CN204835194U - Multi -wavelength fiber laser - Google Patents
Multi -wavelength fiber laser Download PDFInfo
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- CN204835194U CN204835194U CN201520575091.1U CN201520575091U CN204835194U CN 204835194 U CN204835194 U CN 204835194U CN 201520575091 U CN201520575091 U CN 201520575091U CN 204835194 U CN204835194 U CN 204835194U
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Abstract
The utility model discloses a multi -wavelength fiber laser, including adjustable light source (1), optical coupler (2) and spectrum appearance (9), the first port (a) of adjustable light source (1) and optical coupler (2) is through the fiber connection, and the third port (c) of optical coupler (2) is through linear chamber no. 1 or annular chamber no. 2 or linear chamber no. 1 and two back and second port (b) fiber connections of annular chamber, and the fourth port (d) of optical coupler (2) and spectrum appearance (9) are through the fiber connection. Single times of brillouin's frequency displacement wavelength interval, double brillouin's frequency displacement wavelength interval and triple brillouin frequency displacement wavelength interval can be realized to it.
Description
Technical field
The utility model belongs to technical field of photo communication, and be specifically related to the tunable multi-wavelength optical fiber laser in a kind of wavelength interval based on Brillouin scattering, it can realize the Laser output that wavelength interval is 0.082nm, 0.164nm and 0.246nm.
Background technology
The technical fields such as the generation of multi-wavelength optical fiber laser in optical communication system, Fibre Optical Sensor, spectrum analysis, microwave signal source and THz source have very important application, always the dark concern by numerous scientific workers and Ge great laser manufacturer.The close wavelength-division multiplex technology of the communications field improves message capacity greatly, utilizes fiber laser to produce microwave signal source etc. by beat frequency technology, and multiple-wavelength laser is absolutely necessary equipment.Current multi-wavelength optical fiber laser of a great variety, structure is varied, realize method that multi-wavelength exports and principle different.
Wherein, multi-wavelength Brillouin erbium-doped fiber laser the Linear Amplifer effect of the stimulated Brillouin scattering Image magnify in optical fiber and Er-doped fiber to be combined and the multi-wavelength that realizes ambient-temp-stable exports, the multi-wavelength interval that multi-wavelength Brillouin erbium-doped fiber laser exports mainly is determined by the characteristic of the optical fiber as brillouin gain medium, and the Brillouin shift of conventional optical fiber communication is in 10GHz (0.08nm) left and right.When light source as dense wave division multipurpose (DWDM) system of the multi-wavelength optical fiber laser of wavelength interval about 10GHz, add the complexity of Demodulation Systems, and easily cause the crosstalk between channel, reduce actual using value.
To sum up, current multi-wavelength optical fiber laser is not good enough on output stability, and the tunable ability of each wavelength.
Utility model content
For the multi-wavelength output stability solving current multi-wavelength optical fiber laser is not good enough, the problem of ability that wavelength interval is tunable, the utility model discloses the tunable multi-wavelength optical fiber laser in a kind of wavelength interval, it can realize single times of Brillouin shift wavelength interval, double Brillouin frequency shift wavelength interval and three times of Brillouin shift wavelength intervals.
The utility model takes following technical scheme: a kind of multi-wavelength optical fiber laser, comprise tunable light source (1), optical coupler (2) and spectrometer (9), tunable light source (1) passes through Fiber connection with the first port (a) of optical coupler (2), 3rd port (c) of optical coupler (2) is by linear cavity one (realizing the Laser output of single times of Brillouin shift) or annular chamber two (realizing the Laser output of double Brillouin frequency shift) or linear cavity one and annular chamber two is rear and the second port (b) Fiber connection, 4th port (d) and the spectrometer (9) of optical coupler (2) pass through Fiber connection.
