Burst firing creates an attractor in synaptic weight dynamics.
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The authors' code
Julia · 130 lines · 4.2 KB · no license
- # Functions
- function ISIfunc(Spkt::Array{Float64}) # Computes the interspike intervals out of spike times
- ISI = zeros(200000)
- l::Int64 = 1
- for i = 2:length(Spkt)
- ISI[l] = Spkt[i] - Spkt[i-1]
- l += 1
- end
- return ISI
- end
- function remove0(ISI::Array{Float64}) # Removes 0's in spike times/interspike intervals vectors
- f = findall(ISI .== 0)
- if f[1] > 1
- ISI = ISI[1:f[1]-1]
- else
- ISI = [0.]
- end
- return ISI
- end
- function isbursting(ISI::Array{Float64}) # Check if the neuron is bursting using the rule 3*minISI < maxISI
- bursting::Int64 = 0
- if minimum(ISI)*4 < maximum(ISI)
- bursting = 1
- end
- return bursting
- end
- function SPB_PER_DC_IBFfunc(ISI::Array{Float64}) # Computes spike per burst (SPB), period (PER), duty cycle (DC) and mean intraburst frequency of bursting neurons.
- minISI = minimum(ISI)
- maxISI = maximum(ISI)
- interburst = findall(ISI .>= maxISI/3)
- intraburst = findall(ISI .<= maxISI/3)
- SPB = round(length(intraburst)/length(interburst))+1
- IBP = mean(ISI[intraburst])
- Burstdur = IBP*(SPB-1)
- PER = Burstdur+mean(ISI[interburst])
- DC = Burstdur/PER
- IBF = 1000/IBP
- return (SPB, PER, DC, IBF)
- end
- function compute_params(spk_ncells::Array{Float64},Ttransient::Int64,tstepstart::Int64,tstepinit::Int64,tstepstop::Int64) # Extracts frequency or (SPB, PER, DC and IBF) out of the spiketimes saved in the Spkt$n.dat files. The number of cells is given by the number of lines in gs.
- ncells = length(spk_ncells[:,1])
- ISIs_depol = zeros(200000)
- ISIs_hyperpol = zeros(200000)
- PARAMS_depol = zeros(ncells,4) #[SPB;PER;DC;IBF]
- PARAMS_hyperpol = zeros(ncells,4) #[SPB;PER;DC;IBF]
- freq_depol = zeros(ncells)
- freq_hyperpol = zeros(ncells)
- for n = 1:ncells
- f1 = findall(spk_ncells[n,:] .>= Ttransient) #Removes the transient of depol period
- f2 = findall(spk_ncells[n,:] .>= tstepstart) #Finds end of depol period
- f3 = findall(spk_ncells[n,:] .>= tstepinit) #Removes the transient of hyperpol period
- f4 = findall(spk_ncells[n,:] .>= tstepstop) #Finds end of hyperpol period
- f5 = findall(spk_ncells[n,:] .== 0) #Removes the zeros at the end of the vector
- if length(f1) == 0
- Spkt_depol = [0.]
- Spkt_hyperpol = [0.]
- elseif length(f1) == length(f2)
- Spkt_depol = [0.]
- if length(f3) == length(f4)
- Spkt_hyperpol = [0.]
- elseif length(f4) > 0
- if(isempty(f3))
- Spkt_hyperpol = [0.]
- else
- Spkt_hyperpol = spk_ncells[n,f3[1]:f4[1]-1]
- end
- else
- if(isempty(f5)||isempty(f3))
- Spkt_hyperpol = [0.]
- else
- Spkt_hyperpol = spk_ncells[n,f3[1]:f5[1]-1]
- end
- end
- else
- if(isempty(f2))
- Spkt_depol = [0.]
- else
- Spkt_depol = spk_ncells[n,f1[1]:f2[1]-1]
- end
- if length(f3) == length(f4)
- Spkt_hyperpol = [0.]
- elseif length(f4) > 0
- if(isempty(f3))
- Spkt_hyperpol = [0.]
- else
- Spkt_hyperpol = spk_ncells[n,f3[1]:f4[1]-1]
- end
- else
- if(isempty(f5)||isempty(f3))
- Spkt_hyperpol = [0.]
- else
- Spkt_hyperpol = spk_ncells[n,f3[1]:f5[1]-1]
- end
- end
- end
- ISI_depol = ISIfunc(Spkt_depol)
- ISI_hyperpol = ISIfunc(Spkt_hyperpol)
- ISItemp_depol::Array{Float64} = remove0(ISI_depol)
- ISItemp_hyperpol::Array{Float64} = remove0(ISI_hyperpol)
- if isbursting(ISItemp_depol) == 1
- (PARAMS_depol[n,1],PARAMS_depol[n,2],PARAMS_depol[n,3],PARAMS_depol[n,4]) = SPB_PER_DC_IBFfunc(ISItemp_depol)
- #freq_depol[n] = 0.
