Suppression of auto-resonant stimulated Brillouin scattering in supersonic flowing plasmas by different forms of incident lasers

In supersonic flowing plasmas,the auto-resonant behavior of ion acoustic waves driven by stimulated Brillouin backscattering is self-consistently investigated.A nature of absolute instability appears in the evolution of the stimulated Brillouin backscattering.By adopting certain form of incident lights combined by two perpendicular linear polarization lasers or polarization rotation lasers,the absolute instability is suppressed significantly.The suppression of auto-resonant stimulated Brillouin scattering is verified with the fully kinetic Vlasov code.

The Stimulated Brillouin Scattering of a Strong Laser in Partially Stripped Plasmas

The effects of the nonlinear polarization in a partially stripped plasma on stimulated Brillouin scattering (SBS) process of a strong laser are discussed. A set of nonlineax mode coupling equations and the linear growth rate of SBS instability is derived, respectively. When the intensity of an incident laser Io > 10^(17) W/cm^2, the third order susceptibility X(3) will reduce the above mentioned linear growth rate enormously. If taking the maximum value of the second order susceptibility X(2), the growth rate may be decreased observably when Io > 10_^(14)W/cm2. Furthermore, the nonlinear susceptibility can affect the nonlinear evolution of SBS much extensively.

Suppression of stimulated Brillouin and Raman scatterings using an alternating frequency laser and transverse magnetic fields

A novel scheme to suppress both stimulated Brillouin scattering(SBS) and stimulated Raman scattering(SRS) by combining an alternating frequency(AF) laser and a transverse magnetic field is proposed. The AF laser allows the laser frequency to change discretely and alternately over time. The suppression of SBS is significant as long as the AF difference is greater than the linear growth rate of SBS or the alternating time of the laser frequency is shorter than the linear growth time of SBS. However, the AF laser proves ineffective in suppressing SRS, which usually has a much higher linear growth rate than SBS. To remedy that, a transverse magnetic field is included to suppress the SRS instability. The electrons trapped in the electron plasma waves(EPWs) of SRS can be accelerated by the surfatron mechanism in a transverse magnetic field and eventually detrapped. While continuously extracting energy from EPWs, the EPWs are dissipated and the kinetic inflation of SRS is suppressed. The one-dimensional particle-in-cell simulation results show that both SBS and SRS can be effectively suppressed by combining the AF laser with a transverse magnetic field with tens of Tesla. The total reflectivity can be dramatically reduced by more than one order of magnitude. These results provide a potential reference for controlling SBS and SRS under the related parameters of inertial confinement fusion.

High-power free-running single-longitudinal-mode diamond Raman laser enabled by suppressing parasitic stimulated Brillouin scattering

A continuous-wave(CW)single-longitudinal-mode(SLM)Raman laser at 1240 nm with power of up to 20.6 W was demonstrated in a free-running diamond Raman oscillator without any axial-mode selection elements.The SLM operation was achieved due to the spatial-hole-burning free nature of Raman gain and was maintained at the highest available pump power by suppressing the parasitic stimulated Brillouin scattering(SBS).A folded-cavity design was employed for reducing the perturbing effect of resonances at the pump frequency.At a pump power of 69 W,the maximum Stokes output reached 20.6 W,corresponding to a 30%optical-to-optical conversion efficiency from 1064to 1240 nm.The result shows that parasitic SBS is the main physical process disturbing the SLM operation of Raman oscillator at higher power.In addition,for the first time,the spectral linewidth of a CW SLM diamond Raman laser was resolved using the long-delayed self-heterodyne interferometric method,which is 105 kHz at 20 W.

Broadband bidirectional Brillouin–Raman random fiber laser with ultra-narrow linewidth

We present a Brillouin–Raman random fiber laser(BRRFL)with full-open linear cavity structure to generate broadband Brillouin frequency comb(BFC)with double Brillouin-frequency-shift spacing.The incorporation of a regeneration portion consisting of an erbium-doped fiber and a single-mode fiber enables the generation of broadband BFC.The dynamics of broadband BFC generation changing with the pump power(EDF and Raman)and Brillouin pump(BP)wavelength are investigated in detail,respectively.Under suitable conditions,the bidirectional BRRFL proposed can produce a flatamplitude BFC with 40.7-nm bandwidth ranging from 1531 nm to 1571.7 nm,and built-in 242-order Brillouin Stokes lines(BSLs)with double Brillouin-frequency-shift spacing.Moreover,the linewidth of single BSL is experimentally measured to be about 2.5 kHz.The broadband bidirectional narrow-linewidth BRRFL has great potential applications in optical communication,optical sensing,spectral measurement,and so on.

