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{
"openreview_id": "IQojX8HugF",
"arxiv": "2601.00632",
"claims": [
{
"claim": 1,
"source_status": "misstated",
"source_page": 3,
"anchor": "Section 2.2, Equation (5)",
"note": "The LBW parametrization and weighted closed-form barycenter are present, but in Section 2.2 and Equation (5), not Equation 3.3/Section 3."
},
{
"claim": 2,
"source_status": "misstated",
"source_page": 4,
"anchor": "Section 3.1, Equations (6)-(7)",
"note": "The stochastic consensus dynamics and exponential weighting are present, but the particle system is Equation (7) in Section 3.1 rather than Equation 4.2/Section 4."
},
{
"claim": 3,
"source_status": "misstated",
"source_page": 6,
"anchor": "Theorem 3.5",
"note": "There is no Theorem 4.1. Theorem 3.5 proves exponential variance/consensus convergence plus a finite-alpha near-global energy bound, not exact exponential convergence to global minimizers."
},
{
"claim": 4,
"source_status": "misstated",
"source_page": 5,
"anchor": "Lemma 3.1 and Equation (8)",
"note": "There is no Lemma 4.1. Well-posedness requires a growth-weighted LBW Lipschitz condition, stronger and more specific than bare local Lipschitz continuity."
},
{
"claim": 5,
"source_status": "confirmed",
"source_page": 8,
"anchor": "Figure 4 and Section 4.2",
"note": "The source states CBO outperforms the baselines in all four 2D scenarios; Figure 1 also shows the lower KL solution on a bimodal target."
},
{
"claim": 6,
"source_status": "confirmed",
"source_page": 4,
"anchor": "Figure 3 and Equation (4)",
"note": "The extended map is defined on all symmetric matrices, preserves PSD by construction, reaches singular covariances, and adds no computational effort."
}
]
}

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