Preferably, the wavelength interval of linear cavity Output of laser is single times of Brillouin shift, linear cavity one comprises first wave division multiplexer (3-1), first pump laser (4-1), first Er-doped fiber (5-1), first optical circulator (6-1), first monomode fiber (7-1), second optical circulator (6-2), 3rd port (c) of optical coupler (2) and the first port (e) of the first light wavelength division multiplexing (3-1) pass through Fiber connection, second port (f) and first pump laser (4-1) of first wave division multiplexer (3-1) pass through Fiber connection, 3rd port (g) of first wave division multiplexer (3-1) is connected with Er-doped fiber (5-1), the other end of Er-doped fiber (5-1) connects the first port (h) of the first optical circulator (6-1), second port (i) of the first optical circulator (6-1) is connected with the first monomode fiber (7-1), the other end of the first monomode fiber (7-1) connects the first port (k) of the second optical circulator (6-2), and the second port (l) and the 3rd port (m) of the second optical circulator (7-2) pass through Fiber connection, 3rd port (j) of the first optical circulator (6-1) and the second port (b) of optical coupler (2) pass through Fiber connection.
Preferably, the wavelength interval of annular chamber Output of laser is double Brillouin frequency shift, annular chamber two comprises four-port photocirculator (8), second monomode fiber (7-2), second Er-doped fiber (5-2), Second Wave division multiplexer (3-2), second pump laser (4-2), 3rd port (c) of optical coupler (2) and the first port (n) of four-port photocirculator (8) pass through Fiber connection, second port (o) of four-port photocirculator (8) connects one end of the second monomode fiber (7-2), the other end of the second monomode fiber (7-2) connects one end of Er-doped fiber (5-2), the other end of Er-doped fiber (5-2) connects the first port (r) of the second light wavelength division multiplexing (3-2), second port (s) of the second light wavelength division multiplexing (3-2) is by Fiber connection second pump laser (4-2), 3rd port (t) of the second light wavelength division multiplexing (3-2) is by the 3rd port (p) of Fiber connection four-port photocirculator (8), 4th port (q) of four-port photocirculator (8) and the second port (b) of optical coupler (2) pass through Fiber connection.
Preferably, when accessing linear cavity and annular chamber in system successively, the optical maser wavelength exported is spaced apart three times of Brillouin shifts, and linear cavity one comprises first wave division multiplexer (3-1), the first pump laser (4-1), the first Er-doped fiber (5-1), the first optical circulator (6-1), the first monomode fiber (7-1), the second optical circulator (6-2), described annular chamber two comprises four-port photocirculator (8), the second monomode fiber (7-2), the second Er-doped fiber (5-2), Second Wave division multiplexer (3-2), the second pump laser (4-2), 3rd port (c) of optical coupler (2) and the first port (e) of the first light wavelength division multiplexing (3-1) are by Fiber connection, and the second port (f) and first pump laser (4-1) of first wave division multiplexer (3-1) pass through Fiber connection, 3rd port (g) of first wave division multiplexer (3-1) is connected with Er-doped fiber (5-1), the other end of Er-doped fiber (5-1) connects the first port (h) of the first optical circulator (6-1), second port (i) of the first optical circulator (6-1) is connected with the first monomode fiber (7-1), the other end of the first monomode fiber (7-1) connects the first port (k) of the second optical circulator (6-2), second port (l) and the 3rd port (m) of the second optical circulator (7-2) pass through Fiber connection, form speculum, 3rd port (j) of the first optical circulator (6-1) and the first port (n) of four-port photocirculator (8) pass through Fiber connection, second port (o) of four-port photocirculator (8) connects one end of monomode fiber (7-2), the other end of monomode fiber (7-2) connects one end of Er-doped fiber (5-2), the other end of Er-doped fiber (5-2) connects the first port (r) of the second light wavelength division multiplexing (3-2), second port (s) of the second light wavelength division multiplexing (3-2) is by Fiber connection second pump laser (4-2), 3rd port (t) of the second light wavelength division multiplexing (3-2) is by the 3rd port (p) of Fiber connection four-port photocirculator (8), 4th port (q) of four-port photocirculator (8) and the second port (b) of optical coupler (2) pass through Fiber connection.
