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l(f)r(sh)g2018-09-08 13:01
ժҪģ-ģw,ڌ·ģ(zhn)ģwݔһ·ģw,ȫwɺϳɼg(sh)еP(gun)IĿǰ,(du)چģ-ģwоmȻȡһM(jn)չ,Ќ(du)ڹںеľwݔ^ԼO(sh)Ӌ(j)Ҏ(gu)ɵȷоԷdzޡ,ᘌ(du)׹ܷĆģ-ģw,31ģ-ģw,Ăݔչ_(sh)ֵо,еĂݔ^,оݔݔw(sh)F(sh)(du)ܵӰ,oģ-ģwO(sh)Ӌ(j)Ҏ(gu)Ҫ:,BˆθFwՓ׺ιW(xu)͹ݔՓķքeo˃ɷNՓ˼·㷨(sh)F(xin),Y(ji)φģ-ģwc(din)ͽY(ji)(gu),(du)˃ɷNIJm÷,ָоģ-ģwĂݔҪʹùݔ,ᘌ(du)ʯӢ׹(c)ƺr,˟oްӔ(sh)ֵģ,о˹ںеݻ^̺Ҏ(gu),ӑՓ˺Y(ji)(gu)(sh)(du)ݔЧʵӰ푡Y(ji),ݔwĔ(sh)ֵ׏(du)ڂݔЧʵӰ^С;ݔwwоFLȑ(yng)ԓԱCݔЧ,ҪƥFȺݔwwоֱ,ʹݔwwоMС,ԫ@^õĹ|(zh)ݔ,ᘌ(du)õʓ׹(Сڰ)ƺr,ްӔ(sh)ֵģ,оްӼҪ(sh)(du)ܵӰY(ji):һ,ڵⲿ|(zh)Ĵ,ʹްڼsͷxҪ,˺FȺ͂ݔЧ;ڶ,ݔwԱֆģݔ,ʹݔwwо(sh)ֵ׏h(yun)СFwӔ(sh)ֵ׏r,Ȼ˸߂ݔЧ,˿ͨ^pСݔwwо(sh)ֵ׏ķʽݔ;,Fwеēp,ݔЧʵһ(g)Oֵ,ԓֵSFpС;,FLȑ(yng)LԝM^Fl,(sh)ֵģMY(ji)@ʾ^FLSF,ݔwwо(sh)ֵ׏wоӱߺݔЧϽY(ji)Փ(du)ģ-ģwO(sh)Ӌ(j)Ҫָ(do)x
[Abstract]:Single-mode and multi-mode fiber beam synthesizer is a key component in all optical fiber incoherent synthesis technology, which is used to output multiple single mode or quasi single mode fiber laser beam to a single mode fiber. At present, although some progress has been made in the study of single-mode and multi-mode optical fiber beam combiners, the research on the specific transmission process of light field in the beam combiner and the design rules of beam combiner are still very limited. Therefore, in this paper, for the single mode multimode fiber bundle combiner fabricated by casing method, taking 3 × 1 single mode multimode fiber bundle combiner as an example, a numerical study is carried out from the transmission characteristics, the transmission process of the light field in it is analyzed and the input is studied. The influence of the output fiber parameters and the tapered parameters on the performance of the buncher is discussed. The design rule of the single-mode and multi-mode fiber bundle combiner is given. The main work is as follows: firstly, the theoretical analysis methods of single tapered fiber, geometric optics method and beam propagation method, are introduced. In this paper, the theoretical thinking and algorithm realization of the two methods are given, and the differences and application range of the two methods are analyzed and compared by combining the characteristics and structure of the single-mode and multi-mode fiber beam combiner. It is pointed out that the beam propagation method is needed to study the propagation characteristics of single-mode multimode optical fiber combiner. Secondly, an infinite cladding numerical model is established to study the evolution process and law of the light field in the beam combiner, aiming at the case that the quartz casing (the refractive index is equal to the cladding index) is used to fabricate the beam holder, and the infinite cladding numerical model is established. The influence of the structure and parameters of the beam combiner on the transmission efficiency is discussed. The results show that the numerical aperture of the output fiber has little effect on the transmission efficiency, and the core and tapered length of the output fiber should be large enough to ensure the transmission efficiency. In addition, it is necessary to match the tapered ratio and the diameter of the output fiber core to make the output fiber core as small as possible in order to obtain better beam quality output. Finally, a finite cladding numerical model is established to study the influence of the limited cladding and other main parameters on the performance of the beam binder by using a low refractive index fluoride-doped casing (refractive index less than the cladding index). The results show that: first, due to the existence of the external medium with low refractive index, the limited cladding plays an important role in restraining and separating the light field, and improves the tapered ratio and transmission efficiency of the beam combiner. The optical field still maintains a single mode transmission in the input fiber cladding, which makes the beam combiner maintain a high transmission efficiency when the output fiber core numerical aperture is much smaller than the melt tapered fiber cladding numerical aperture. Therefore, the output brightness can be improved by reducing the numerical aperture of the output fiber core. Thirdly, due to the loss in the fused tapered fiber bundle, there exists a limit value for the increase of the transmission efficiency of the beam combiner, which decreases with the increase of the tapered ratio. Fourthly, the tapered length should be long enough to satisfy the adiabatic cone condition. The numerical simulation results show that the adiabatic cone length increases with the increase of the tapered ratio. In addition, increasing the input fiber core numerical aperture and the core-cladding ratio can improve the transmission efficiency of the beam combiner. The above conclusions are of great significance to the design of single-mode-multi-mode fiber beam combiner.
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