- else
- PARAMS_depol[n,:] .= 0.
- freq_depol[n] = 1000/mean(ISItemp_depol)
- end
- if isbursting(ISItemp_hyperpol) == 1
- (PARAMS_hyperpol[n,1],PARAMS_hyperpol[n,2],PARAMS_hyperpol[n,3],PARAMS_hyperpol[n,4]) = SPB_PER_DC_IBFfunc(ISItemp_hyperpol)
- #freq_hyperpol[n] = 0.
- else
- PARAMS_hyperpol[n,:] .= 0.
- freq_hyperpol[n] = 1000/mean(ISItemp_hyperpol)
- end
- ISIs_depol = [ISIs_depol ISI_depol]
- ISIs_hyperpol = [ISIs_hyperpol ISI_hyperpol]
- end
- ISIs_depol = ISIs_depol[:,2:end]
- ISIs_hyperpol = ISIs_hyperpol[:,2:end]
- return ISIs_depol, ISIs_hyperpol, PARAMS_depol, PARAMS_hyperpol, freq_depol, freq_hyperpol
- end
PARAMS_cycle.jl at commit f3d3133, no license · at the source
Overview
- Biology Department, Brandeis University, Waltham, Massachusetts, United States of America
- Department of Electrical Engineering and Computer Science, University of Liège, Liège, Belgium
- Viterbi School of Engineering, University of Southern California, Los Angeles, California, United States of America
- Center for Theoretical Neuroscience, Columbia University, New York, New York, United States of America
Abstract
Neural circuits often alternate between tonic and burst firing, two distinct activity regimes that reflect changes in excitability and neuromodulatory state. While tonic firing produces asynchronous spikes driven by diverse external inputs, collective burst firing consists of rapid clusters of spikes followed by a period of silence, happening synchronously within the network. Synaptic plasticity has typically been studied only in either one of these regimes, leaving unclear how their distinct plasticity dynamics can be combined when circuits alternate between regimes. Here, we use a conductance-based network model endowed with calcium-based or spike-timing–based plasticity rules to examine how synaptic weights evolve across tonic and burst firing regimes. During tonic firing, synaptic weights are driven by the statistics of external inputs, producing a broad distribution across the network. In contrast, during collective burst firing, weights converge to a narrow region in weight space: a burst-induced attractor. We derive the location of this attractor analytically in terms of plasticity parameters and activity statistics, and confirm its emergence across diverse plasticity rules. The attractor reflects the synchronization of plasticity-driving signals during bursts, which homogenizes synaptic dynamics and forces convergence toward shared fixed points. We further show that neuromodulation and synaptic tagging can shift or split the burst-induced attractor, stabilizing selected synapses while weakening others. Together, these results identify burst-induced attractors as a robust emergent property of collective bursting. Alternation between tonic and burst firing provides a biologically plausible context in which heterogeneous, input-driven synaptic configurations formed during tonic activity can be selectively consolidated or down-selected by the burst-induced attractor during subsequent bursts. By showing how they can be analytically predicted and experimentally modulated, our work provides a general computational framework linking firing state transitions, synaptic plasticity, and memory organization.
Reproduced under the paper's license (CC BY), from the paper cited above.
Repository
Its files are read in the Code ↔ Paper reader above.
