A Cursory Introduction to the Physicists' Neural Networks

Abstract

The paper is a very short introduction to networks of formal neurons, intended to outline the main problems and trends and provide some basic references. In the past half-century, many attempts have been made to model various parts of the brain, particularly those responsible for such functions as perception, movement, memory and learning. One of the first major contributions to the mathematical modeling of brain function was a paper published in 1943, where Warren S. McCulloch and Walter H. Pitts introduced their "formal neuron", a highly stylized version of the real thing Ill. They showed that networks of interconnected formal neurons could perform specific logical tasks. Less mathematical but extremely influential was the work of the psychophysiologist Donald 0. Hebb, who in 1949 introduced the notion of a "cell assembly", a distributed representation of an external event inside a neural network 121. Hebb proposed that cell assemblies are created, and continually modified during learning, as a consequence of the modification of the synaptic efficacies, i.e., the conductances of the contacts between neurons. According to Hebb's rule, repeated activation of one neuron by another leads to an increase of the strength of the synapses which take part in the activation process. McCulloch and Pitts's formal neuron, as well as Hebb's learning rule, are still widely used in physicists' models. The first attempts at designing machines inspired from the nervous system were made in the 19601s, but these attempts were only partly successful: limitations became soon apparent, that could not be overcome with the technical and conceptual tools available at that time 131. The level of activity in the field remained fairly low for some twenty years. In 1982, the physicist John J. Hopfield published his seminal paper in which he recognized the analogy between Hebb's cell assemblies and disordered magnetic systems 141. The proof that the proposed model was analytically solvable 151 triggered a large research effort in recent years. The number of papers on neural networks, particularly of the Hopfield type, originating from the physics community, is probably well over one hundred at the present day 161. An even larger number of papers, many of which are authored by computer scientists or electrical engineers, describe potential applications of various types of neural networks 151, in such fields as artificial vision, speech understanding and synthesis, combinatorial optimization, interpolation and prediction ... The elementary component in most of these models is the McCulloch-Pitts formal neuron, or a somewhat elaborate version thereof. Such processing units are infinitely less complex than real neurons. It is, however, the very simplicity of these models which makes them attractive, for the following reasons: as mentioned above, the tools of statistical physics can be used to analyze and predict the behaviour of large assemblies of formal neurons; one may in particular investigate the information storage properties and the dynamics of learning and retrieval of such networks acting as associative memories; despite their crudeness, these models are able to account for some properties of biological neural assemblies; such approaches are gradually gaining acceptance among neurobiologists, although debates are far from being settled 171; electronic or opto-electronic networks of formal neurons can be built, thus opening the Article published online by EDP Sciences and available at http://dx.doi.org/10.1051/jphyscol:1989331 C3-208 JOURNAL DE PHYSIQUE way to potential industrial applications. The neural networks studied today belong essentially to two families: Feedforward neural networks, in which information flows from an input layer to an output layer through a small number (one to three) of "hidden layers". These networks use vario'us rules for modifying their synapses, including the popular "error back-propagation algorithm" 161. They exhibit interesting properties for classification and related problems. Although their behaviour is far from being completely understood, they are good candidates for applications; they are probably less relevant as models of biological nervous systems. Feedback neural networks, whose archetype is the Hopfield network. These are dynamical systems, which evolve in time until they reach a stationary state. They have been the favorite subject of investigation for physicists. The initial Hopfield model has been greatly refined in order to gain biological plausibility, one of the major steps being the derivation of analytic results for systems with asymmetric couplings 181. Moreover, results of great importance concerning the limitations of the storage capacity of such networks were derived 191. Although the level of activity in the field has undergone a tremendous increase in recent years, many issues are still to be addressed. In particular, much needs to be done to bring these models closer to rece3t experimental data from neurobiology and cognitive sciences: as was mentioned abode, some of the key ingredients in recent works date back to the 1940's. More elaborate models are still considered untractable, but this will presumably change in the future. Another type of work that is called for concerns the limitations in the capabilities of formal neural networks. As was mentioned above in connection with ref. 8, results concerning the limitations of associative memory networks are now available. Similar results on the learning and generalization capabilities of feedforward networks are still needed; this lack of solid conceptual bounds might lead to unreasonable hopes, especially in the field of short-term applications.

Cite this paper

@inproceedings{Personnaz2017ACI, title={A Cursory Introduction to the Physicists' Neural Networks}, author={L{\'e}on Personnaz and Elie Bienenstock and G{\'e}rard Dreyfus}, year={2017} }