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Dynamic Field Theory (DFT): Applications in Cognitive Science and ...

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In the follow<strong>in</strong>g we briefly discuss representative examples that shall illustrate<br />

the basic concepts of <strong>DFT</strong> <strong>and</strong> its application <strong>in</strong> different cognitive doma<strong>in</strong>s (for a<br />

recent survey of the mathematical treatment see [5]). As embodied validations of the<br />

approach, we <strong>in</strong>clude studies <strong>in</strong> which autonomous robots were endowed with some<br />

cognitive capacities such as decision mak<strong>in</strong>g, memory, action underst<strong>and</strong><strong>in</strong>g or<br />

anticipation. The reader is encouraged to visit the orig<strong>in</strong>al publications for proper<br />

treatment.<br />

Basic concepts<br />

<strong>Dynamic</strong> fields are def<strong>in</strong>ed over metric dimensions that <strong>in</strong> most applications reflect<br />

parameters of the experimental setup such as for <strong>in</strong>stance visual space, object features or<br />

movement parameters. A localized peak of activation with<strong>in</strong> the field represents metric<br />

<strong>in</strong>formation about the underly<strong>in</strong>g dimension. In analogy to the concept of neural<br />

population cod<strong>in</strong>g, the localized peak may be <strong>in</strong>terpreted as the activation pattern of a<br />

pool of neighbour<strong>in</strong>g neurons with similar tun<strong>in</strong>g properties <strong>in</strong> an otherwise <strong>in</strong>active<br />

population [8]. The peak evolves under the <strong>in</strong>fluence of time-dependent external <strong>in</strong>put<br />

but is ma<strong>in</strong>ly shaped by the recurrent <strong>in</strong>teractions with<strong>in</strong> the population. Due to the<br />

<strong>in</strong>teractions the peak is self-susta<strong>in</strong>ed <strong>and</strong> may thus serve to memorize <strong>in</strong>formation.<br />

However, <strong>in</strong> order to perform a work<strong>in</strong>g memory the field dynamics has to be bi-stable.<br />

The attractor state of a persistent fir<strong>in</strong>g pattern coexists with a stable homogenous<br />

activation distribution that represents the absence of <strong>in</strong>formation. A sufficiently strong<br />

transient <strong>in</strong>put specify<strong>in</strong>g a particular <strong>in</strong>stance of the metric dimension is able to<br />

“switch on” the memory function by destabiliz<strong>in</strong>g the uniform rest state. A suitable<br />

<strong>in</strong>hibitory signal, on the other h<strong>and</strong>, may destabilize the excited state, result<strong>in</strong>g <strong>in</strong> a<br />

decay of activation back to rest<strong>in</strong>g state. The critical parameter that decides whether or<br />

not the uniform state becomes unstable is <strong>in</strong>put strength. Below a certa<strong>in</strong> threshold,<br />

<strong>in</strong>homogeneous solutions of the field dynamics exist that are ma<strong>in</strong>ly <strong>in</strong>put driven. In<br />

many applications this regime is exploited to represent for <strong>in</strong>stance ambiguous prior<br />

<strong>in</strong>formation about the dimension spanned by the field. Much like prior distributions <strong>in</strong><br />

the Bayesian sense, multi-modal patterns of subthreshold activation may encode the<br />

probability of choices [9].<br />

With<strong>in</strong> the <strong>DFT</strong> framework, the existence of a memory function is closely l<strong>in</strong>ked<br />

to decision mak<strong>in</strong>g. A self-susta<strong>in</strong>ed activation peak is the result of the <strong>in</strong>terplay<br />

between excitatory <strong>and</strong> <strong>in</strong>hibitory forces with<strong>in</strong> the field. Excitatory <strong>in</strong>teractions<br />

between neighbour<strong>in</strong>g neurons are counterbalance by lateral <strong>in</strong>hibition. S<strong>in</strong>ce <strong>in</strong>hibitory<br />

<strong>in</strong>teractions dom<strong>in</strong>ate at larger distances, a competition process takes place whenever<br />

two or more suprathreshold <strong>in</strong>puts are simultaneously applied. At the field site that<br />

<strong>in</strong>tegrates the highest level of sensory or other evidence a s<strong>in</strong>gle activation peak will<br />

emerge. It suppresses the activation elsewhere <strong>in</strong> the field below rest<strong>in</strong>g level. Once the<br />

stable attractor state has been reached, the decision represented by the peak location is<br />

protected aga<strong>in</strong>st noise <strong>and</strong> fluctuations <strong>in</strong> the <strong>in</strong>put stream. This does not mean,<br />

however, that the peak is completely immune aga<strong>in</strong>st change. Localized <strong>in</strong>put that<br />

spatially overlaps with the peak position causes the peak to drift <strong>in</strong> the direction of this<br />

<strong>in</strong>put. Mathematically, the attractor can be described as be<strong>in</strong>g cont<strong>in</strong>uous along the<br />

dimension spanned by the field. This property of the field dynamics has been exploited<br />

for <strong>in</strong>stance to expla<strong>in</strong> <strong>and</strong> apply the capacity of track<strong>in</strong>g time-vary<strong>in</strong>g <strong>in</strong>put <strong>in</strong> real time<br />

([10], [11]).<br />

Although the formation of spatially localized peaks is certa<strong>in</strong>ly the backbone of<br />

most <strong>DFT</strong>-based models thus fare, it is important to note that the field dynamics - if<br />

properly tuned - may exhibit other types of self-organiz<strong>in</strong>g patterns (e.g., .travell<strong>in</strong>g

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