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Ultrafast all-optical switching in multiple-quantum-well Y-junction waveguides at the band gap resonance

机译:带隙共振下多量子阱Y结波导中的超快全光切换

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摘要

An integrated Y-junction switch is used to demonstrate all-optical switching due to two mechanisms in GaAs-AlGaAs multiple quantum well structures at room temperature. Carrier-induced nonlinearities are compared to nonlinearities due to the optical Stark effect for ultrafast operation. In the first case, device geometry is exploited by a two-pulse switching process, whereby one control pulse turns the device on and a second control pulse turns the device off. Time gating of signal pulses within an 8 ps window was realized in our experiments. In the second case, the nonlinearity is ultrafast, and hence switching and recovery take place during the control pulse evolution. Consecutive switching events spaced 1.7 ps apart have been achieved. In our measurements, two-photon absorption played a significant role in the switching characteristics of the device. In order to access the carrier-induced nonlinearity, the pulse energy that is needed for switching (9 pJ in this case) results in a very high peak intensity that leads to two-photon absorption. This is observed as a strongly induced absorption exactly at the precise zero time delay between the control and signal pulses. In the second case, two-photon absorption competes directly with the optical Stark effect since both are instantaneous intensity dependent effects. Furthermore, the optical Stark effect appears to saturate at a low intensity level (0.9 pJ or 200 MW/cm/sup 2/); consequently only incomplete switching with a 2:1 contrast ratio was observed, whereas a 9:1 switching contrast was achieved with the carrier-induced nonlinearity.
机译:由于室温下GaAs-AlGaAs多量子阱结构中的两种机制,集成的Y结开关用于演示全光开关。由于光学斯塔克效应,可将载波感应的非线性与非线性进行比较,以实现超快操作。在第一种情况下,器件的几何结构是通过两脉冲切换过程来实现的,其中一个控制脉冲将器件导通,第二个控制脉冲将器件截止。在我们的实验中实现了8 ps窗口内信号脉冲的时间门控。在第二种情况下,非线性非常快,因此在控制脉冲演变过程中会发生切换和恢复。已经实现了间隔为1.7 ps的连续切换事件。在我们的测量中,双光子吸收在器件的开关特性中起着重要作用。为了获得载流子引起的非线性,切换所需的脉冲能量(在这种情况下为9 pJ)会导致很高的峰值强度,从而导致双光子吸收。可以观察到,这恰好是在控制脉冲和信号脉冲之间精确的零时间延迟时产生的强烈吸收。在第二种情况下,双光子吸收与光学斯塔克效应直接竞争,因为两者都是瞬时强度依赖性效应。此外,光学斯塔克效应似乎在低强度水平(0.9 pJ或200 MW / cm / sup 2 /)下饱和。因此,仅观察到对比度为2:1的不完全切换,而在载波感应的非线性下实现了9:1的切换对比度。

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