CN103825190B - The method and device of high-energy basic mode laser is exported based on stimulated Brillouin scattering technology in large core fiber - Google Patents
The method and device of high-energy basic mode laser is exported based on stimulated Brillouin scattering technology in large core fiber Download PDFInfo
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Abstract
基于受激布里渊散射技术在大芯径光纤中输出高能量基模激光的方法及装置,属于光学领域,本发明为解决大芯径光纤中输出高能量单基模激光存在泵浦利用率不高的问题。本发明方法为:空间激光被分束为泵浦光和种子光;泵浦光经耦合注入光纤环形器,并注入大芯径光纤;种子光经耦合注入单模光纤,对种子光进行相位调制,产生斯托克斯频移,形成调制后种子光;单模光纤和大芯径光纤中心对准熔接在一起,调制后种子光从单模光纤进入大芯芯径光纤,并与泵浦光相遇,在大芯径光纤中采用受激布里渊散射放大的方法将泵浦光拥有的高能量转入基模形态的种子光中,经受激布里渊散射后获取了高能量基模激光由光纤环形器输出。
A method and device for outputting high-energy fundamental-mode laser in a large-core-diameter optical fiber based on stimulated Brillouin scattering technology, which belongs to the field of optics. The present invention solves the problem of pump utilization in the output of high-energy single-mode laser in a large-core-diameter optical fiber. Not a high question. The method of the invention is as follows: the space laser beam is split into pumping light and seed light; the pumping light is coupled into a fiber circulator and injected into a large-core-diameter optical fiber; the seed light is coupled into a single-mode optical fiber to perform phase modulation on the seed light , resulting in a Stokes frequency shift to form the modulated seed light; the center of the single-mode fiber and the large-core fiber are aligned and fused together, and the modulated seed light enters the large-core fiber from the single-mode fiber and is combined with the pump light In the large-core fiber, the stimulated Brillouin scattering amplification method is used to transfer the high energy of the pump light into the seed light in the form of the fundamental mode, and the high-energy fundamental mode laser is obtained after the stimulated Brillouin scattering Output from fiber optic circulator.
Description
技术领域technical field
本发明涉及一种高能量基模激光输出方法,属于光学领域。The invention relates to a high-energy fundamental-mode laser output method, which belongs to the field of optics.
背景技术Background technique
光纤激光器拥有很多其它激光器难以比拟的优点,如:高输出功率、高泵浦转换效率、宽带增益、很好的横模稳定性和易于散热等,在现今的研究中可谓炙手可热。然而,由于光纤口径极小,故而常规光纤损伤阈值很低,且容易发生非线性效应,这使得光纤的输出功率受到极大限制。通过增大光纤芯径,可以有效克服这些问题,但增大光纤芯径又会使输出光束多模化,大幅降低光束质量。Fiber lasers have many advantages that are incomparable to other lasers, such as: high output power, high pump conversion efficiency, broadband gain, good transverse mode stability and easy heat dissipation, etc., which can be described as hot in today's research. However, due to the extremely small aperture of the fiber, the damage threshold of the conventional fiber is very low, and nonlinear effects are prone to occur, which greatly limits the output power of the fiber. These problems can be effectively overcome by increasing the core diameter of the fiber, but increasing the core diameter of the fiber will make the output beam multi-mode and greatly reduce the beam quality.
