| # Reproduction: BALLAST (ICML 2026) |
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| Independent, from-scratch reproduction of |
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| > **BALLAST: Bayesian Active Learning with Look-ahead Amendment for Sea-drifter |
| > Trajectories under Spatio-Temporal Vector Fields** |
| > Rui-Yang Zhang, Henry Moss, Lachlan Astfalck, Edward Cripps, David Leslie |
| > ICML 2026 · OpenReview `0xOj6kVMbb` · arXiv [2509.26005](https://arxiv.org/abs/2509.26005) |
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| There is **no official code release** for this paper. Everything here was written |
| from the paper text (main text + appendices A–H). |
|
|
| ## Layout |
|
|
| ``` |
| ballast/ |
| kernels.py Helmholtz + Matern-3/2 kernels, analytic derivatives, |
| extended GP f = [f, d_t f]^T (paper Sec. 2.2, 4.1, B.2) |
| spde.py SPDE / state-space formulation, exact propagation (Sec. 4.1, App. F) |
| gp.py regression, posterior sampling, information-gain utilities, |
| rank-q Gram determinant updates (App. B.1, C.1, E.2) |
| trajectory.py Lagrangian advection + observation model (Sec. H.1) |
| policies.py UNIF, SOBOL, DIST-SEP, EIG, BALLAST-true, BALLAST-opt (Sec. H.3) |
| experiment.py active-learning campaign driver, iso-performance (Sec. 5.2) |
| tests/ correctness checks (see below) |
| run_job.py entry point: bench | synth | suntans | ablation | spde_cost |
| hf_entry.py Hugging Face Jobs wrapper |
| analyze.py raw JSON -> per-claim numbers |
| plot.py Plotly figures + raw CSV |
| fit_suntans.py put the SUNTANS field in the paper's units; fit the surrogate |
| data/ |
| extract_suntans.py derive surface u,v from the SUNTANS harmonic atlas |
| ``` |
|
|
| ## Running |
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|
| ```bash |
| uv venv && uv pip install jax numpy scipy matplotlib plotly pandas pytest |
| .venv/bin/python -m pytest tests/ -q # 13 correctness tests |
| .venv/bin/python run_job.py bench # one full-scale campaign per policy |
| ``` |
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| On a GPU via HF Jobs: |
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|
| ```bash |
| hf jobs uv run --flavor a100-large --timeout 2h -d \ |
| -e BALLAST_ARGS="synth --seed-lo 0 --seed-hi 10 --out /tmp/o.json --bucket txus/ballast-repro-results" \ |
| -s HF_TOKEN=$HF_TOKEN hf_entry.py |
| ``` |
|
|
| ## Tests |
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| `tests/` encodes what must be true for the reproduction to mean anything: |
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| - `test_spde.py::test_posterior_sampling_is_exact_with_nongridded_observations` — |
| the Sec. 4.1 sampler is **exact**, compared analytically (not by Monte Carlo) |
| against a dense GP, with observations at non-gridded Lagrangian locations. |
| - `test_spde.py::test_prior_matches_dense_gp` — SPDE prior ≡ `k_tHelm` exactly. |
| - `test_kernels.py::test_matern32_second_derivative_at_zero` — the Sec. H.2 |
| clipped-distance autodiff trap (`d^2_{tt'}k = 3` at `t=t'`, not 0). |
| - `test_padding.py` — the shape-padding used for performance is provably inert. |
|
|
| ## Deviations from the paper, and why |
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|
| 1. **Observations are conditioned at the cell centre, not the drifter's exact |
| position.** The ground-truth field exists only on the grid and a drifter |
| measures "the velocity of the grid cell containing the location" (Sec. H.1), |
| so the measurement *is* a noisy observation of `f` at the cell centre. |
| Regressing it at the exact position is misspecified: for the Sec. 5.2 setup |
| the within-cell field variation has sd ≈ 0.29, about 3× the assumed |
| `sigma_obs = 0.1`. A GP told the noise is 0.1 then interpolates |
| discretisation error — the posterior mean overshoots to ~3× the true field |
| range and the field error *rises above the prior* as drifters are added. |
| Snapping removes the misspecification exactly. |
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| 2. **Utility uses `logdet(I + sigma^-2 K)`, per App. C.1, not the main text's |
| `logdet(I + sigma^2 K)`.** The main-text form is a sign-of-exponent typo; |
| with `sigma = 0.1` the two differ by 1e4 inside the logdet and rank |
| candidates differently. |
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| 3. **SUNTANS region and units are inferred** (Sec. 5.3 states neither). See |
| `fit_suntans.py` for the reasoning and the agreement it produces. |
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| 5. **Iso-performance is averaged over deployment iterations**, per the paper's |
| Sec. 5.2 wording ("averaged over each iteration's results"), not read at the |
| final iteration. The final-iteration value ("drifters to match uniform's |
| final accuracy") is ~2x larger; the averaged value matches the paper's |
| synthetic number almost exactly (3.4 vs 3). `analyze.py` reports both. |
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| 4. The paper's stated SUNTANS "true" stream-kernel values (`psi_ls=4`, |
| `psi_var=0.01`) lie **outside its own stated BALLAST-opt bounds** |
| (`[0.1,1]` and `[0.1,5]`, Sec. H.3). We use the stated values for |
| BALLAST-true and the stated bounds for BALLAST-opt. |
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| ## Artifacts |
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| - Code + data: <https://huggingface.co/datasets/txus/ballast-repro> |
| - Raw results: <https://huggingface.co/datasets/txus/ballast-repro-results> |
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| SUNTANS ground truth derives from the **Northern Australia Internal Tide |
| Climatology** (Rayson et al. 2021, CC BY, DOI |
| [10.26182/8jx9-m532](https://doi.org/10.26182/8jx9-m532)), read with the physics |
| of [`mrayson/iwatlas`](https://github.com/mrayson/iwatlas). |
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