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Scale-Free Memory to Swiftly Generate Fuzzy Future Predictions

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Proceedings of the Fifth International Conference on Fuzzy and Neuro Computing (FANCCO - 2015)

Part of the book series: Advances in Intelligent Systems and Computing ((AISC,volume 415))

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Abstract

A flexible access to how the current state of memory would evolve into the future is extremely valuable in predicting events to occur in distant future. We propose a neural mechanism to non-destructively translate the current state of temporal memory into the future, so as to construct a timeline of future predictions. In a two-layer memory network that encodes the Laplace transform of the past, time-translation can be accomplished by modulating the weights between the layers. Computationally, such a network appears to be extremely resource-conserving, and could prove useful in AI systems. We hypothesize that such a mechanism is neurally realistic in the sense that the brain performs it. We propose that within each cycle of hippocampal theta oscillations, the memory state is swept through a range of time-translations to yield a future timeline of predictions. A physical constraint requiring coherence in time-translation across memory nodes results in a Weber-Fechner spacing for the representation of both past (memory) and future (prediction) timelines.

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Notes

  1. 1.

    The phase \(\theta \) deterministically varies in real time \(\tau \) with a periodicity of 250 ms. However, in the context of representing memory from much larger timescales, it is convenient to treat \(\theta \) and \(\tau \) in Eq. 4 as independent. Within each theta cycle, treating \(\tau \) as a constant is a fair approximation.

  2. 2.

    To ensure continuity around \(\theta _s=0\), we take the Eq. 7 to hold true even when \(\theta _s \in (-\pi ,0)\). However, since notationally \(\theta _s\) makes a jump from \(+\pi \) to \(-\pi \), \(\varPhi (\theta _s)\) must make a quick transition from \(\varPhi _{\text {max}}\) (\(\theta _s=\pi \)) to \(\varPhi _{\text {min}}=\varPhi _o^2/\varPhi _{\text {max}}\) (\(\theta _s=-\pi \)).

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Acknowledgments

Supported by NSF PHY 1444389 and the Initiative for the Physics and Mathematics of Neural Systems.

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Correspondence to Karthik H. Shankar .

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Appendix

Appendix

This appendix provides an explicit recipe for computing \(\mathbf {L}^{{{-1}}}_{\text {k}}\) for the distribution of \(s_n\) derived in the text and \(k=2\). A more general derivation can be found in [14]. When \(s_n = s_o (1+c)^{-n}\) the connection strengths in the \(\mathbf {L}^{{{-1}}}_{\text {k}}\) operator takes a special form–for every n, the local connectivity from the \((2k+1)\) \(\mathbf {t} _{ } \)-nodes to the n-th \(\mathbf {T} _{ } \)-node has an identical form multiplied by \(s_n\). For example, with \(k=2\), the connection strengths to the n-th \(\mathbf {T} _{ } \) node from the \(\mathbf {t} _{ } \) nodes in the local neighborhood are given by

$$\begin{aligned} \mathbf {t} _{n+2 }\rightarrow & {} s_n \frac{(c+1)^5}{c^2(c+2)^2} \\ \mathbf {t} _{n+1 }\rightarrow & {} s_n \frac{-(c+1)^2}{c} \\ \mathbf {t} _{n }\rightarrow & {} s_n \frac{c^4+3c^3 +c^2 -4c-2}{c^2(c+2)^2} \\ \mathbf {t} _{n-1 }\rightarrow & {} s_n \frac{1}{c^2+c} \\ \mathbf {t} _{n-2 }\rightarrow & {} s_n \frac{1}{c^2(c+1)(c+2)^2} \\ \end{aligned}$$

The factor \(s_n\) can be treated as a post-synaptic weight and the rest (which only depend on c) can be treated as pre-synaptic weight which are constant along the dorsoventral axis.

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Shankar, K.H., Howard, M.W. (2015). Scale-Free Memory to Swiftly Generate Fuzzy Future Predictions. In: Ravi, V., Panigrahi, B., Das, S., Suganthan, P. (eds) Proceedings of the Fifth International Conference on Fuzzy and Neuro Computing (FANCCO - 2015). Advances in Intelligent Systems and Computing, vol 415. Springer, Cham. https://doi.org/10.1007/978-3-319-27212-2_15

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  • DOI: https://doi.org/10.1007/978-3-319-27212-2_15

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