近二十年来,为了在大芯径光纤中得到单模输出光,目前已提出了诸多方案,但都各有缺陷。例如,上世纪末,双包层光纤因能提高输出能量且保持单基模输出光而得到了广泛研究和应用,但是,双包层光纤中信号光仍然只能在细小的纤芯中传输,已经不能满足现今光纤激光器高功率化的需求。有一种方法是通过弯曲光纤来过滤掉大芯径光纤中的高阶模式,从而获得较好的输出光束,但是这种方法会带来很多光损耗,不仅效率极低,还违背了光纤激光器高功率高能量化的主旨,难以应用。还有一种途径利用长周期光纤光栅在大芯径光纤中选择性的激发想要的传输模式,同时还可以通过光栅或全息板将传输光还原成基模光。这种方法虽然有效利用了大芯径光纤的场面积,却还没有提供放大技术,近期内还难以实现光纤激光器高能量化的需求。大模场区域光纤(LMA)能够在较大芯径光纤中输出单模激光,在近年也得到了广泛关注,但目前这种方法用的都只能做到几十微米量级芯径的光纤,在输出能量上依然受到了一定的限制。另外,南安普顿大学通过熔接拉锥的方法在百微米量级大芯径光纤中准确激发了基模光,十分吸引眼球。但在他们的方案中同样没有提供任何放大机制,目前其输出光束能量仍然只有普通单模光纤水平。In the past two decades, in order to obtain single-mode output light in large-core-diameter optical fibers, many schemes have been proposed, but each has its own defects. For example, at the end of last century, double-clad fiber has been widely researched and applied because it can increase the output energy and maintain a single fundamental mode output light. However, the signal light in double-clad fiber can only be transmitted in a small core, which has been It cannot meet the high power requirements of today's fiber lasers. There is a way to filter out the high-order modes in the large-core fiber by bending the fiber, so as to obtain a better output beam, but this method will bring a lot of optical loss, which is not only extremely inefficient, but also violates the high efficiency of fiber lasers. The main purpose of high power and energy is difficult to apply. There is also a way to selectively excite the desired transmission mode in a large-core fiber by using a long-period fiber grating, and at the same time, the transmitted light can be reduced to the fundamental mode light through the grating or holographic plate. Although this method effectively utilizes the field area of the large-core-diameter fiber, it has not yet provided amplification technology, and it is difficult to meet the demand for high-energy fiber lasers in the near future. The large mode area fiber (LMA) can output single-mode laser in a larger core diameter fiber, and it has also received extensive attention in recent years, but at present, this method can only be used for fibers with a core diameter of tens of microns. , the output energy is still limited to a certain extent. In addition, the University of Southampton accurately excited the fundamental mode light in a large-core-diameter optical fiber of the order of 100 microns by splicing the taper method, which is very eye-catching. However, no amplification mechanism is provided in their scheme, and the output beam energy is still only at the level of ordinary single-mode fiber.
总体来说,以往对于大芯径光纤中单基模激光输出的方法一般都只将光纤芯径提高到数十微米芯径量级,能够承受的激光能量还很有限,且泵浦利用率并不是很高,一般不超过80%。Generally speaking, the previous methods for single-mode laser output in large-core fibers generally only increase the core diameter of the fiber to the order of tens of microns, the laser energy that can be tolerated is still very limited, and the pump utilization rate is not high. Not very high, generally no more than 80%.
发明内容Contents of the invention
本发明目的是为了解决大芯径光纤中输出高能量单基模激光存在泵浦利用率不高的问题,提供了一种基于受激布里渊散射技术在大芯径光纤中输出高能量基模激光的方法及装置。The purpose of the present invention is to solve the problem of low pump utilization rate in outputting high-energy single fundamental mode laser in a large-core-diameter fiber, and provides a method based on stimulated Brillouin scattering technology to output high-energy fundamental-mode laser in a large-core-diameter fiber. Method and device for modulo laser.
本发明所述基于受激布里渊散射技术在大芯径光纤中输出高能量基模激光的方法,该方法为:The method for outputting high-energy fundamental-mode laser in a large-core-diameter optical fiber based on stimulated Brillouin scattering technology in the present invention, the method is:
空间激光被分束为泵浦光和种子光;The space laser is split into pump light and seed light;
泵浦光经耦合注入光纤环形器,并通过光纤环形器注入大芯径光纤;The pump light is coupled and injected into the fiber circulator, and injected into the large core diameter fiber through the fiber circulator;
种子光经耦合注入单模光纤,然后对注入的种子光进行相位调制,产生斯托克斯频移,形成调制后种子光;The seed light is coupled and injected into the single-mode fiber, and then the injected seed light is phase-modulated to generate a Stokes frequency shift to form the modulated seed light;
单模光纤和大芯径光纤中心对准,采用熔接法连接在一起,或熔接后再采用拉锥法进行处理;The single-mode fiber and the large-core fiber are centered and connected together by fusion splicing, or processed by tapering after fusion;
调制后种子光从单模光纤进入大芯芯径光纤,并与泵浦光相遇,在大芯径光纤中采用受激布里渊散射放大的方法将泵浦光拥有的高能量转入基模形态的种子光中,经受激布里渊散射后的光束由光纤环形器输出,获取了高能量基模激光。After modulation, the seed light enters the large-core fiber from the single-mode fiber and meets the pump light. In the large-core fiber, the high energy of the pump light is transferred into the fundamental mode by the method of stimulated Brillouin scattering amplification. In the seed light of the form, the beam after the stimulated Brillouin scattering is output by the fiber circulator, and the high-energy fundamental mode laser is obtained.
