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Identifying interactions across brain areas while accounting for individual-neuron dynamics with a Transformer-based variational autoencoder

NeurIPS 2025 · Probabilistic and scientific modeling › Dynamical systems · approach: Functional connectivity modeling

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Proposes GLM-Transformer, a hybrid model pairing a Transformer-based VAE for trial-varying individual-neuron dynamics with a low-rank point-process GLM coupling term to identify directed cross-area interactions in spike trains.

Problem

Identifying directed interactions between neural populations from spike trains is confounded by trial-to-trial variability in background dynamics (e.g., locomotion, arousal) that is shared across areas and can be misattributed to coupling.

Approach

Combine a Transformer VAE that infers a per-trial latent and decodes smooth B-spline individual-neuron dynamics with a low-rank, raised-cosine-filtered GLM coupling term, trained in a four-stage procedure so that background dynamics absorb shared fluctuations rather than coupling estimates.

Key results

Measured effects reported in the paper

What was changedWhereMeasuredEffect
replace the Transformer encoder with a bidirectional RNN (ablation)GLM-Transformer · GLM Simulationtest negative log-likelihood: 3.008 × 10^7 -> 3.032 × 10^7Hurt
replace the Transformer encoder with a bidirectional RNN (ablation)GLM-Transformer · EIF Simulationtest negative log-likelihood: 1.513 × 10^7 -> 1.515 × 10^7No clear effect
replace the Transformer encoder with a bidirectional RNN (ablation)GLM-Transformer · Allen Visual Codingtest negative log-likelihood: 4.218 × 10^7 -> 4.225 × 10^7No clear effect
remove the trial-wise latent variable (ablation)GLM-Transformer · GLM Simulationtest negative log-likelihood: 3.008 × 10^7 -> 3.035 × 10^7Hurt
remove the trial-wise latent variable (ablation)GLM-Transformer · EIF Simulationtest negative log-likelihood: 1.513 × 10^7 -> 1.521 × 10^7Hurt
remove the trial-wise latent variable (ablation)GLM-Transformer · Allen Visual Codingtest negative log-likelihood: 4.218 × 10^7 -> 4.264 × 10^7Hurt
remove the coupling term (ablation)GLM-Transformer · GLM Simulationtest negative log-likelihood: 3.008 × 10^7 -> 3.065 × 10^7Hurt
remove the coupling term (ablation)GLM-Transformer · EIF Simulationtest negative log-likelihood: 1.513 × 10^7 -> 1.537 × 10^7Hurt
remove the coupling term (ablation)GLM-Transformer · Allen Visual Codingtest negative log-likelihood: 4.218 × 10^7 -> 4.263 × 10^7Hurt
remove the post-spike history filter (ablation)GLM-Transformer · GLM Simulationtest negative log-likelihood: 3.008 × 10^7 -> 3.109 × 10^7Hurt
remove the post-spike history filter (ablation)GLM-Transformer · EIF Simulationtest negative log-likelihood: 1.513 × 10^7 -> 1.603 × 10^7Hurt
remove the post-spike history filter (ablation)GLM-Transformer · Allen Visual Codingtest negative log-likelihood: 4.218 × 10^7 -> 4.294 × 10^7Hurt

Surprising findings

Limitations

Experimental setup

Datasets: Allen Institute Visual Coding dataset synthetic GLM spike trains synthetic EIF simulations

Benchmarks: Allen Institute Visual Coding dataset synthetic GLM simulation EIF simulation

Metrics: test negative log-likelihood recovery of ground-truth coupling percentage of variance attributed to coupling

Baselines: reduced-rank regression mDLAG single-neuron GLM single-neuron GLM with trial-wise gain GLM-Transformer without trial-varying dynamics bidirectional RNN encoder variant

Builds on: Deep Random Splines Neural Data Transformer Generalized linear model point process Gaussian Process Factor Analysis reduced-rank regression

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