Asymmetric multimode interference isolator based on nonreciprocal phase shift

This paper presents an asymmetric multimode interference-based (MMI) optical isolator, by utilizing the magneto-optical nonreciprocal phase shift (NPS). Equivalent beam propagation method (BPM) simulation of symmetric and asymmetric isolators are performed using configuration of Air/Ce:YIG/SiO₂ on silicon substrate for integration. The asymmetric isolator is found to be much more compact in size and efficient in isolation compared with symmetric isolator. Simulation results show that the isolation of asymmetric structure is 23.8 dB higher than that of symmetric one. It is mainly because both symmetric mode and anti-symmetric mode are excited in asymmetric structure and hence can interfere destructively. The proposed device may play an important role in the optical communication systems and photonic integrated devices.     

Tamely uniform orders

The following two results are proven.

(i) Let G be a finitely generated torsion-free linear group. If every torsion-free section of G is an R-group, then G is soluble of finite rank. Conversely, if G has finite rank, then it has a subgroup of finite index, in which every torsion-free section is an R-group.

Let G be a finitely generated torsion-free soluble group. If in every torsion-free section of G the normalizer of each isolated subgroup is isolated, then G has finite rank. Conversely, if G has finite rank, then it has a subgroup K of finite index such that in every torsion-free section of K the normalizer of each isolated subgroup is isolated.     

高功率法拉第隔离器多模退偏特性

理论分析了隔离器在高功率多模激光入射时的自退偏特性.结果表明:线性双折射致退偏与圆双折射致退偏均与入射光功率的平方成正比,线性双折射致退偏与光斑大小无关,而圆双折射致退偏随光斑半径的增大而减小.当光斑半径与旋转晶体半径相比很小时(R0/r0≥80)圆双折射引起的退偏大于线性双折射引起的退偏,当光斑半径接近旋转晶体半径(R0/r0≤3)时,与线性双折射引起的退偏相比,圆双折射引起的退偏可以忽略.对比单模激光入射,在同种条件下,多模入射使得线性双折射致退偏减小了0.4倍, 最小圆双折射致退偏减小为0.05倍.     

高功率法拉第隔离器多模退偏特性

理论分析了隔离器在高功率多模激光入射时的自退偏特性.结果表明：线性双折射致退偏与圆双折射致退偏均与入射光功率的平方成正比,线性双折射致退偏与光斑大小无关,而圆双折射致退偏随光斑半径的增大而减小.当光斑半径与旋转晶体半径相比很小时（R0/r0≥80）圆双折射引起的退偏大于线性双折射引起的退偏,当光斑半径接近旋转晶体半径（R0/r0≤3）时,与线性双折射引起的退偏相比,圆双折射引起的退偏可以忽略.对比单模激光入射,在同种条件下,多模入射使得线性双折射致退偏减小了0.4倍, 最小圆双折射致退偏减小为0.05倍.     

基于单壁碳纳米管的双向锁模掺铒光纤激光器

设计了一种没有隔离器的单壁碳纳米管双向被动锁模光纤孤子激光器.该光纤激光器由波分复用器、掺铒光纤、光耦合器、碳纳米管、单模光纤和偏振控制器组成.在环形腔的两个相反方向上,同时实现基于碳纳米管饱和吸收体的被动锁模,得到两个反向稳定脉冲序列.调节激光腔中的偏振控制器以及泵浦激光源,分析该实验装置在不同泵浦功率下的输出特性.结果表明,中心波长变化范围为1 558~1 560nm,顺时针脉冲宽度变化范围为854~959ps,逆时针脉冲宽度变化范围为247~624ps.此外,泵浦功率较大时,逆时针方向上脉冲序列分裂.     

级联双包层铒镱共掺光纤放大器的性能分析

基于速率方程和光传输方程,对级联双包层铒镱共掺光纤放大器（Er3+/Yb3+ co-Doped Fiber Amplifier,EYDFA）进行了研究.数值模拟计算得到级联双包层EYDFA的最佳光纤长度,以及前后向泵浦功率之比和光隔离器位置对于增益以及噪音系数的影响.通过选择合适的前后向泵浦功率之比和隔离器的位置优化级联放大器结构,其增益提高了4 dB,噪音系数降低了近3 dB.     

Ku波段低温低噪声放大器设计

本文采用插指电容新结构设计了一个Ku波段低温低噪声放大器(LNA),并通过优化的封装工艺制备了放大器样品,分析了隔离器对LNA性能的影响.在77K温度下测试结果表明,放大器增益约10dB,噪声系数小于2.0dB,反射系数小于-17dB.     

周期性非轴对称孔槽结构隔声性能数值模拟研究

设计了一种利用周期性非轴对称孔槽来消除钻铤模式波的隔声体结构,并采用三维有限元法对其隔声效果进行了数值模拟。结果表明:所提出的隔声体的隔声效果与孔槽圆弧的半径、孔槽间隔及孔槽的数目等有关;适当选取刻槽方式时,1 m长的隔声体对单极子源激发的钻铤波的衰减可达22 dB,但对偶极子源激发的挠曲波的衰减效果不明显。