实现所述基于受激布里渊散射技术在大芯径光纤中输出高能量基模激光的方法的装置包括光源、分束镜、第一耦合器、第二耦合器、第一大芯径光纤、第一单模光纤、光纤环形器、第二大芯径光纤、第二单模光纤、相位调制器和反射镜;The device for realizing the method for outputting high-energy fundamental-mode laser in a large-core-diameter fiber based on stimulated Brillouin scattering technology includes a light source, a beam splitter, a first coupler, a second coupler, and a first large-core-diameter fiber , a first single-mode fiber, a fiber circulator, a second large core diameter fiber, a second single-mode fiber, a phase modulator and a mirror;
光源输出的空间光束入射至分束镜,经分束镜形成透射光束和反射光束;The spatial beam output by the light source is incident on the beam splitter, and the transmitted beam and reflected beam are formed by the beam splitter;
所述透射光束由第一耦合器耦合至第一大芯径光纤形成泵浦光,第一大芯径光纤输出的浦泵光注入光纤环形器的A口,浦泵光从光纤环形器的B口输出并入射至第二大芯径光纤中;The transmitted light beam is coupled to the first large-core fiber by the first coupler to form pump light, the pump light output by the first large-core fiber is injected into the A port of the fiber circulator, and the pump light is sent from the B port of the fiber circulator port output and incident into the second largest core diameter fiber;
所述反射光束入射至反射镜,由反射镜反射输出的光束经第二耦合器耦合至第一单模光纤形成种子光,所述种子光经相位调制器调制后输出,并进入第二单模光纤,调制后种子光注入第二大芯径光纤中;The reflected light beam is incident on the mirror, and the light beam reflected and output by the mirror is coupled to the first single-mode optical fiber through the second coupler to form seed light, and the seed light is output after being modulated by the phase modulator, and enters the second single-mode optical fiber. Optical fiber, the modulated seed light is injected into the second largest core diameter optical fiber;
调制后的种子光与浦泵光相遇,经布里渊散射放大后注入光纤环形器的B口,并由光纤环形器的C口输出。The modulated seed light meets the pump light, is amplified by Brillouin scattering, and then injected into port B of the fiber optic circulator, and output from port C of the fiber optic circulator.
本发明的优点:本发明提供了一种能在数百微米芯径光纤中得到基模输出激光方法,且输出稳定结构简单,转化效率极高,理论上泵浦利用率可达99%。对光纤激光器高功率化具有突破性意义。本发明方法不但使大芯径光纤输出激光能量高,而且,激发及输出光束稳定,重复性高,输出光束保证为基模光束。Advantages of the present invention: the present invention provides a method that can obtain fundamental mode output laser in optical fibers with a core diameter of hundreds of microns, and has a stable output structure, simple structure, high conversion efficiency, and theoretically, the pump utilization rate can reach 99%. It has a breakthrough significance for the high power of fiber laser. The method of the invention not only makes the output laser energy of the large-core-diameter optical fiber high, but also has stable excitation and output beams and high repeatability, and the output beams are guaranteed to be fundamental mode beams.
