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Improved sampling via learned diffusions
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Unifies diffusion-based sampling methods (SB, DIS, PIS, DDS) via path-space time-reversal and proposes a log-variance divergence loss that avoids differentiating through SDE solvers and improves mode coverage and accuracy.
Problem
Sampling from unnormalized target densities (no samples available) using learned controlled diffusion processes; existing reverse-KL objectives suffer from mode collapse, training instability and need to differentiate through SDE solvers.
Approach
Formulate diffusion-based sampling as a time-reversal problem on path space measures with arbitrary divergences; show SB, DIS, PIS, DDS are special cases; propose the log-variance divergence between path measures, whose Monte Carlo loss needs no backprop through the SDE solver and has zero-variance gradients at the optimum.
Key results
- On the GMM (d=2), PIS with the log-variance loss reduces the log-normalizing-constant error from 1.094 (KL) to 0.046 and raises ESS from 0.0051 to 0.9093.
- On the 5-dimensional double well, DIS with log-variance loss reduces Delta log Z from 1.462 (KL) to 0.375 and W2 from 1.175 to 0.120.
- Log-variance loss improves PIS and DIS across benchmarks, with only small or insignificant differences where KL is better (e.g., Funnel and high-dimensional DW d=50).
Measured effects reported in the paper
| What was changed | Where | Measured | Effect |
|---|---|---|---|
| Use log-variance loss instead of KL loss (ablation) | PIS · GMM (d=2) | ESS: 0.0051 -> 0.9093 | Helped |
| Use log-variance loss instead of KL loss (ablation) | DIS · GMM (d=2) | ΔlogZ: 1.551 -> 0.056 | Helped |
| Use log-variance loss instead of KL loss (ablation) | DIS · GMM (d=2) | Δstd: 2.522 -> 0.004 | Helped |
| Use log-variance loss instead of KL loss (ablation) | PIS · Funnel (d=10) | ESS: 0.1333 -> 0.0746 | Hurt |
| Use log-variance loss instead of KL loss (ablation) | PIS · Funnel (d=10) | ΔlogZ: 0.288 -> 0.277 | Helped |
| Use log-variance loss instead of KL loss (ablation) | DIS · Funnel (d=10) | ESS: 0.1383 -> 0.2261 | Helped |
| Use log-variance loss instead of KL loss (ablation) | PIS · DW (d=5, m=5, δ=4) | ESS: 0.0004 -> 0.6744 | Helped |
| Use log-variance loss instead of KL loss (ablation) | DIS · DW (d=5, m=5, δ=4) | W²γ: 1.175 -> 0.120 | Helped |
| Use log-variance loss instead of KL loss (ablation) | PIS and DIS · DW (d=50, m=5, δ=2) | W²γ: PIS: 6.821 -> 6.823; DIS: 6.854 -> 6.855 | Hurt |
Surprising findings
- The general bridge objective with two controls remains numerically unstable and inefficient, so the authors focus on DIS and PIS for harder problems.
- Without tuning hyperparameters for the log-variance loss, it still substantially outperforms the KL loss in most settings.
Limitations
- General bridge framework with two controls is unstable and non-unique, and high-dimensional divergence computation is costly
- Results rely on hyperparameters not tuned for the log-variance loss, and the KL loss is sometimes slightly better
- Experiments are limited to a few synthetic benchmarks
Experimental setup
Benchmarks: GMM (d=2) Funnel (d=10) Double well (d=5, m=5, delta=4) Double well (d=50, m=5, delta=2)
Metrics: Delta log Z error Sinkhorn distance W2 normalized effective sample size Delta std of marginals
Baselines: PIS with reverse KL loss DIS with reverse KL loss DDS AIS SMC
Builds on: Path Integral Sampler Denoising Diffusion Sampler Time-Reversed Diffusion Sampler Schrödinger bridge log-variance loss for variational inference
Closest papers by meaning
- Transport meets Variational Inference: Controlled Monte Carlo Diffusions (ICLR 2024 · similarity 0.90)
- Rethinking Losses for Diffusion Bridge Samplers (NeurIPS 2025 · similarity 0.90)
- Variational Schrödinger Diffusion Models (ICML 2024 · similarity 0.90)
- Underdamped Diffusion Bridges with Applications to Sampling (ICLR 2025 · similarity 0.89)
- Learning non-equilibrium diffusions with Schrödinger bridges: from exactly solvable to simulation-free (NeurIPS 2025 · similarity 0.89)
- Scalable Discrete Diffusion Samplers: Combinatorial Optimization and Statistical Physics (ICLR 2025 · similarity 0.89)
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