啁啾光纤布拉格光栅展宽器的设计与制作

为获得较大展宽量的光纤器件,在相位掩模版刻写技术的基础上设计并制作了两种啁啾光纤布拉格光栅(CFBG)展宽器。基于相位掩模版刻写技术的原理和CFBG的色散补偿理论,提出了两种展宽器的制作方法,并优化了刻写光路,获得了高反射率、大反射带宽的CFBG。通过拉力传感器控制CFBG的反射谐振波长,通过改进刻写方式制作了大色散量的CFBG级联展宽器和大反射带宽的CFBG串联展宽器。搭建了两种展宽器的测试光源,通过直接测量的方式得到CFBG级联展宽器所提供的展宽量约为345 ps,这与理论结果相符;通过正、反接的方式间接推算了CFBG串联展宽器所提供的展宽量约为278.7 ps,这小于理论结果。     

4×10Gb/s 400km 啁啾光纤光栅色散补偿研究

介绍了利用光纤光栅成功实现了4×10Gb/s 400km G-652光纤的色散补偿，各信道传输部分在误码率为10-10时，无误码传输的功率代价均小于2dB，且最好的功率代价为负值- 关键词： 光纤光栅 色散补偿 功率代价     

低纹波系数色散补偿光纤光栅的研究

介绍用扫描法研制成功的长13．5cm、带宽0．447nm、反射谱平坦的切趾啁啾光纤光栅，功率波动小于1dB，用色散分析仪测试得到时延曲线上的纹波系数小于20ps，用该光纤光栅对200km的G．652光行色散补偿，补偿量大于98％（原始脉冲宽度为36．78ps，色散补偿后的脉冲宽度为37．23ps）。     

高速光通信系统中光纤光栅色散补偿研究

通过对光栅制作过程的优化设计，解决了光纤光栅温度稳定性、纹波系数、带宽、偏振模色 散补偿等关键技术，所制作光纤光栅已经达到温度系数小于00005 nm/℃，带宽大于14 nm，纹波系数小于50 ps，色散量超过 -1000 ps/nm的先进水平. 采用琼斯矩阵本征值法较 精确地测量了光栅的偏振模色散，并对其进行了补偿，光纤光栅色散补偿器的偏振模色散由 补偿前的91406 ps改善为补偿后的01521 ps. 在此基础上，成功地建立了一个稳定可靠 、速率为40 Gb/s，传输链路为122 km G 关键词： 高速光通信系统 普通单模光纤 光纤光栅 色散补偿     

大容量长距离传输用低非线性效应非零色散位移光纤

利用非等温等离子体化学气相沉积 (PCVD)工艺制备了一种适合于大容量高速率长途干线网与城域网的中芯下陷型纤芯结构非零色散位移光纤。该光纤的有效面积大于 95 μm2 ,在 15 5 0nm波段的色散值约为9ps/(nm·km) ,有效的抑制了传输过程中光非线性效应的产生。通过对光纤剖面结构的优化设计 ,光纤的 15 5 0nm处的传输损耗降到约 0 .2 1dB/km ,与传统单模光纤的熔接损耗低于 0 .11dB ,且在直径为 6 0mm圆筒上绕 10 0圈后在 14 6 0nm到 16 2 5nm波长范围所引起的附加弯曲损耗均低于 0 .0 2dB/km。同时 ,该光纤色散斜率低于0 .0 6 5 ps/(nm2 ·km) ,偏振模色散 (PMD)小于 0 .0 5 ps·km-1/2 。此外 ,由于光纤的零色散点移到了 14 30nm以下 ,使波分复用 (WDM)传输在S波段 (14 6 0～ 15 30nm)、C波段 (15 30～ 15 6 5nm)、L(15 6 5～ 16 2 5nm)波段上都兼容。     

双包层太赫兹光子晶体光纤的传输特性

为了在太赫兹波段实现远距离宽频带传输,设计了一种具有低吸收损耗的环烯烃共聚物(COC)作为基底材料双包层太赫兹光子晶体光纤。利用全矢量有限元法及模式选择理论,数值模拟了该光纤的单模传输范围、限制损耗、色散以及有效模场面积等特性。结果表明:优化结构参数可使在1~10 THz范围内基模限制损耗小于0.1 dB/m,二阶模限制损耗大于1 dB/m。因此可以获得1~10 THz的宽频带单模传输并且在1.5~10 THz内群速度色散可以控制在±0.1 ps/(THz·cm)。     