附图说明Description of drawings
图1是本发明所述基于受激布里渊散射技术在大芯径光纤中输出高能量基模激光装置的光路结构示意图;Fig. 1 is a schematic diagram of the optical path structure of a high-energy fundamental-mode laser device output in a large-core-diameter fiber based on the stimulated Brillouin scattering technology of the present invention;
图2是大芯径光纤与单模光纤对接图;Figure 2 is a diagram of the connection between a large-core fiber and a single-mode fiber;
图3是输出高能量基模激光的光斑图;Fig. 3 is the light spot pattern of output high-energy fundamental mode laser;
图4是入射的空间光束的波形图;Fig. 4 is the waveform diagram of the incident space light beam;
图5是输出高能量基模激光的波形图。Fig. 5 is a waveform diagram of outputting high-energy fundamental mode laser light.
具体实施方式detailed description
具体实施方式一:下面结合图1说明本实施方式,本实施方式所述基于受激布里渊散射技术在大芯径光纤中输出高能量基模激光的方法,使用与种子光有布里渊频差并反向传输的高能量泵浦光对基模种子光进行受激布里渊散射放大;在大芯径光纤中激发基模种子光的方法为:将大芯径光纤和单模光纤进行对心连接;具体方法为:Specific Embodiment 1: The present embodiment will be described below in conjunction with FIG. 1. The method for outputting high-energy fundamental-mode laser in a large-core-diameter fiber based on the stimulated Brillouin scattering technique described in this embodiment uses The high-energy pump light with frequency difference and reverse transmission performs stimulated Brillouin scattering amplification on the fundamental mode seed light; the method of exciting the fundamental mode seed light in the large-core fiber is as follows: the large-core fiber and the single-mode fiber Make a heart-to-heart connection; the specific method is:
空间激光被分束为泵浦光和种子光;The space laser is split into pump light and seed light;
泵浦光经耦合注入光纤环形器,并通过光纤环形器注入大芯径光纤;The pump light is coupled and injected into the fiber circulator, and injected into the large core diameter fiber through the fiber circulator;
种子光经耦合注入单模光纤,然后对注入的种子光进行相位调制,产生斯托克斯频移,形成调制后种子光;The seed light is coupled and injected into the single-mode fiber, and then the injected seed light is phase-modulated to generate a Stokes frequency shift to form the modulated seed light;
单模光纤和大芯径光纤中心对准,采用熔接法连接在一起,或熔接后再采用拉锥法进行处理;The single-mode fiber and the large-core fiber are centered and connected together by fusion splicing, or processed by tapering after fusion;
调制后种子光从单模光纤进入大芯芯径光纤,并与泵浦光相遇,在大芯径光纤中采用受激布里渊散射放大的方法将泵浦光拥有的高能量转入基模形态的种子光中,经受激布里渊散射后的光束由光纤环形器输出,获取了高能量基模激光。After modulation, the seed light enters the large-core fiber from the single-mode fiber and meets the pump light. In the large-core fiber, the high energy of the pump light is transferred into the fundamental mode by the method of stimulated Brillouin scattering amplification. In the seed light of the form, the beam after the stimulated Brillouin scattering is output by the fiber circulator, and the high-energy fundamental mode laser is obtained.
大芯径光纤为折射率渐变光纤,例如可以采用平方率渐变光纤。The large-core optical fiber is a graded-index fiber, for example, a graded-square-rate fiber can be used.
具体实施方式二:下面结合图2说明本实施方式,本实施方式对实施方式一作进一步说明,单模光纤和大芯径光纤中心对准,采用熔接法连接在一起;或熔接后再采用拉锥法进行处理;Specific embodiment 2: The present embodiment will be described below in conjunction with FIG. 2 . This embodiment will further explain Embodiment 1. The center of the single-mode optical fiber and the large-core-diameter optical fiber are aligned and connected together by fusion splicing; or after fusion splicing, tapered method for processing;
大芯径光纤为多模光纤,大芯径光纤的纤芯直径大于或等于100μm。当其包层直径与单模光纤直径相同时,采用对心熔接方法进行对接,连接处形成熔点12;如图2所示,二者包层直径相同,但二者的纤芯直径不同。The large-core fiber is a multimode fiber, and the core diameter of the large-core fiber is greater than or equal to 100 μm. When the diameter of the cladding is the same as that of the single-mode fiber, it is butted by center fusion splicing, and the melting point 12 is formed at the joint; as shown in Figure 2, the diameter of the cladding of the two is the same, but the diameter of the core of the two is different.
