 polarization maintaining beam combiner. The beam splitter may employ a polarization maintaining beam splitter.
The resonant cavity assembly comprises a reflection grating 3, a first gain fiber 2 and a saturable absorber integration mechanism 1. The first path of optical signal enters the first beam combiner 4, propagates to the reflection grating 3 through the first beam combiner 4, and propagates to the first gain optical fiber 2 after being reflected by the reflection grating 3. The first path of optical signals are amplified by the first gain optical fiber 2 and then projected to the saturable absorber integration mechanism 1. The optical signal projected to the saturable absorber integration mechanism 1 is transmitted to the first beam combiner 4 through the first gain optical fiber 2 and the reflection grating 3 after being totally reflected, and is output to the output mechanism through the second output port of the first beam combiner 4. Meanwhile, the second optical signal also enters the output mechanism from the second output port of the optical splitter 6, and the two optical signals are output as a laser source via the output mechanism.
It can be understood that the pump source 7, the beam splitter 6, the first beam combiner 4, the resonant cavity assembly and the output mechanism are all welded by optical fibers.
The emission grating, the first gain optical fiber 2 and the saturable absorber integration mechanism 1 form a cavity, and the intensity of the first optical signal can be amplified in the process of propagation of the first optical signal in the cavity; in addition, the frequency of the output laser can be more accurately adjusted by adjusting the cavity length of the cavity. The structure is simple, the components are few, and the maintenance is easy.
In a specific embodiment, the saturable absorber integration mechanism 1 comprises a saturable absorber; the saturable absorber is adhered to the jumper port of the saturable absorber integrated mechanism 1, and the end face of the saturable absorber is perpendicular to the light path projected onto the saturable absorber. On the basis of the above-described embodiment, the present embodiment specifically describes the structure of the saturable absorber integration mechanism 1.
The saturable absorber integration mechanism 1 may be a semiconductor saturable absorber mirror or the like. The saturable absorber of the saturable absorber integration mechanism 1 may be a semiconductor such as SESAM or graphene. The saturable absorber is adhered to the jumper wire port, so that the design of a space light path can be avoided, the stability is higher, the maintenance is easier, and the maintenance cost is low. And moreover, a structure that the saturable absorber is adhered to the jumper wire port is adopted, so that all-fiber fusion of the pulse seed source is more convenient, and the structure can be further simplified. Meanwhile, the saturable absorber is vertically arranged in the light path, so that the total reflection of the first optical signal is facilitated, and the pulse power of mode locking is improved.
In a specific embodiment, the output mechanism comprises a second beam combiner 8 and an output terminal 10; the second output port of the beam splitter 6 is connected with the input port of the second beam combiner 8;
a first isolator 9 is arranged between the second beam combiner 8 and the output terminal 10, an input port of the first isolator 9 is connected with an output port of the second beam combiner 8, and an output port of the first isolator 9 is connected with the output terminal 10.
On the basis of the above embodiments, the present embodiment specifically describes the structure of the output mechanism. The provision of the first isolator 9 between the second beam combiner 8 and the output terminal 10 can prevent or mitigate the adverse effect of back light on the pulsed seed source or the laser system. The second beam combiner 8 may have two input ports, the second output port of the first beam combiner 4 is connected to one input port of the second beam combiner 8, and the second output port of the beam splitter is connected to the other input port of the second beam combiner 8. The two paths of optical signals enter the second beam combiner 8 for beam combination and then are output.
The first beam combiner 4, the second beam combiner 8, and the first isolator 9 may be connected by optical fiber fusion. The second beam combiner 8 may be a wavelength division multiplexer or a (2+1) x 1 polarization maintaining beam combiner. The output terminal 10 may employ bare fibers, jumper outputs, collimated outputs, etc.
In a specific embodiment, the second gain fiber 11 is further included; one port of the second gain fiber 11 is connected to the output port of the second combiner 8, and the other port of the second gain fiber 11 is connected to the input port of the first isolator 9. On the basis of the above embodiments, the present embodiment specifically describes the arrangement of the second gain fiber 11.
