The thermodynamic limit in mean field neural networks

Elena Agliari, Adriano Barra, Pierluigi Bianco, Alberto Fachechi, Diego Pallara
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Abstract

In the last five decades, mean-field neural-networks have played a crucial role in modelling associative memories and, in particular, the Hopfield model has been extensively studied using tools borrowed from the statistical mechanics of spin glasses. However, achieving mathematical control of the infinite-volume limit of the model's free-energy has remained elusive, as the standard treatments developed for spin-glasses have proven unfeasible. Here we address this long-standing problem by proving that a measure-concentration assumption for the order parameters of the theory is sufficient for the existence of the asymptotic limit of the model's free energy. The proof leverages the equivalence between the free energy of the Hopfield model and a linear combination of the free energies of a hard and a soft spin-glass, whose thermodynamic limits are rigorously known. Our work focuses on the replica-symmetry level of description (for which we recover the explicit expression of the free-energy found in the eighties via heuristic methods), yet, our scheme is expected to work also under (at least) the first step of replica symmetry breaking.
平均场神经网络的热力学极限
在过去的五十年里,均值场神经网络在联想记忆建模中发挥了至关重要的作用,尤其是利用从自旋玻璃统计力学中借鉴的工具对 Hopfield 模型进行了广泛的研究。然而,由于为自旋玻璃开发的标准处理方法已被证明不可行,实现对该模型自由能的无限体积极限的数学控制仍然难以实现。在这里,我们解决了这个长期存在的问题,证明了理论阶次参数的量浓度假设足以保证模型自由能渐近极限的存在。证明利用了 Hopfield 模型自由能与硬自旋玻璃和软自旋玻璃自由能的线性组合之间的等价性,而后者的热力学极限是严格已知的。我们的工作集中在复制对称水平的描述上(我们通过启发式方法恢复了八十年代发现的自由能的解释性表达),然而,我们的方案预计也能在(至少)复制对称破缺的第一步下工作。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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