Preferably, the gain ranging of the first Er-doped fiber (5-1) is 1530nm to 1570nm, and Er-doped fiber length is 8m.
Preferably, the gain ranging of the second Er-doped fiber (5-2) is 1530nm to 1570nm, and Er-doped fiber length is 8m.
Preferably, produce the first monomode fiber (7-1) the choice criteria silica fiber of Brillouin scattering effect, fiber lengths is 25km.
Preferably, produce the second monomode fiber (7-2) the choice criteria silica fiber of Brillouin scattering effect, fiber lengths is 25km.
Preferably, the 3rd port of optical coupler (2) is 90% port, and the 4th port is 10% port.
The utility model adopts without all optical fibre structure of discrete component, has good beam quality, power output is high, output wavelength interval is tunable, compact conformation, the advantage such as stable and reliable for performance, while can realize the tuning output in wavelength interval.
The multi-wavelength that the utility model laser can realize three kinds of different wave length intervals exports: the multi-wavelength of single times of Brillouin shift exports, the multi-wavelength of double Brillouin frequency shift exports and the multi-wavelength of three times of Brillouin shifts exports.When only access in system tunable light source (1), optical coupler (2), linear cavity one and spectrometer (9) time, achieve the multi-wavelength optical fiber laser at one single times Brillouin shift interval; When only access in system tunable light source (1), optical coupler (2), annular chamber two and spectrometer (9) time, achieve the multi-wavelength optical fiber laser of a double Brillouin frequency shift interval; When access in system tunable light source (1), optical coupler (2), linear cavity one, annular chamber two and spectrometer (9) time, achieve the multi-wavelength optical fiber laser at three times of Brillouin shift intervals.
General principle of the present utility model is as follows:
The laser principle at single times of Brillouin shift interval: Brillouin's pump signal (BP) that narrow line width regulatable laser (1) exports is through a port of optical coupler (1), 90% signal enters the e port of first light wavelength division multiplexing (3-1) of linear cavity one along clockwise direction after being coupled to c port, then the pump light signals coupled in common produced with the first pump laser (4-1) enters in Er-doped fiber (5-1) to be exaggerated, signal after amplification enters in SMF (7-1) from bottom to top via the h-i port of the first optical circulator (6-1), when the intensity of the BP signal be exaggerated exceedes the threshold value producing brillouin gain, due to SBS effect, top-down 1 rank Stokes signal (BS) that same BP signal propagation direction is contrary can be produced in a fiber.1 rank BS signal exports the b port of optical coupler (2) to through the i-j port of the first optical circulator (6-1), the signal of 10% exports spectrometer to, 90% signal coupling enters in linear cavity one, produce the Stokes signal of high-order, the multi-wavelength that can be observed single times of Brillouin shift interval like this on spectrometer exports.
The laser principle of double Brillouin frequency shift interval: Brillouin's pump signal (BP) that narrow line width regulatable laser exports inputs to the n-o port of four-port photocirculator (8) through a port of optical coupler (1), clockwise direction is transferred in SMF (7-2), when the intensity of BP signal exceedes the threshold value producing brillouin gain, due to SBS effect, 1 rank Stokes signal (BS) along counterclockwise transmission that same BP signal propagation direction is contrary can be produced in a fiber.1 rank BS signal continues at cavity circulation through the o-p port of four-port photocirculator (8), then by by (3-2), (4-2) EDFA formed with (5-2) amplifies, again enter in SMF (7-2) and produce 2 rank Stokes light, 2 rank Stokes fairing clockwises are from the p-q port of four-port circulator (8), after optical coupler (2), 10% exports from OSA, remaining 90% enters clockwise transmission in annular chamber two through the n-o port of four-port photocirculator (8), when 2 rank BS signal strength signal intensities meet brillouin gain threshold condition, can as the anticlockwise 3 rank BS signals of new BP signal excitation.3 rank BS signals are the same with initial BP signal, and in annular chamber two, left-hand circular produces the Stokes signal on 4 rank, and 4 rank Stokes signals are clockwise direction transmission in chamber, exports, by that analogy through the p-q of four port circulators (8).In annular chamber two, the Stokes signal on odevity rank is respectively along counterclockwise and clockwise direction transmission, and the Stokes signal of odd-order is limited in annular chamber Inner eycle, only have the BS signal of initial BP signal and even-order can coupling output, the multi-wavelength achieving wavelength interval double Brillouin frequency shift exports.This process constantly repeats, until when the intensity of the new BS signal produced does not meet brillouin gain threshold condition, cascade process stops.The output of laser is carried out observation by spectrometer (AQ6370B) and is measured.