Stimulated Brillouin scattering evolution and suppression in an integrated stimulated thermal Rayleigh scattering-based fiber laser

The spectral purity of fiber lasers has become a critical issue in both optical sensing and communication fields.As a result of ultra-narrow intrinsic linewidth, stimulated thermal Rayleigh scattering(STRS) has presented special potential to compress the linewidth of fiber lasers. To suppress stimulated Brillouin scattering(SBS), the most dominant disturbance for STRS in optical fibers, a semi-quantitative estimation has been established to illuminate the mechanism of suppressing SBS in a periodic tapered fiber, and it agrees with experimental results. Finally, a linewidth compression device based on STRS is integrated into a single-longitudinal-mode ring-cavity fiber laser with secondary cavities, and its linewidth is verified to be 200 Hz through a self-heterodyne detecting and Voigt fitting method.

Amplification of 200-ps high-intensity laser pulses via frequency matching stimulated Brillouin scattering

Laser pulses of 200 ps with extremely high intensities and high energies are sufficient to satisfy the demand of shock ignition,which is an alternative path to ignition in inertial confinement fusion(ICF).This paper reports a type of Brillouin scheme to obtain high-intensity 200-ps laser pulses,where the pulse durations are a challenge for conventional pulsed laser amplification systems.In the amplification process,excited Brillouin acoustic waves fulfill the nonlinear optical effect through which the high energy of a long pump pulse is entirely transferred to a 200-ps laser pulse.This method was introduced and achieved within the SG-Ⅲprototype system in China.Compared favorably with the intensity of 2 GW/cm^2 in existing ICF laser drivers,a 6.96-GW/cm^2 pulse with a width of 170 ps was obtained in our experiment.The practical scalability of the results to larger ICF laser drivers is discussed.

Output characteristics of high-power stimulated Brillouin scattering pulse compression enhanced by thermal effects based on HT270

Thermal effects are typically considered as obstacles to high-repetition-rate stimulated Brillouin scattering(SBS)pulse compression.In this paper,a novel method is proposed for improving the SBS output characteristics by exploiting thermal effects on the liquid medium.Using HT270,the SBS output parameters with the medium purification and rotating off-centered lens methods are studied at different repetition rates.The results indicate that these two methods can alleviate thermal effects and improve the energy efficiency,but the rotating method reduces the energy stability because of the aggravated optical breakdown at the kilohertz-level repetition rate.For a 35-mJ pump energy,the energy efficiency at 2 kHz without the rotating method is 30%higher than that at 100 Hz and 70%higher than that at 500 Hz.The enhancement of the SBS output characteristics by thermal effects is demonstrated theoretically and experimentally,and 2-kHz high-power SBS pulsecompression is achieved with HT270.

Photonic crystal fibre Brillouin laser based on Bragg grating Fabry-Perot cavity

A photonic crystal fibre Brillouin laser based on fibre Bragg grating Fabr-Perot cavity is presented. A highly nonlinear photonic crystal fibre 25 m in length is used as Brillouin gain medium and fibre Bragg grating Fabry-Perot cavity is chosen in order to enhance the laser conversion efficiency and suppress the higher-order Stokes waves. The laser reaches the threshold at input power of 35 mW, and the experimental laser conversion efficiency achieves 18% of the input power of 140 mW and does not show higher-order Stokes waves. A photonic crystal fibre Brillouin laser with shorter fibre length and lower threshold is experimentally realized.