KJacquerie/Burst-Attractor
f3d31332899dc4a53ed7d4e623443d653430d3fa, 14 February 2026Availability: 1 check, the latest on 30 September 2026: the link answers
- 30 September 2026: the link answers
42 files
- Fig1/
julia/ , Julia, 130 linesPARAMS_cycle.jl - Fig1/
julia/ , Julia, 349 linesSimu_scenario_GB2012.jl - Fig1/
julia/ , Julia, 409 linesmodel_scenario_GB2012_RE SET.jl - Fig1/
matlab/ , MATLAB, 955 linesFig1.m - Fig2_Demo/
CalciumRule/ , Julia, 303 linesSimu_reduced_AMPA.jl - Fig2_Demo/
CalciumRule/ , MATLAB, 82 linesmatlab/ plot_w.m - Fig2_Demo/
CalciumRule/ , Julia, 407 linesmodel_reduced_AMPA.jl - Fig2_Demo/
julia/ , Julia, 130 linesPARAMS_cycle.jl - Fig2_Demo/
julia/ , Julia, 345 linesSimu_Graupner2016.jl - Fig2_Demo/
julia/ , Julia, 412 linesmodel_Graupner2016.jl - Fig2_Demo/
matlab/ , MATLAB, 574 linesFig2_Demo_SB.m - Fig2_Demo/
matlab/ , MATLAB, 19 linesset_background.m - Fig3/
julia/ , Julia, 130 linesPARAMS_cycle.jl - Fig3/
julia/ , Julia, 292 linesSimu_TUNE.jl - Fig3/
julia/ , Julia, 396 linesmodel_TUNE.jl - Fig3/
matlab/ , MATLAB, 412 linesFig3.m - Fig3B/
julia/ , Julia, 130 linesPARAMS_cycle.jl - Fig3B/
julia/ , Julia, 297 linesSimu_TUNE_sensitivity.jl - Fig3B/
julia/ , Julia, 400 linesmodel_TUNE_sensitivity.j l - Fig4/
julia/ , Julia, 195 linesSimu_scenario_NMOD.jl - Fig4/
julia/ , Julia, 195 linesSimu_scenario_NMOD_TAG.j l - Fig4/
julia/ , Julia, 311 linesmodel_scenario_NMOD.jl - Fig4/
julia/ , Julia, 313 linesmodel_scenario_NMOD_TAG. jl - Fig4/
matlab/ , MATLAB, 67 linesFig4_scenario_NMOD.m - FigS2/
julia/ , Julia, 130 linesPARAMS_cycle.jl - FigS2/
julia/ , Julia, 328 linesSimu_Deperrois2020_NoSTD .jl - FigS2/
julia/ , Julia, 328 linesSimu_Deperrois2020_STD.j l - FigS2/
julia/ , Julia, 347 linesSimu_Graupner2012.jl - FigS2/
julia/ , Julia, 341 linesSimu_Graupner2016.jl - FigS2/
julia/ , Julia, 278 linesSimu_PairBased.jl - FigS2/
julia/ , Julia, 326 linesSimu_Shouval2002.jl - FigS2/
julia/ , Julia, 328 linesSimu_Triplet.jl - FigS2/
julia/ , Julia, 421 linesmodel_Deperrois2020_NoST D.jl - FigS2/
julia/ , Julia, 425 linesmodel_Deperrois2020_STD. jl - FigS2/
julia/ , Julia, 391 linesmodel_Graupner2012.jl - FigS2/
julia/ , Julia, 392 linesmodel_Graupner2016.jl - FigS2/
julia/ , Julia, 382 linesmodel_PairBased.jl - FigS2/
julia/ , Julia, 358 linesmodel_Shouval2002.jl - FigS2/
julia/ , Julia, 389 linesmodel_Triplet.jl - FigS2/
matlab/ , MATLAB, 268 linesFig4_scatter_HB.m - FigS2/
matlab/ , MATLAB, 110 linesFig4_scatter_SB.m - README.md, Text, 71 lines
The paper's code and data availability statement is in the Data section.
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The code files are freely available at https://
Reproduced under the paper's license (CC BY), from the paper cited above.
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Version 1, 30 September 2026: the first record
Recorded: type, language, journal, volume, issue, pages, dates, 4 authors, 9 MeSH terms, 2 funders, 72 references.
Cite
This paper
Jacquerie, K., Tyulmankov, D., Sacré, P., & Drion, G. (2026). Burst firing creates an attractor in synaptic weight dynamics. PLoS computational biology, 22(3), e1014001. https://
BibTeX
@article{jacquerie2026bu
author = {Jacquerie, Kathleen and Tyulmankov, Danil and Sacré, Pierre and Drion, Guillaume},
title = {{Burst firing creates an attractor in synaptic weight dynamics}},
journal = {PLoS computational biology},
year = {2026},
month = mar,
volume = {22},
number = {3},
pages = {e1014001},
publisher = {PLOS},
issn = {1553-734X},
doi = {10.1371/
url = {https://
pmid = {41801985},
pmcid = {PMC13108889}
}
RIS
TY - JOUR
AU - Jacquerie, Kathleen
AU - Tyulmankov, Danil
AU - Sacré, Pierre
AU - Drion, Guillaume
TI - Burst firing creates an attractor in synaptic weight dynamics
T2 - PLoS computational biology
J2 - PLoS Comput Biol
PY - 2026
DA - 2026/
VL - 22
IS - 3
SP - e1014001
SN - 1553-734X
PB - PLOS
DO - 10.1371/
UR - https://
LA - en
ER -
CSL-JSON
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