The BP signal that the laser principle at three times of Brillouin shift intervals: TLS (1) produces transfers in linear cavity one through optical coupler (2) can produce 1 rank BS signal, at this moment during input signal (BP) of 1 rank BS signal as annular chamber two, in annular chamber two, meet SBS effect condition, clockwise direction will be obtained and transmit 3 rank Stokes signals, 3 rank Stokes signals clockwise transmission in annular chamber two is output to during the p-q port of four-port circulator (8), this process constantly repeats, until when the intensity of the new BS signal produced does not meet brillouin gain threshold condition, cascade process stops.The output of laser is carried out observation by spectrometer (AQ6370B) and is measured.Spectrometer (9) can be observed BP signal and the 3 rank Stokes signals of TLS generation, so also just achieve the Laser output that wavelength interval is three times of Brillouin shifts.
The structure of the utility model laser is simple, cost is low, be easy to that fibre system is integrated, wavelength interval is adjustable (0.082nm, 0.164nm, 0.246nm), the good stability of line width, Laser output, and it is specially adapted to the technical fields such as DWDM light source, light sensing, photo-induced microwave signal source.
Accompanying drawing explanation
Fig. 1 is the structural representation of the tunable multi-wavelength optical fiber laser in wavelength interval.
Fig. 2 is the structural representation of the multi-wavelength optical fiber laser at single times of Brillouin shift interval.
Fig. 3 is the structural representation of the multi-wavelength optical fiber laser of double Brillouin frequency shift interval.
Fig. 4 is the output spectrum figure of the multi-wavelength optical fiber laser at single times of Brillouin shift interval.
Fig. 5 is the output spectrum figure of the multi-wavelength optical fiber laser of double Brillouin frequency shift interval
Fig. 6 is the output spectrum figure of the multi-wavelength optical fiber laser at three times of Brillouin shift intervals
Fig. 7 is single times, double and three times of laser output spectrum figure obtaining under identical pumping power condition.
Embodiment
Below in conjunction with accompanying drawing, the utility model is elaborated.
Embodiment 1
As shown in Figure 1, the tunable multi-wavelength optical fiber laser in the present embodiment wavelength interval comprises tunable light source 1, optical coupler 2, first light wavelength division multiplexing 3-1, the first pump laser 4-1, Er-doped fiber 5-1, the first optical circulator 6-1, the first optical circulator 6-2, monomode fiber 7-1, four-port photocirculator 8, Er-doped fiber 5-2, monomode fiber 7-2, Second Wave division multiplexer 3-2, the second pumping source 4-2 and spectrometer 9, and the gain ranging of Er-doped fiber 5-1,5-2 is 1530nm to 1570nm.The working range of optical coupler 2 is 1530nm to 1580nm, and the port d of optical coupler 2 is as Laser output port.