采用QPSK调制的50 Gbit/s高速大气激光通信传输特性研究

高级多电平调制格式在海上高速和高光谱效率的光通信中已经显示出巨大的潜力。将正交相移键控(QPSK)调制格式引入自由空间光(FSO)通信,实验证明可实现高达50 Gbit/s的高速FSO传输链路,能够清楚地观察到所发送的QPSK信号的眼图和星座图。通过比较传输之前和之后的误码率曲线,可以发现接收灵敏度都小于-36.7 dBm。当误码率为3.8×10-3时,它们的功率损失都小于4.2 dB。     

40Gb/s光时分复用传输光纤光栅补偿色散研究

用精密扫描掩模法写入宽阻带啁啾光纤光栅,掩模板背面两端各10％长度处镀有按4阶高斯函数透过率的膜,写入的啁啾光栅的时延纹波最大值为20ps。为减少写入光纤光栅的偏振模色散,研制了新的低偏振模色散光纤光栅补偿写入法。采用补偿写入法前的平均微分群时延为9．1406 ps;采用补偿写入法后的平均微分群时延为0．1521 ps。并利用低偏振模色散光纤光栅对40Gb／s光时分复用系统在普通G．652光纤传输122km的色散进行了补偿实验,功率代价为1．5dB。     

W波段回旋管宽带低损耗输入耦合系统

给出了一种十字交叉型TE□10-TE○01宽带模式转换器的设计原理,同时完成了一套W波段低损耗输入耦合系统的设计方案。根据该设计方案在电磁模拟软件HFSS中建立三维模型进行优化仿真。得到了衰减为0.14dB、最大驻波比为1.388、带宽为10GHz的高性能TE□10-TE○01宽带模式转换器。同时计算得到整套传输系统的衰减小于1dB,远小于采用矩形波导TE10模式的衰减(约15dB),大大提高了传输效率,降低了能量损耗。实际加工得到了一对模式转换器,经测试可得其衰减为1dB左右,整套系统的衰减约为3dB,与矩形波导(衰减约为15dB)相比,有了很大的提高。     

基于1085 km实地光纤链路的双波长光纤时间同步研究

在长距离高精度光纤时间同步系统中,为了减少后向反射光与光纤色散对传输精度的影响,本文在双波长光纤时间同步传输方法之上,提出了一种具有色散误差修正功能的双波长光纤时间同步传输方法.以自行研制的工程样机在长度约为800 km的实验室光纤链路上和1085 km的实地光纤链路上进行了实验测试,也是国内首次实现千公里级实地光纤时间同步传输.在实验室光纤链路上,测得传输链路色散补偿后的色散时延误差为10 ps,时间同步标准差为5.7 ps,稳定度为1.12 ps@105 s,不确定度为18.4 ps.在实地光纤链路上,测得传输链路色散补偿后的色散时延误差为60 ps,时间同步标准差为18 ps,稳定度为5.4 ps@4×10⁴ s,不确定度为63.5 ps.     

光纤光栅时延波动对传输系统性能的影响

对啁啾光栅的时延波动进行了详细的分析，建立了时延波动的简易模型和光栅的滤波函数。大量实验和计算表明，光纤光栅的时延纹波周期在0．01～0．1nm之间，并且在光纤光栅的阻带内，时延纹波周期随波长增大而逐渐增大。利用薛定谔方程对时延波动对系统的影响进行了仿真，得出了时延波动对系统的影响不仅与波动大小有关，而且还与时延波动周期有关，并用实验进行了验证。     

The system of L-band 2×10 Gb/s WDM transmission over conventional single mode fibre with 600 km by chirped fibre Bragg gratings dispersion compensation

A chirped fibre Bragg grating according to ITU-T suggested L-band (2nd channel $\lambda _{1}=1570.83$~nm; 80th channel $\lambda _{2}=1603.57$ nm) with more than 1800 ps/nm single channel dispersion compensation is presented in this paper, of which the cladding mode loss, the delay curve ripple and the power fluctuation of the reflected spectrum are less than 0.5 dB, 50 ps and 0.25 dB, respectively. With this new FBG as dispersion compensation device, a $2\times 10$ Gb/s wavelength division multiplexing (WDM) L-band transmission of 600 km based on conventional single mode fibre (G.652 fibre) is performed without forward error correction. The bit error rate (BER) is less than 10$^{ - 12}$ and the power penalties of the 2{nd} and 80{th} channel of L-band are 1.8~dB and 2.0~dB, respectively.     

