【摘 要】
:
In this article, we report on an experimentally generated soliton and bound-state soliton passively mode-locked erbium-doped fiber laser by incorporating a saturable absorber (SA) made of MoS2/fluorine mica (FM) that was fabricated with the Langmuir–Blodg
【机 构】
:
SchoolofPhysicsandInformationTechnology,ShaanxiNormalUniversity,Xi’an710119,ChinaSchoolofScience,Xi’
【出 处】
:
PhotonicsResearch
论文部分内容阅读
In this article, we report on an experimentally generated soliton and bound-state soliton passively mode-locked erbium-doped fiber laser by incorporating a saturable absorber (SA) made of MoS2/fluorine mica (FM) that was fabricated with the Langmuir–Blodgett (LB) method. The FM substrate is 20 μm thick and easy to bend or cut, like a polymer. However, it has a higher damage threshold and a better thermal dissipation than polymers. In addition, the LB method can be used to fabricate a thin film with good uniformity. In this study, the modulation depth, saturable intensity, and unsaturated loss of the SA are measured as 5.9%, 57.69 MW/cm2, and 13.4%, respectively. Based on the SA, a soliton mode-locked laser is achieved. The pulse duration, repetition rate, and signal-to-noise ratio are 581 fs, 15.67 MHz, and 65 dB, respectively. By adjusting the polarization controller and pump power, we obtain a bound-state soliton mode-locked pulse. The temporal interval between the two solitons forming the bound-state pulse is 2.7 ps. The repetition rate of the bound-state pulses is proportional to the pump power. The maximum repetition rate is 517 MHz, corresponding to the 33rd harmonic of the fundamental repetition rate. The results indicate that the MoS2/FM LB film absorber is a promising photonic device in ultrafast fiber lasers.
其他文献
Metasurfaces have been used to realize optical functions such as focusing and beam steering. They use subwavelength nanostructures to control the local amplitude and phase of light. Here we show that such control could also enable a new function of artifi
Wired local network is used widely in a vehicle. It brings the benefits of sharing information and controlling automatically as well as causes negative reaction and a troublesome problem to vehicle such as weight, cost, electromagnetism and space and so o
In this paper, we present a detailed comparison of applying three advanced modulation formats including carrierless amplitude and phase modulation (CAP), orthogonal frequency division multiplexing (OFDM), and discrete Fourier transform spread orthogonal f
为了研究光学表面制造残差对成像系统性能的影响,提出了基于光学系统出瞳位相差的空间频段误差划分方法,推导出了统计意义下的中频(MSF)误差对调制传递函数(MTF)的影响函数解析式,确定了MTF 受中频误差影响的特征分辨率.对比低频(LSF)误差与MSF 误差影响的区别,MSF 误差导致系统调制传递函数从低分辨率处开始迅速下降,并根据中频影响函数解析式得到MSF 误差导致MTF 曲率突变特征分辨率.
We present an image recognition method to distinguish targets with cat-eye effect from the dynamic background based on target shape and modulation frequency. Original image sequences to be processed are acquired through an imaging mechanism that utilizes
We propose a high sensitivity sensor based on a mode number-encoded multi-longitudinal mode fiber laser. The fiber laser incorporates a uniform fiber Bragg grating (FBG) and a fiber Fabry-Perot interferometer (FFPI) as sensitive components in the cavity.
Asymmetric broad-waveguide separate-confinement heterostructure (BW-SCH) quantum well (QW) laser diode emitting at 808 nm is analyzed and designed theoretically. The dependence of the optical field distribution, vertical far-field angle, and internal loss
提出一种用于顺电相晶体Kerr系数和透射率的数字全息测量方法。该方法是数字记录晶体在不同电压时的全息图,再现数字全息图,得到晶体的复振幅信息,即振幅和相位分布。由晶体的振幅分布获得晶体的透射率;由相位分布得到不同电压差时的折射率变化量,从而计算得到晶体的电光系数。对顺电相Mn0.25%KLTN晶体进行了测量,记录了不同入射光模式以及不同电压时的数字全息图,得到了晶体透射率T和电光系数R11、R12。研究结果表明,该方法可用于顺电相晶体电光系数和透射率的测量,并且对晶体形状,照明光斑大小没有要求。
已研制成配有四级差分泵单元的2.5kW小型壁稳氩弧光源.其光谱辐射稳定性和重复性优于±0.5%,一致性优于±1%.其连续光谱分布可用Hofsaess理论计算,准确度达10%.等离子体光谱学诊断表明:氩弧电流40A、气压1.75×10~5Pa时,等离子体温度为12,650K,电子密度为1.29×10~(17)cm~(-3).