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A complex network of 1600 holographically coupled opto-electronic oscillators: Network dynamics and utilisation for reservoir computing

机译:由1600个全息耦合光电振荡器组成的复杂网络:储层计算的网络动力学和利用

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Networks of photonic elements are a key enabling technology for the realization of multiple next generation photonic systems. Phased beam arrays, coherent beam combining or neuromorphic computing in photonic networks: all these high-impact applications fundamentally require coupling between a large number of photonic components. Recently, a small network of ~20 semiconductor lasers based on coupling via a holographic element was reported [1]. However, the demonstration of large-scale complex photonic networks is lacking.Here, we demonstrate the scalability of holographic coupling, creating a large scale complex network of 1600 opto-electronic oscillators. The network's nonlinear nodes are implemented using a spatial light modulator (SLM) operated in intensity modulation mode. Imaging the SLM-surface through a polarizing beam splitter (PBS) onto a camera and closing the loop between camera and the SLM, we realize a nonlinear iterative map. The state of SLM pixel n is then given by In(t + 1) = sin2(κIn(t) + φ0). Here, In(t)is the nth pixel intensity at time t, κ the feedback gain and φ0 a constant phase offset. This equation corresponds to a simplified version of the Ikeda map. Figure 1 (a) schematically illustrates the experimental implementation. An exemplary bifurcation diagram for node (23, 8) is shown in Fig. 1 (b). The route to chaos shown in Fig. 1(b) exhibits the period-doubling behaviour expected from such an Ikeda system.
机译:光子元件网络是实现多个下一代光子系统的关键使能技术。光子网络中的相控光束阵列,相干光束组合或神经形态计算:所有这些高冲击性应用基本上都需要在大量光子组件之间进行耦合。近来,据报道有一个由20个半导体激光器组成的小型网络,该网络基于通过全息元件的耦合[1]。但是,缺乏大规模复杂光子网络的演示,此处我们展示了全息耦合的可扩展性,从而创建了由1600个光电振荡器组成的大规模复杂网络。使用在强度调制模式下运行的空间光调制器(SLM)来实现网络的非线性节点。通过偏振分束器(PBS)将SLM表面成像到相机上并关闭相机和SLM之间的环路,我们实现了非线性迭代图。然后通过I n (t +1)= sin 2 (κI n (t)+φ< sub> 0 )。在这里,I n (t)是在时间t处的第n个像素强度,κ是反馈增益,而φ 0 是恒定的相位偏移。该方程式对应于池田地图的简化版本。图1(a)示意性地说明了实验实现。图1(b)示出了节点(23、8)的示例性分叉图。图1(b)所示的混乱之路表现出了从这种池田系统所期望的周期倍增行为。

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