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All-optical logic OR gate based on cross gain modulation in Semiconductor Optical Amplifiers

机译:基于半导体光放大器中交叉增益调制的全光学逻辑或门

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Semiconductor Optical Amplifiers (SOAs) are very attractive components for optical communication systems. We have already shown that two-cascaded SOAs in a counterpropagating configuration (TC-SOA-CC) based on XGM is interesting for all-optical signal processing (Fig. 1) [1-3]. The contra-directional input signals P{sub}(in,1)(λ{sub}1), P{sub}(in,3)(λ{sub}3) and P{sub}(in,2)(λ{sub}2) are injected in SOA{sub}1 and SOA{sub}2 respectively. In this configuration, a negative feedback controls the evolution of the SOAs gains. In the absence of P{sub}(in,3) and the presence of a low power P{sub}(in,1), the P{sub}(in,2) signal profits from the high SOA{sub}2 gain G{sub}2 allowing to saturate the SOA{sub}1 gain G{sub}1. By increasing P{sub}(in,1), the SOA{sub}1 output optical power injected in the SOA{sub}2 becomes enough to saturate the gain G{sub}2. This reduction in G{sub}2 can induce an increase in G{sub}1 if the total injected power, coming from SOA{sub}2 and from the increase in P{sub}(in,1), decreases. Figure 1 shows the evolution of the SOA{sub}1,2 gains versus the input optical power P{sub}(in,1)(λ{sub}1) and in the presence of P{sub}(in,2)(λ{sub}2) = -15 dBm. For high G{sub}2 (I{sub}2 = 280 mA), G{sub}1 presents a positive variation for P{sub}(in,1) range - 23 dBm < P{sub}(in,1) < -14 dBm, while G{sub}2 decreases strongly beyond P{sub}(in,1)> -23 dBm. This positive slope disappears for low G{sub}2 (I{sub}2 = 150 mA). In this case, the G{sub}2 reduction which occurs with high P{sub}(in,1) power (P{sub}(in,1) = -13 dBm) is not sufficient to drop off the total injected power and the SOA{sub}1 starts to saturate.
机译:半导体光学放大器(SOA)是光通信系统的非常有吸引力的组件。我们已经表明,基于XGM的反执行配置(TC-SOA-CC)中的双级联SOA是有趣的,对所有光信号处理有趣(图1)[1-3]。对准输入信号P {Sub}(in,1)(λ{sub} 1),p {sub}(in,3)(λ{sub} 3)和p {sub}(在,2)( λ{sub} 2分别注入SOA {sub} 1和SOA {sub} 2中。在这种配置中,负反馈控制SOA增益的演变。在没有p {sub}(在3)的情况下以及低功率p {sub}(在,1),p {sub}(in,2)信号利用来自高SOA {sub} 2增益g {sub} 2允许饱和SOA {sub} 1增益g {sub} 1。通过增加P {sub}(在,1),SOA {sub} 1在SOA {sub} 2中注入的光功率变得足以使增益G {sub} 2饱和。如果来自SOA {sub} 2的总注入功率和P {sub}(在1)增加,则该G {Sub} 2的减小可以引起G {Sub} 1的增加。图1示出了SOA {sub} 1,2增益的演变与输入光功率p {sub}(in,1)(λ{sub} 1)和在p {sub}的存在中(在,2) (λ{sub} 2)= -15 dBm。对于高g {sub} 2(i {sub} 2 = 280 mA),g {sub} 1呈现p {sub}(in,1)范围 - 23 dbm {sub}的正变型(在,1 )<-14 dBm,而g {sub} 2强烈地减少了p {sub}(在,1)> -23 dBm。该正斜率消失为低g {sub} 2(i {sub} 2 = 150 mA)。在这种情况下,高p {sub}(1)功率(p {sub}(in,1)= -13 dBm)发生的g {sub} 2减少不足以下降到总注入的电源并且SOA {sub} 1开始饱和。

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