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Monolithically integrated Sagnac interferometer for all-optical wavelength conversion

机译:用于全光波长转换的单片集成的锯齿干涉仪

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All-optical wavelength conversion in the C-band is demonstrated using a regrowth free monolithically integrated Sagnac interferometer. A single semiconductor optical amplifier (SOA) placed asymmetrically in the loop acts as the non-linear element in the interferometer. Most integrated wavelength converters use the Mach-Zehnder geometry, which requires two SOAs, hence balancing the interferometer becomes an arduous task. The Sagnac geometry, on the other hand, uses a single SOA and the clockwise and the counter clockwise signals traverse the same optical path, thereby negating the effects of optical path length differences. A schematic diagram of the device along with an electron microscope image is shown in fig. 1. The passive elements of the device are comprised of etched waveguides and multimode-interference (MMI) couplers. Planar integration of the SOA onto the passive section is achieved using adiabatic tapered mode transformers. The principle of operation of the wavelength converter lies along the lines of the terahertz optical asymmetric demultiplexer (TOAD), or the semiconductor laser amplifier in a loop mirror (SLALOM). The SOA which is placed asymmetrically in the loop introduces a switching window. A continuous wave signal is fed into port 1 of the interferometer and is split equally by the 3dB MMI coupler. The two signals that are split by the MMI propagate in the clockwise and counter clockwise direction, finally interfering at the input MMI and dropping out of port 1 (reflective mode). The introduction of a time varying control signal (data) in port 3 makes the optical properties of the SOA also time dependent. When a wave front in the loop experiences an index difference relative to the counter propagating complement, the loop is no longer reflective and the signal is dropped out of port 2 for the duration corresponding to the switching window. The maximum repetition rate at which the wavelength converter can operate is limited by the recovery time of the SOA and hence is on the order of 10GHz.
机译:使用再生单片集成的SAGNAC干涉仪来证明C波段中的全光波长转换。在环路中不对称地放置的单个半导体光学放大器(SOA)用作干涉仪中的非线性元件。大多数集成的波长转换器使用Mach-Zehnder几何形状,这需要两个SOA,因此平衡干涉仪变为艰巨的任务。另一方面,SAGNAC几何形状使用单个SOA和顺时针和顺时针信号遍历相同的光路,从而否定光路长度差异的效果。图1中示出了装置和电子显微镜图像的装置的示意图。该装置的无源元件包括蚀刻波导和多模 - 干扰(MMI)耦合器。使用绝热锥形模式变压器实现SOA在无源部分上的平面整合。波长转换器的操作原理沿着太赫兹光学不对称多路分解器(蟾蜍)或环路镜(骨架)中的半导体激光放大器的线。在环路中不对称地放置的SOA引入了一个切换窗口。连续波信号被送入干涉仪的端口1,并由3DB MMI耦合器相等地分开。由MMI分开的两个信号在顺时针和逆时针方向上传播,最后干扰输入MMI并丢弃端口1(反射模式)。引入端口3中的时变控制信号(数据)使得SOA的光学特性也取决于时间。当循环中的波前面经历相对于计数器传播补充的索引差,循环不再反射,并且信号被丢弃出端口2,用于对应于切换窗口的持续时间。波长转换器可以操作的最大重复率受到SOA的恢复时间的限制,因此大约为10GHz。

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