Spacing-adjustable and wavelength-tunable multiwavelength fibre laser with nonlinear Brillouin gain and birefringence fibre loop mirror

This paper demonstrates a room-temperature multiwavelength fibre laser with spacing-adjustability and wavelength-tunability. The nonlinear gain of self-excited stimulated Brillouin scattering can suppress mode competition induced by homogeneous broadening of Erbium-doped fibre. With the use of a birefringence fibre loop filter, the wavelength spacing can be adjusted by changing the length of the used birefringence fibre, and the lasing wavelengths can be finely tuned through modifying the filtering profile of the birefringence filter. Multiwavelength output with spectral spacing as small as 0.076 nm and a wavelength number of more than 80 has been successfully produced.

A low-threshold multiwavelength Brillouin fiber laser with double-frequency spacing based on a small-core fiber

We demonstrate multiwavelength Brillouin fiber lasers(MWBFLs)with double-frequency spacing based on a small-core fiber(SCF)and a standard single-mode fiber(SMF),which have core diameters of 5 and 8.8μm,respectively.Experimental results show that the SCF-based MWBFL exhibits a higher laser output power and a lower pump threshold.The output powers of the SCF-based MWBFL are>1.4 times those of the SMF-based MWBFL.Moreover,the threshold power required to generate each channel of the SCF-based MWBFL is 59%that of the SMF-based MWBFL.When the same pump power of 180 mW is injected,the number of laser channels generated for the SCF-based MWBFL is 13,which is twice that generated for the SMF-based MWBFL.In addition,the SCF-based MWBFL exhibits good wavelength tunability from 1535 to 1565 nm and temporal stability over an hour.

Laser-induced damage on large-aperture fused silica gratings

Two sets of laser-damage experiments on large-aperture fused silica optics have been carried out in a high-power laser facility. Severe damage has been found on the grating which presented dense craters on the front surface. This phenomenon is quite different from other fused silica optics, which are damaged on the rear surface. The damage possibility due to the redeposition layer was ruled out by acid-etching the grating＇s front surface. The remarkable stimulated Brillouin scattering （SBS） effect was observed in grating and the reason for the front surface damage is thought to be the backward SBS.

Brillouin gain spectrum characterization in Ge-doped large-mode-area fibers

The dependence of Brillouin gain spectrum(BGS)characteristics,including the Brillouin frequency shift(BFS)and the BGS bandwidth,on germanium concentration in large-mode-area Ge-doped passive fibers is investigated theoretically and experimentally.The simulation results show that the BFS is inversely proportional to GeO_(2)concentration,and the BGS bandwidth initially increases with the augment of GeO_(2)concentration,and then decreases.The BGSs of four fibers with core diameters of 10μm and 20μm for different GeO_(2)concentrations are compared experimentally.Experimental results demonstrate that with the same core diameter,the variations of BFS and BGS bandwidths with GeO_(2)concentration accord with the simulation results.Additionally,the BGS characteristics of three large-mode-area passive fibers with diameters of 10μm,25μm,and 30μm are measured,which confirm that the increasing of the fiber diameters will cause the BGS bandwidth to broaden.We believe that these results can provide valuable references for modulating the high-power narrowlinewidth fiber lasers and Brillouin fiber amplifiers.

Long-Pulse Single-Frequency All-Fiber Amplifier

In this paper, we report a high power long-pulse single-frequency all-fiber amplifier at 1064 nm with near-diffraction-limited beam quality based on a polarization-maintaining tapered Yb-doped fiber (T-YDF). By applying square wave pulse modulation to the diodes, with a frequency of 50 Hz and a pulse width of 668 μs, the peak power of the output laser reached 257 W with an average power of 8.65 W, linewidth of 10.6 kHz and M2 < 1.5. .

Linewidth narrowing in free-space-running diamond Brillouin lasers

This study analyzes the linewidth narrowing characteristics of free-space-running Brillouin lasers and investigates the approaches to achieve linewidth compression and power enhancement simultaneously.The results show that the Stokes linewidth behavior in a free-space-running Brillouin laser cavity is determined by the phase diffusion of the pump and the technical noise of the system.Experimentally,a Stokes light output with a power of 22.5 W and a linewidth of 3.2 kHz was obtained at a coupling mirror reflectivity of 96%,which is nearly 2.5 times compressed compared with the linewidth of the pump(7.36 kHz).In addition,the theorical analysis shows that at a pump power of 60Wand a coupling mirror reflectivity of 96%,a Stokes output with a linewidth of 1.6 kHz and up to 80%optical conversion efficiency can be achieved by reducing the insertion loss of the intracavity.This study provides a promising technical route to achieve high-power ultra-narrow linewidth special wavelength laser radiations.