给出一个具体例子:二者包层直径均为125μm,大芯径光纤的纤芯直径为105μm,单模光纤的纤芯直径为8.3μm。单模光纤与大芯径光纤中心对准,并熔接成为一根光纤。A specific example is given: both cladding diameters are 125 μm, the core diameter of the large-core fiber is 105 μm, and the core diameter of the single-mode fiber is 8.3 μm. The single-mode fiber is centered with the large-core fiber and fused into one fiber.
如果多模光纤包层直径大于单模光纤的包层直径,则采用熔接拉锥的方法将两种光纤连接。If the cladding diameter of the multimode fiber is larger than that of the single-mode fiber, the two fibers are connected by fusion splicing and tapering.
具体实施方式三:下面结合图1至图5说明本实施方式,实现实施方式一所述基于受激布里渊散射技术在大芯径光纤中输出高能量基模激光的方法的装置,它包括光源1、分束镜2、第一耦合器3、第二耦合器4、第一大芯径光纤5、第一单模光纤6、光纤环形器7、第二大芯径光纤8、第二单模光纤9、相位调制器10和反射镜11;Specific Embodiment Three: The present embodiment will be described below in conjunction with FIGS. 1 to 5. The device for implementing the method for outputting high-energy fundamental-mode laser in a large-core-diameter optical fiber based on the stimulated Brillouin scattering technology described in Embodiment 1 includes: Light source 1, beam splitter 2, first coupler 3, second coupler 4, first large-core fiber 5, first single-mode fiber 6, fiber circulator 7, second large-core fiber 8, second Single-mode optical fiber 9, phase modulator 10 and mirror 11;
光源1输出的空间光束入射至分束镜2,经分束镜2形成透射光束和反射光束;The spatial beam output by the light source 1 is incident on the beam splitter 2, and the transmitted beam and the reflected beam are formed by the beam splitter 2;
所述透射光束由第一耦合器3耦合至第一大芯径光纤5形成泵浦光,第一大芯径光纤5输出的浦泵光注入光纤环形器7的A口,浦泵光从光纤环形器7的B口输出并入射至第二大芯径光纤8中;The transmitted light beam is coupled to the first large-core fiber 5 by the first coupler 3 to form pumping light, and the pumping light output by the first large-core fiber 5 is injected into the A port of the optical fiber circulator 7, and the pumping light is transmitted from the optical fiber The B port output of the circulator 7 is incident into the second large core diameter optical fiber 8;
所述反射光束入射至反射镜11,由反射镜11反射输出的光束经第二耦合器4耦合至第一单模光纤6形成种子光,所述种子光经相位调制器10调制后输出,并进入第二单模光纤9,调制后种子光注入第二大芯径光纤8中;The reflected light beam is incident on the mirror 11, and the light beam reflected and output by the mirror 11 is coupled to the first single-mode fiber 6 through the second coupler 4 to form a seed light, and the seed light is output after being modulated by the phase modulator 10, and Entering the second single-mode fiber 9, the modulated seed light is injected into the second large core diameter fiber 8;
调制后种子光与浦泵光发生布里渊散射后注入光纤环形器7的B口,并由光纤环形器7的C口输出。The modulated seed light and the pump light undergo Brillouin scattering and are injected into port B of the optical fiber circulator 7 and output from port C of the optical fiber circulator 7 .
光源1采用空间激光器。由于目前光纤激光器所能达到的能量有限,空间激光器能够提供较大的泵浦能量,所以使用空间激光器作为光源。被分成两束:泵浦光和种子光,二者的比例由分束镜2的分束比例决定。The light source 1 is a space laser. Due to the limited energy that fiber lasers can achieve at present, space lasers can provide greater pumping energy, so space lasers are used as light sources. It is divided into two beams: the pump light and the seed light, and the ratio of the two is determined by the beam splitting ratio of the beam splitter 2.