The present embodiment is the multi-wavelength optical fiber laser at three times of Brillouin shift intervals, the connected mode of each device is: the first port a of tunable light source 1 and optical coupler 2 is by Fiber connection, and the port e of the first wave division multiplexer 3-1 in the 3rd port c of optical coupler 2 and linear cavity one passes through Fiber connection; The n port of the optical circulator 8 in the port j of the first optical circulator 6-1 in linear cavity one and annular chamber two passes through Fiber connection; The q port of the four-port photocirculator 8 in the second port b of optical coupler 2 and annular chamber two passes through Fiber connection.
Device connected mode in linear cavity one: the g port of the first light wavelength division multiplexing 3-1 is connected with one end of the first Er-doped fiber 5-1, the port f of the first light wavelength division multiplexing 3-1 and the first pump laser 4-1 is by Fiber connection, and the other end of the first Er-doped fiber 5-1 connects the port h of the first optical circulator 6-1; The port i of the first optical circulator 6-1 is connected with one end of the first monomode fiber 7-1, and the other end of the first monomode fiber 7-1 connects the port k of the second optical circulator 6-2, and port l and the m of the second optical circulator 6-2 passes through Fiber connection.
Device connected mode in annular chamber two: the o port of four-port photocirculator 8 connects one end of the second monomode fiber 7-2, the other end of the second monomode fiber 7-2 connects Er-doped fiber 5-2, the other end of the second Er-doped fiber 5-2 connects the port r of the second light wavelength division multiplexing 3-2, and port s and the second pump laser 4-2 of the second light wavelength division multiplexing 3-2 pass through Fiber connection; The port t of the second light wavelength division multiplexing 3-2 and the p port of four-port photocirculator 8 pass through Fiber connection.
4th port d and the spectrometer 9 of optical coupler 2 pass through Fiber connection, as the output port of laser.
Embodiment 2
As shown in Figure 2, the present embodiment is the multi-wavelength optical fiber laser at single times of Brillouin shift interval, the connected mode of each device is: tunable light source 1 passes through Fiber connection with the first port a of optical coupler 2,3rd port c of optical coupler 2 and the e port of first wave division multiplexer 3-1 are by Fiber connection, and the second port b of the optical coupler 2 and port j of the first optical circulator 6-1 passes through Fiber connection; The g port of the first light wavelength division multiplexing 3-1 is connected with one end of the first Er-doped fiber 5-1, the port f of the first light wavelength division multiplexing 3-1 and the first pump laser 4-1 is by Fiber connection, and the other end of the first Er-doped fiber 5-1 connects the port h of the first optical circulator 6-1; The port i of the first optical circulator 6-1 is connected with one end of the first monomode fiber 7-1, and the other end of the first monomode fiber 7-1 connects the port k of the second optical circulator 6-2, and port l and the m of the second optical circulator 6-2 passes through Fiber connection; 4th port d and the spectrometer 9 of optical coupler 2 pass through Fiber connection, as the output port of laser.
Embodiment 3
As shown in Figure 3, the present embodiment is the multi-wavelength optical fiber laser of double Brillouin frequency shift interval, the connected mode of each device is: tunable light source 1 passes through Fiber connection with the first port a of optical coupler 2, 3rd port c of optical coupler 2 and the n port of four-port photocirculator 8 pass through Fiber connection, second port b of optical coupler 2 and the q port of four-port photocirculator 8 pass through Fiber connection, the o port of four-port photocirculator 8 connects one end of the second monomode fiber 7-2, the other end of the second monomode fiber 7-2 connects Er-doped fiber 5-2, the other end of the second Er-doped fiber 5-2 connects the port r of the second light wavelength division multiplexing 3-2, port s and the second pump laser 4-2 of the second light wavelength division multiplexing 3-2 pass through Fiber connection, the port t of the second light wavelength division multiplexing 3-2 and the p port of four-port photocirculator 8 pass through Fiber connection, 4th port d and the spectrometer 9 of optical coupler 2 pass through Fiber connection, as the output port of laser.
The utility model can obtain stable single doubly, multiwavelength laser that is double and three times of Brillouin shift intervals exports, the power output of its multi-wavelength is subject to the control such as Output optical power, length of ring cavity of tunable light source and pumping, along with the development of various photoelectric device, will obtain more stable output, and its application also will be more extensive.
