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