The second gain fiber 11 may be disposed between the second combiner 8 and the first isolator 9. The optical signal may be amplified in one step. The second gain optical fiber 11 is matched with the first gain optical fiber 2, so that two-stage amplification treatment can be carried out on an optical signal, the signal intensity of output laser is conveniently enhanced, and the output power is improved.
In a specific embodiment, a second separator 5 is also included; the input port of the second isolator 5 is connected with the second output port of the first beam combiner, and the output port of the second isolator 5 is connected with the input port of the output mechanism. On the basis of the above embodiments, the present embodiment specifically describes the setting state of the second separator 5. A second isolator 5 is arranged between the first beam combiner 4 and the output mechanism, and forms two-stage isolation with the first isolator 9, so that return light can be further isolated, and adverse effects of the return light on a pulse seed source or a laser system are reduced. The output port of the second isolator 5 is connected to the input port of the output mechanism, and the second isolator 5 may be connected to an input port of the second combiner 8.
In a specific embodiment, referring to fig. 2, a second gain fiber 11 is further included; one port of the second gain fiber 11 is connected to the second output port of the first combiner 4, and the other port of the second gain fiber 11 is connected to the input port of the output mechanism. On the basis of the above embodiments, this embodiment specifically describes another arrangement form of the second gain fiber 11.
The second gain optical fiber 11 is disposed between the first beam combiner 4 and the output mechanism, when the output mechanism includes the second beam combiner 8, one port of the second gain optical fiber 11 is connected to the second output port of the first beam combiner 4, and the other port of the second gain optical fiber 11 is connected to an input port of the second beam combiner 8.
In a specific embodiment, a second separator 5 is also included; the input port of the second isolator 5 is connected to the second output port of the first combiner 4, the output port of the second isolator is connected to one port of the second gain fiber 11, and the other port of the second gain fiber 11 is connected to the input port of the output mechanism. On the basis of the above embodiments, the present embodiment specifically describes another setting state of the second separator 5. When the second gain fiber 11 is disposed between the first beam combiner 4 and the second beam combiner 8, the output port of the second isolator 5 is connected to one port of the second gain fiber 11, and the other port of the second gain fiber 11 is connected to the input port of the output mechanism.
Specifically, the first gain fiber 2 and the second gain fiber 11 may both use a high ytterbium-doped single-clad polarization-maintaining fiber or a high ytterbium-doped double-clad polarization-maintaining fiber. It will be appreciated that the specification parameters of the above devices, such as the first separator 9 and the second separator 5, may be selected according to actual needs, for example, the maximum passing power of the first separator 9 and the second separator 5, etc.
In a specific embodiment, there is also provided a laser system comprising the pulsed seed source described above.
The pulse seed source and the laser system with the pulse seed source divide the optical signal emitted by the pumping source into two paths, wherein one path of the optical signal is directly output to one input port of the second beam combiner, namely the pumping leg of the second beam combiner, and the other path of the optical signal is processed by the resonant cavity component and then output to the other input port of the second beam combiner, namely the signal leg of the second beam combiner, and the amplified optical signal is used as a laser signal to be output; in addition, the saturable absorber of the saturable absorber integration mechanism in the resonant cavity assembly is stuck to the jumper wire port, and the saturable absorber is vertically arranged in the light path, so that the structure can be simplified, and the stability of the pulse seed source can be improved; in addition, through the two-stage gain optical fiber amplification treatment, the return light is isolated by the two isolators, so that the signal intensity can be further enhanced and the stable operation can be realized. The pulse seed source can be used for providing seed source laser with stable power and pulse width less than 10 ps.
Finally, the method of the present invention is only a preferred embodiment and is not intended to limit the scope of the present invention. Any modification, equivalent replacement, improvement, etc. made within the spirit and principle of the present invention should be included in the protection scope of the present invention.