Above preferred embodiment of the present utility model and principle are described in detail; for those of ordinary skill in the art; according to the thought that the utility model provides, embodiment will change, and these changes also should be considered as protection range of the present utility model.
Claims (9)
1. a multi-wavelength optical fiber laser, it is characterized in that comprising tunable light source (1), optical coupler (2) and spectrometer (9), tunable light source (1) passes through Fiber connection with the first port (a) of optical coupler (2), 3rd port (c) of optical coupler (2) is by linear cavity one or annular chamber two or linear cavity one and annular chamber two is rear and the second port (b) Fiber connection, and the 4th port (d) and the spectrometer (9) of optical coupler (2) pass through Fiber connection.
2. multi-wavelength optical fiber laser as claimed in claim 1, it is characterized in that: described linear cavity one comprises first wave division multiplexer (3-1), first pump laser (4-1), first Er-doped fiber (5-1), first optical circulator (6-1), first monomode fiber (7-1), second optical circulator (6-2), 3rd port (c) of optical coupler (2) and the first port (e) of the first light wavelength division multiplexing (3-1) pass through Fiber connection, second port (f) and first pump laser (4-1) of first wave division multiplexer (3-1) pass through Fiber connection, 3rd port (g) of first wave division multiplexer (3-1) is connected with Er-doped fiber (5-1), the other end of Er-doped fiber (5-1) connects the first port (h) of the first optical circulator (6-1), second port (i) of the first optical circulator (6-1) is connected with the first monomode fiber (7-1), the other end of the first monomode fiber (7-1) connects the first port (k) of the second optical circulator (6-2), and the second port (l) and the 3rd port (m) of the second optical circulator (7-2) pass through Fiber connection, 3rd port (j) of the first optical circulator (6-1) and the second port (b) of optical coupler (2) pass through Fiber connection.
3. multi-wavelength optical fiber laser as claimed in claim 1, it is characterized in that: described annular chamber two comprises four-port photocirculator (8), second monomode fiber (7-2), second Er-doped fiber (5-2), Second Wave division multiplexer (3-2), second pump laser (4-2), 3rd port (c) of optical coupler (2) and the first port (n) of four-port photocirculator (8) pass through Fiber connection, second port (o) of four-port photocirculator (8) connects one end of the second monomode fiber (7-2), the other end of the second monomode fiber (7-2) connects one end of Er-doped fiber (5-2), the other end of Er-doped fiber (5-2) connects the first port (r) of the second light wavelength division multiplexing (3-2), second port (s) of the second light wavelength division multiplexing (3-2) is by Fiber connection second pump laser (4-2), 3rd port (t) of the second light wavelength division multiplexing (3-2) is by the 3rd port (p) of Fiber connection four-port photocirculator (8), 4th port (q) of four-port photocirculator (8) and the second port (b) of optical coupler (2) pass through Fiber connection.