宽带激光辐照平面薄膜靶的近前向散射

激光等离子体相互作用(LPI)过程一直以来是惯性约束聚变(ICF)点火中重要的研究内容,宽带激光在理论上一直以来被认为具有抑制LPI的潜力.宽带二倍频激光装置——“昆吾”,为实验研究宽带激光LPI效果提供了可靠的实验研究平台.针对大尺度低密度等离子体的LPI过程中强烈的受激布里渊散射和受激拉曼散射信号,开展了相同条件下宽带和窄带激光驱动C_(8)H_(8)平面薄膜靶的透过激光、前向散射和大角度近前向散射的实验研究.主要针对宽带和窄带激光前向透过信号的组分和近前向散射的光谱及份额信息进行对比研究,发现宽带和窄带激光驱动的LPI过程具有显著差异.同时,初步结果显示宽带激光相比于窄带激光体现出更强的穿透能力,烧蚀靶并穿过等离子体的时间提前了近1 ns,透过能量提升了近10倍,穿透等离子体后有更小的空间发散角.这些结果对于更好地理解宽带激光对于LPI的作用效果具有很好的参考价值.

激光等离子体的受激Brillouin散射

研究了激光等离子体背向和侧向受激 Brillouin散射光谱结构。激光等离子体相互作用时 ,受激 Brillouin散射光谱受激光等离子体状态的影响而产生 Doppler效应。当激光以 4 5°入射不同材料的平面靶时 ,等离子体运动产生不同的二维效应 ,高 Z材料产生的等离子体冕区主要沿靶法向运动 ,受激 Brillouin散射光谱在侧向产生较大蓝移 ,而低 Z材料则主要在激光入射方向产生较大蓝移。

Single-frequency upconverted laser generation by phase summation

The phase summation effect in sum-frequency mixing process is utilized to avoid a nonlinearity obstacle in the power scaling of single-frequency visible or ultraviolet lasers.Two single-frequency fundamental lasers are spectrally broadened by phase modulation to suppress stimulated Brillouin scattering in fiber amplifier and achieve higher power.After sum-frequency mixing in a nonlinear optical crystal,the upconverted laser returns to single frequency due to phase summation,when the phase modulations on two fundamental lasers have a similar amplitude but opposite sign.The method was experimentally proved in a Raman fiber amplifier-based laser system,which generated a power-scalable sideband-free single-frequency 590 nm laser.The proposal manifests the importance of phase operation in wave-mixing processes for precision laser technology.

非线性光学激光合束技术研究进展

回顾了非线性光学激光合束技术的发展历程,阐述了基于光学相位共轭和基于非线性放大过程的合束思想和基本原理,梳理了重叠耦合、种子注入和布里渊四波混频增强相位锁定激光合束方式的标志性成果,总结了等离子体交叉光束能量转移、金刚石拉曼放大和液体布里渊放大激光合束技术的优势和瓶颈。面向高峰值功率、高平均功率、高重复频率激光输出的实现需求,基于布里渊放大激光合束技术具备系统结构简单、功率负载高且散热效率高的优点,提出了实现单脉冲能量100 J、脉冲宽度10 ns、重复频率10 Hz合束激光输出的可行性方案。

All-optical carrier recovery for self-homodyne detection via injection locked Brillouin laser in whispering-gallery-mode microcavity

We demonstrate comprehensive investigation of the injection locking dynamics of a backscattered Brillouin laser in silica whispering-gallery-mode microcavity. Via injection locking, the Brillouin laser acquires highly correlated phase with the seed laser, enabling ultra-narrow bandwidth, high gain, and coherent optical amplification. Also, for the first time,to the best of our knowledge, the injection locked Brillouin laser is utilized to implement all-optical carrier recovery from coherent optical data signals. We show that by using the injection locked Brillouin laser as a local oscillator for self-homodyne detection, high-quality data receiving can be realized, even without traditional electrical compensations for carrier frequency and phase drifts.