High-power flat L-band erbium-doped fiber ASE source using dual forward-pumping scheme

We experimentally investigate a high output power L-band (1565–1605 nm) erbium-doped fiber amplified spontaneous emission (ASE) source using dual forward-pumping configuration. Such configuration allows high pumping-power operation and enhances the pumping efficiency. The high pumping efficiency of 36.1% is achieved for such ASE source with a mirror reflectance of 30%. The output power of about 72.2 mW and a linewidth of 40.8 nm with a power ripple of 0.7 dB are obtained without using any external spectral filters.     

Fast and accurate group delay ripple measurement technique for ultralong chirped fiber Bragg gratings

A simple and very precise group delay ripple (GDR) measurement technique for linearly chirped fiber Bragg gratings (CFBGs) is proposed. It is based on real-time optical Fourier transformation of an ultrashort pulse directly induced by the CFBG dispersion. We have experimentally demonstrated highly accurate characterization of the GDR profile of a commercial 10-m-long CFBG with a dispersion of +2000 ps/nm, having achieved a remarkably small standard deviation in our measurements of about 4 ps over a bandwidth of 28 nm. The proposed method has the unique potential to provide real-time GDR monitoring (in the MHz range) by use of commercially available high-speed sampling electronics.     

L-Band掺铒光纤放大器的优化设计

提出了泵浦分配两段级联,并利用前向ASE推动下一级EDF工作的L-Band放大器的新结构.基于Giles模型并考虑了ASE噪声的影响,运用数值模拟算法系统分析了泵浦光功率分配和铒光纤分配比例对这种EDFA性能的影响.最后优化得到高增益且增益谱平坦的L-Band EDFA,其在输入信号光功率为-20 dBm时,在1571～1608 nm范围内,增益值高达35 dB,增益偏差小于1 dB.     

Phase ripple correction: theory and application

Spectral phase ripple associated with novel dispersive devices can distort broadband optical signals. We present a digital postprocessing algorithm to correct for this distortion by exploiting the static deterministic nature of the ripple. This algorithm is demonstrated with empirical data for several systems employing chirped fiber Bragg gratings (CFBGs). We employ this technique in a photonic time-stretch system incorporating CFBGs, improving the signal fidelity by 9 dB. Simulations and experiments show that this algorithm, which can be reduced to a simple interpolation and matrix multiplication, also mitigates additive noise. We see that the act of distortion correction yields signal fidelity superior to that of an ideal dispersive element.     

Modal Birefringence Dependent Supercontinuum Due to Cross-Phase Modulation in a Dispersion-Flattened/Decreasing Fiber

It was found by numerical analysis that a 320 nm wide and flat spectrum at 20 dB less than the central maximum intensity is generated from cross-phase modulated soliton pulses with 3.5 ps pulse width and 2.3 W peak power, which are propagated through a 2.4km length of dispersion-flattened/decreasing fiber (DFDF). The cross-phase modulation (XPM) at a central wavelength of 1.55 μm is achieved by exciting two orthogonally polarized modes into the principal axes. The wave-vector mismatch between the orthogonal pulses can be neglected because of soliton trapping when the modal birefringence of the DFDF is less than |n_ox - n_0y| = 10⁻⁶. The effect of modal birefringence on supercontinuum generation is discussed in temporal and spectral regimes by numerical analysis.     

掺锗硅基高非线性光纤超连续光源研究

利用非线性偏振旋转锁模掺铒光纤激光器和1100m长的掺锗硅基高非线性光纤制作了超连续光源，获得了从1150～1750nm的超宽带输出光谱，其中1150～1350nm波段光谱起伏小于3dB，1600～1700nm波段平坦度优于1dB，并有很好的向长波延展空间。光谱展宽的机理为孤子分裂与受激拉曼散射，而四波混频使光谱进一步展宽。