Claims (8)
1. The pulse seed source is characterized by comprising a pumping source, a beam splitter, a first beam combiner, a resonant cavity assembly and an output mechanism; the output end of the pump source is connected with the input end of the optical splitter, the first output port of the optical splitter is connected with the input port of the first beam combiner, and the first output port of the first beam combiner is connected with the input port of the resonant cavity component; the second output port of the beam splitter and the second output port of the first beam combiner are both connected with the input port of the output mechanism;
the resonant cavity assembly comprises a reflection grating, a first gain fiber and a saturable absorber integration mechanism; one port of the reflection grating is connected with the first output port of the first beam combiner, the other port of the reflection grating is connected with one port of the first gain optical fiber, and the other port of the first gain optical fiber is connected with the saturable absorber integration mechanism.
2. The pulsed seed source of claim 1, wherein the saturable absorber integration mechanism comprises a saturable absorber; the saturable absorber is adhered to a jumper wire port of the saturable absorber integration mechanism, and the end face of the saturable absorber is perpendicular to an optical path projected onto the saturable absorber.
3. The pulsed seed source of claim 1, wherein the output mechanism comprises a second combiner and an output terminal; the second output port of the beam splitter is connected with the second output port of the first beam combiner, and the second output port of the beam splitter is connected with the input port of the second beam combiner;
the first isolator is arranged between the second beam combiner and the output terminal, an input port of the first isolator is connected with an output port of the second beam combiner, and an output port of the first isolator is connected with the output terminal.
4. The pulsed seed source of claim 3, further comprising a second gain fiber; and one port of the second gain optical fiber is connected with the output port of the second beam combiner, and the other port of the second gain optical fiber is connected with the input port of the first isolator.
5. The pulsed seed source of claim 1 or 4, further comprising a second isolator; the input port of the second isolator is connected with the second output port of the first beam combiner, and the output port of the second isolator is connected with the input port of the output mechanism.
6. The pulsed seed source of claim 1, further comprising a second gain fiber; one port of the second gain optical fiber is connected with a second output port of the first beam combiner, and the other port of the second gain optical fiber is connected with an input port of the output mechanism.
7. The pulsed seed source of claim 6, further comprising a second isolator; the input port of the second isolator is connected with the second output port of the first beam combiner, the output port of the second isolator is connected with one port of the second gain optical fiber, and the other port of the second gain optical fiber is connected with the input port of the output mechanism.
8. A laser system comprising the pulsed seed source of any one of claims 1-7.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN201811390574.9A CN109672078B (en) | 2018-11-21 | 2018-11-21 | Pulse seed source and laser system with same |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN201811390574.9A CN109672078B (en) | 2018-11-21 | 2018-11-21 | Pulse seed source and laser system with same |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| CN109672078A CN109672078A (en) | 2019-04-23 |
| CN109672078B true CN109672078B (en) | 2024-01-26 |
Family
ID=66142124
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CN201811390574.9A Active CN109672078B (en) | 2018-11-21 | 2018-11-21 | Pulse seed source and laser system with same |
Country Status (1)
| Country | Link |
|---|---|
| CN (1) | CN109672078B (en) |
Citations (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6097741A (en) * | 1998-02-17 | 2000-08-01 | Calmar Optcom, Inc. | Passively mode-locked fiber lasers |
