Photonic Reservoir Computing by Daniel Brunner Miguel C. Soriano Guy Van der Sande
Author:Daniel Brunner, Miguel C. Soriano, Guy Van der Sande
Language: eng
Format: epub
Publisher: Walter de Gruyter
Published: 2019-04-15T00:00:00+00:00
5.5.1 Interconnection structure through system dynamics
When , the state of a given virtual node at time t depends on the states of the previous virtual nodes due to the noninstantaneous response of the system (T) to the inputs. The strength of this dependency for low-pass filtered systems is an exponentially decaying function of the separation of the virtual nodes.
For the case of (i.âe., the only connection between the virtual nodes are through the system dynamics) and a time series prediction task (NARMA10), it was found that is the best choice for virtual nodes [6]. This ratio leads to significant coupling between neighboring virtual nodes, as illustrated in Figure 5.7. In Figure 5.7(a), the node output never leaves the transient regime. Since the state of one virtual node depends on the state of the previous ones because of the system dynamics, the equivalent connectivity graph is given by Figure 5.7(b). All nodes are connected to adjacent nodes, with the connection weights exponentially decreasing as we move further back in time. They also experience the self-coupling as in this case.
The relation between the timescales can be used to establish a more formal link between the traditional formulation of reservoir computing, such as given in Section 5.2 and the virtual interconnections created through the system dynamics. In what follows, we will derive an approximate interconnection matrix describing the coupling between virtual nodes processing information from different input time steps where they are only connected through the system dynamics. For simplicity of notation, in the following we normalize all times with respect to the intrinsic time scale of the nonlinear system T, that is we work in units where . In the following, we consider nonlinear equations of the form:
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