第一大芯径光纤5和第一单模光纤6的长度不需要太长,只需完成耦合光束传输即可。第二大芯径光纤8需要足够长,以保证种子光和泵浦光能够进行充分的“受激布里渊散射放大”。同时应控制两者光程,让泵浦光进入大芯径光纤后尽快与种子光相遇,以免泵浦光发生“受激布里渊散射产生”而不能将能量全部转移到种子光中。散射后的光束从光纤环形器7的B口入,C口出,端口C输出的大能量光束如果需要用作空间激光,可再用透镜将其转化为平行光束。如果作为光纤光可直接使用。The lengths of the first large-core-diameter optical fiber 5 and the first single-mode optical fiber 6 do not need to be too long, and only need to complete the coupling beam transmission. The second large core-diameter fiber 8 needs to be long enough to ensure that the seed light and the pump light can perform sufficient "stimulated Brillouin scattering amplification". At the same time, the optical paths of the two should be controlled so that the pump light meets the seed light as soon as possible after entering the large core diameter fiber, so as to prevent the pump light from being "produced by stimulated Brillouin scattering" and unable to transfer all the energy to the seed light. The scattered light beam enters from port B of the fiber optic circulator 7 and exits from port C. If the high-energy beam output from port C needs to be used as a space laser, it can be converted into a parallel beam by using a lens. If it is used as fiber optic light, it can be used directly.
放大后的单基模光仍然能保持良好的单基模状态,输出光束如图3所示。同时,放大后的激光保持了与种子光还几乎保持了相同的波形,如图4、图5所示。The amplified single fundamental mode light can still maintain a good single fundamental mode state, and the output beam is shown in Figure 3. At the same time, the amplified laser maintains almost the same waveform as the seed light, as shown in Figure 4 and Figure 5 .
在受激布里渊散射的机理中,泵浦能量越大,其转化效率越高。有人预测,当泵浦能量到达一定程度后,转化效率能达到99%。故而在此方案下,能量需求越大,泵浦利用率越高。一般来说,在已有的光纤放大器中,泵浦利用率很难超过80%。在我们已有的实验中,仅在一百微米光纤能承受的能量下,泵浦利用率已经超过90%,我们预计,大芯径光纤的引入和使用,可大幅提高光纤承受能量,并将输出能量和泵浦利用率提高到很大的程度。In the mechanism of stimulated Brillouin scattering, the greater the pump energy, the higher the conversion efficiency. Some people predict that when the pump energy reaches a certain level, the conversion efficiency can reach 99%. Therefore, under this scheme, the greater the energy demand, the higher the pump utilization rate. Generally speaking, in existing optical fiber amplifiers, the pump utilization rate is difficult to exceed 80%. In our existing experiments, the pump utilization rate has exceeded 90% only under the energy that a 100-micron fiber can bear. The output energy and pump utilization are improved to a great extent.
使用的图2所示的,二者中心对准后,采用熔接法连接在一起,其激发原理与芯径大小无关,理论上多大芯径的光纤都可以使用。我们至少可以拓展至几百微米芯径光纤,甚至几毫米芯径光纤,用以承受强大的泵浦光能量。所以,我们能够得到的输出光束能量和峰值功率都很高。我们预计,纳秒脉冲下,至少可获得几十毫焦耳的能量,皮秒脉冲下,至少可获得几十兆瓦的峰值功率。另外,我们使用的这种熔接法,一旦熔接点完成,以后每次输出光束都会保持同一状态。输出稳定且操作简单,十分具有应用价值和前景。As shown in Figure 2, after the centers of the two are aligned, they are connected together by fusion splicing. The excitation principle has nothing to do with the size of the core diameter. In theory, fibers with a large core diameter can be used. We can at least expand to a core diameter fiber of several hundred microns, or even a few millimeters core diameter fiber, to withstand the powerful pump light energy. Therefore, the output beam energy and peak power we can get are very high. We expect that at least tens of millijoules of energy can be obtained under nanosecond pulses, and at least tens of megawatts of peak power can be obtained under picosecond pulses. In addition, the welding method we use, once the welding point is completed, the output beam will maintain the same state every time in the future. The output is stable and the operation is simple, which has great application value and prospect.
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