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Optimal configurations of spatial scale for grid cell firing under noise and uncertainty

We examined the accuracy with which the location of an agent moving within an environment could be decoded from the simulated firing of systems of grid cells. Grid cells were modelled with Poisson spiking dynamics and organized into multiple ‘modules’ of cells, with firing patterns of similar spatia...

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Autores principales: Towse, Benjamin W., Barry, Caswell, Bush, Daniel, Burgess, Neil
Formato: Online Artículo Texto
Lenguaje:English
Publicado: The Royal Society 2014
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3866454/
https://www.ncbi.nlm.nih.gov/pubmed/24366144
http://dx.doi.org/10.1098/rstb.2013.0290
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author Towse, Benjamin W.
Barry, Caswell
Bush, Daniel
Burgess, Neil
author_facet Towse, Benjamin W.
Barry, Caswell
Bush, Daniel
Burgess, Neil
author_sort Towse, Benjamin W.
collection PubMed
description We examined the accuracy with which the location of an agent moving within an environment could be decoded from the simulated firing of systems of grid cells. Grid cells were modelled with Poisson spiking dynamics and organized into multiple ‘modules’ of cells, with firing patterns of similar spatial scale within modules and a wide range of spatial scales across modules. The number of grid cells per module, the spatial scaling factor between modules and the size of the environment were varied. Errors in decoded location can take two forms: small errors of precision and larger errors resulting from ambiguity in decoding periodic firing patterns. With enough cells per module (e.g. eight modules of 100 cells each) grid systems are highly robust to ambiguity errors, even over ranges much larger than the largest grid scale (e.g. over a 500 m range when the maximum grid scale is 264 cm). Results did not depend strongly on the precise organization of scales across modules (geometric, co-prime or random). However, independent spatial noise across modules, which would occur if modules receive independent spatial inputs and might increase with spatial uncertainty, dramatically degrades the performance of the grid system. This effect of spatial uncertainty can be mitigated by uniform expansion of grid scales. Thus, in the realistic regimes simulated here, the optimal overall scale for a grid system represents a trade-off between minimizing spatial uncertainty (requiring large scales) and maximizing precision (requiring small scales). Within this view, the temporary expansion of grid scales observed in novel environments may be an optimal response to increased spatial uncertainty induced by the unfamiliarity of the available spatial cues.
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spelling pubmed-38664542014-02-05 Optimal configurations of spatial scale for grid cell firing under noise and uncertainty Towse, Benjamin W. Barry, Caswell Bush, Daniel Burgess, Neil Philos Trans R Soc Lond B Biol Sci Part III: Modelling grid cells We examined the accuracy with which the location of an agent moving within an environment could be decoded from the simulated firing of systems of grid cells. Grid cells were modelled with Poisson spiking dynamics and organized into multiple ‘modules’ of cells, with firing patterns of similar spatial scale within modules and a wide range of spatial scales across modules. The number of grid cells per module, the spatial scaling factor between modules and the size of the environment were varied. Errors in decoded location can take two forms: small errors of precision and larger errors resulting from ambiguity in decoding periodic firing patterns. With enough cells per module (e.g. eight modules of 100 cells each) grid systems are highly robust to ambiguity errors, even over ranges much larger than the largest grid scale (e.g. over a 500 m range when the maximum grid scale is 264 cm). Results did not depend strongly on the precise organization of scales across modules (geometric, co-prime or random). However, independent spatial noise across modules, which would occur if modules receive independent spatial inputs and might increase with spatial uncertainty, dramatically degrades the performance of the grid system. This effect of spatial uncertainty can be mitigated by uniform expansion of grid scales. Thus, in the realistic regimes simulated here, the optimal overall scale for a grid system represents a trade-off between minimizing spatial uncertainty (requiring large scales) and maximizing precision (requiring small scales). Within this view, the temporary expansion of grid scales observed in novel environments may be an optimal response to increased spatial uncertainty induced by the unfamiliarity of the available spatial cues. The Royal Society 2014-02-05 /pmc/articles/PMC3866454/ /pubmed/24366144 http://dx.doi.org/10.1098/rstb.2013.0290 Text en http://creativecommons.org/licenses/by/3.0/ © 2013 The Authors. Published by the Royal Society under the terms of the Creative Commons Attribution License http://creativecommons.org/licenses/by/3.0/, which permits unrestricted use, provided the original author and source are credited.
spellingShingle Part III: Modelling grid cells
Towse, Benjamin W.
Barry, Caswell
Bush, Daniel
Burgess, Neil
Optimal configurations of spatial scale for grid cell firing under noise and uncertainty
title Optimal configurations of spatial scale for grid cell firing under noise and uncertainty
title_full Optimal configurations of spatial scale for grid cell firing under noise and uncertainty
title_fullStr Optimal configurations of spatial scale for grid cell firing under noise and uncertainty
title_full_unstemmed Optimal configurations of spatial scale for grid cell firing under noise and uncertainty
title_short Optimal configurations of spatial scale for grid cell firing under noise and uncertainty
title_sort optimal configurations of spatial scale for grid cell firing under noise and uncertainty
topic Part III: Modelling grid cells
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3866454/
https://www.ncbi.nlm.nih.gov/pubmed/24366144
http://dx.doi.org/10.1098/rstb.2013.0290
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