4. multi-wavelength optical fiber laser as claimed in claim 1, is characterized in that: described linear cavity one comprises first wave division multiplexer (3-1), the first pump laser (4-1), the first Er-doped fiber (5-1), the first optical circulator (6-1), the first monomode fiber (7-1), the second optical circulator (6-2), described annular chamber two comprises four-port photocirculator (8), the second monomode fiber (7-2), the second Er-doped fiber (5-2), Second Wave division multiplexer (3-2), the second pump laser (4-2), 3rd port (c) of optical coupler (2) and the first port (e) of the first light wavelength division multiplexing (3-1) are by Fiber connection, and the second port (f) and first pump laser (4-1) of first wave division multiplexer (3-1) pass through Fiber connection, 3rd port (g) of first wave division multiplexer (3-1) is connected with Er-doped fiber (5-1), the other end of Er-doped fiber (5-1) connects the first port (h) of the first optical circulator (6-1), second port (i) of the first optical circulator (6-1) is connected with the first monomode fiber (7-1), the other end of the first monomode fiber (7-1) connects the first port (k) of the second optical circulator (6-2), and the second port (l) and the 3rd port (m) of the second optical circulator (7-2) pass through Fiber connection, 3rd port (j) of the first optical circulator (6-1) and the first port (n) of four-port photocirculator (8) pass through Fiber connection, second port (o) of four-port photocirculator (8) connects one end of monomode fiber (7-2), the other end of monomode fiber (7-2) connects one end of Er-doped fiber (5-2), the other end of Er-doped fiber (5-2) connects the first port (r) of the second light wavelength division multiplexing (3-2), second port (s) of the second light wavelength division multiplexing (3-2) is by Fiber connection second pump laser (4-2), 3rd port (t) of the second light wavelength division multiplexing (3-2) is by the 3rd port (p) of Fiber connection four-port photocirculator (8), 4th port (q) of four-port photocirculator (8) and the second port (b) of optical coupler (2) pass through Fiber connection.
5. the multi-wavelength optical fiber laser as described in claim 2 or 4, is characterized in that: the gain ranging of described the first Er-doped fiber (5-1) is 1530nm to 1570nm.
6. the multi-wavelength optical fiber laser as described in claim 3 or 4, is characterized in that: the gain ranging of described the second Er-doped fiber (5-2) is 1530nm to 1570nm.
7. the multi-wavelength optical fiber laser as described in claim 2 or 4, is characterized in that: the first monomode fiber (7-1) choice criteria silica fiber, fiber lengths is 25km.
8. the multi-wavelength optical fiber laser as described in claim 3 or 4, is characterized in that: the second monomode fiber (7-2) choice criteria silica fiber, fiber lengths is 25km.
9. the multi-wavelength optical fiber laser as described in any one of claim 1-4, is characterized in that: the 3rd port of optical coupler (2) is 90% port, and the 4th port is 10% port.
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| Application Number | Priority Date | Filing Date | Title |
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| CN201520575091.1U CN204835194U (en) | 2015-08-03 | 2015-08-03 | Multi -wavelength fiber laser |
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| CN201520575091.1U CN204835194U (en) | 2015-08-03 | 2015-08-03 | Multi -wavelength fiber laser |
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| CN204835194U true CN204835194U (en) | 2015-12-02 |
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Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN105048260A (en) * | 2015-08-03 | 2015-11-11 | 杭州电子科技大学 | Multi-wavelength fiber laser with tunable wavelength intervals |
| CN111834879A (en) * | 2020-07-20 | 2020-10-27 | 桂林电子科技大学 | Multi-wavelength Brillouin fiber laser |
| CN111834881A (en) * | 2020-07-20 | 2020-10-27 | 桂林电子科技大学 | Optical generation device for microwave signals |
| CN111834880A (en) * | 2020-07-20 | 2020-10-27 | 桂林电子科技大学 | Device for optically generating microwave signal |
-
2015
- 2015-08-03 CN CN201520575091.1U patent/CN204835194U/en not_active Withdrawn - After Issue
Cited By (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN105048260A (en) * | 2015-08-03 | 2015-11-11 | 杭州电子科技大学 | Multi-wavelength fiber laser with tunable wavelength intervals |
| CN105048260B (en) * | 2015-08-03 | 2018-05-29 | 杭州电子科技大学 | The multi-wavelength optical fiber laser that wavelength interval is tunable |
| CN111834879A (en) * | 2020-07-20 | 2020-10-27 | 桂林电子科技大学 | Multi-wavelength Brillouin fiber laser |
| CN111834881A (en) * | 2020-07-20 | 2020-10-27 | 桂林电子科技大学 | Optical generation device for microwave signals |
| CN111834880A (en) * | 2020-07-20 | 2020-10-27 | 桂林电子科技大学 | Device for optically generating microwave signal |
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