| CN102185243A (en) * | 2009-12-11 | 2011-09-14 | 苏州大学 | Mode-locked all-fiber laser with all-normal-dispersion cavity |
| KR101334498B1 (en) * | 2012-07-19 | 2013-11-29 | 인하대학교 산학협력단 | Actively pulsed fiber laser device with a saturable absorber |
| CN103701022A (en) * | 2013-12-19 | 2014-04-02 | 北京工业大学 | Double-resonant-cavity all-optical-fiber mode-locked pulse laser |
| KR20170135541A (en) * | 2016-05-31 | 2017-12-08 | 한국과학기술원 | A long-term stable all-polarization-maintaining fiber laser oscillator based on saturable absorber |
| CN209266837U (en) * | 2018-11-21 | 2019-08-16 | 武汉锐科光纤激光技术股份有限公司 | Pulse seed source and laser system with the pulse seed source |
-
2018
- 2018-11-21 CN CN201811390574.9A patent/CN109672078B/en active Active
Patent Citations (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6097741A (en) * | 1998-02-17 | 2000-08-01 | Calmar Optcom, Inc. | Passively mode-locked fiber lasers |
| CN102185243A (en) * | 2009-12-11 | 2011-09-14 | 苏州大学 | Mode-locked all-fiber laser with all-normal-dispersion cavity |
| KR101334498B1 (en) * | 2012-07-19 | 2013-11-29 | 인하대학교 산학협력단 | Actively pulsed fiber laser device with a saturable absorber |
| CN103701022A (en) * | 2013-12-19 | 2014-04-02 | 北京工业大学 | Double-resonant-cavity all-optical-fiber mode-locked pulse laser |
| KR20170135541A (en) * | 2016-05-31 | 2017-12-08 | 한국과학기술원 | A long-term stable all-polarization-maintaining fiber laser oscillator based on saturable absorber |
| CN209266837U (en) * | 2018-11-21 | 2019-08-16 | 武汉锐科光纤激光技术股份有限公司 | Pulse seed source and laser system with the pulse seed source |
Non-Patent Citations (1)
| Title |
|---|
| "基于SESAM的全光纤被动锁模光纤激光器";王雄飞 等.;《激光与红外》;第45卷(第11期);1319-1324 * |
Also Published As
| Publication number | Publication date |
|---|---|
| CN109672078A (en) | 2019-04-23 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US7567376B2 (en) | High power fiber chirped pulse amplification system utilizing telecom-type components | |
| US9008133B2 (en) | Giant-chirp oscillator for use in fiber pulse amplification system | |
| JP2010093246A (en) | Passive mode synchronized fiber laser employing carbon nanotube | |
| EP1729379A1 (en) | Optical fiber laser using rare earth-added fiber and wide band light source | |
| CN107045248B (en) | Nonlinear optical fiber amplification broadband four-wave mixing generation device | |
| US8897325B1 (en) | Fiber laser | |
| KR101875992B1 (en) | Laser source having a peak power of more than 100 terawatts and high contrast | |
| CN111373614B (en) | Device for providing optical radiation | |
| CN101083381A (en) | Semiconductor laser seed pulse principal oscillation magnifying full-fiber laser | |
| WO2013127334A1 (en) | Optical fiber laser with super continuous spectrum | |
| CN110600978A (en) | Ytterbium-doped nanosecond pulse line laser source based on all-fiber structure | |
| JP2009506560A (en) | Fiber laser | |
| US8194709B2 (en) | High-repetition-rate guided-mode femtosecond laser | |
| CN109672078B (en) | Pulse seed source and laser system with same | |
| CN101771236A (en) | Chirped pulse amplification fiber laser system without stretcher | |
| CN110350387A (en) | A kind of full polarization fibre mode-locked laser of the high single pulse energy of low-repetition-frequency | |
| TW201228161A (en) | Mode locked fiber laser system | |
| CN209266837U (en) | Pulse seed source and laser system with the pulse seed source | |
| CN110957627A (en) | High-power 2-micron intermediate infrared thulium-doped optical fiber picosecond laser | |
| CN217281617U (en) | Pulse width adjustable optical fiber laser | |
| CA2693288C (en) | Low-average-power parabolic pulse amplification | |
| CN103825177B (en) | A kind of pulse full polarization fibre laser based on multiple non-linear amplification annular mirrors | |
| CN110086078A (en) | Picosecond optical fiber seed laser | |
| CN113783090B (en) | Optical fiber amplifier | |
| CN210443791U (en) | Low-noise high-speed pulse light source optical path structure |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| PB01 | Publication | ||
| PB01 | Publication | ||
| SE01 | Entry into force of request for substantive examination | ||
| SE01 | Entry into force of request for substantive examination | ||
| GR01 | Patent grant | ||
| GR01 | Patent grant |