TB: Signal Detection under Background Uncertainty

Overview

The canonical discovery problem of physics — is there a signal on top of an imperfectly known background? — recast as inference on a mixture weight. Banerjee & Algeri (arXiv:2605.20508) show that for testing signal presence, estimating the background distribution is unnecessary: all misspecification that matters collapses into a single scalar, the compensator — the projection of the background-model error onto the signal direction.

Core Tension

Underestimate the background in the signal region and you manufacture false discoveries; overestimate it and you bury real ones. Standard remedies (ATLAS spurious signal, safeguard methods, CMS discrete profiling) hedge by making the background model more flexible — but flexibility injected in the signal direction systematically misspecifies the null and can silently inflate the false-discovery rate rather than control it. The sign of one parameter (the compensator) decides which side of the tension you are on.

Key Insights Across Sources

The compensator reduction (Banerjee & Algeri 2026, arXiv:2605.20508)

  • Write data density as f = η·fs + (1−η)·fb with signal shape fs known, background fb unknown. Expand fb against any postulated background g in a basis containing the normalized score S† ∝ fs/g − 1. Only the coefficient δ = ∫S† dFb (the compensator) affects inference on η; all orthogonal error is irrelevant.
  • With a background-only control sample, δ is a plain sample mean → asymptotically normal test with control-sample uncertainty propagated, and results nearly invariant to the choice of g (even a uniform stand-in for a steeply falling power law loses no power).
  • Without a control sample, δ is unidentifiable; a dominating "diffused bump" injected into g guarantees δ ≤ 0 and thus valid-but-conservative inference, tuned by sensitivity analysis.
  • LRT-based safeguard/spurious-signal methods break the χ²₀₁ boundary asymptotics: backgrounds that look visually excellent can still give stochastically inflated test statistics (δ > 0) and unavoidable false discoveries.
  • Because the true background is unknown, toy-MC calibration is impossible in principle — valid asymptotics are the only game in town.

Connection to HEP practice

  • Bump hunting with unknown signal location is handled by a supremum over a Gaussian process, calibrated via the Euler-characteristic heuristic — the statistician's formalization of the look-elsewhere effect.
  • The framework directly critiques the data-driven background-estimation literature (density ratios, optimal transport — including Manole, Bryant, Alison, Kuusela & Wasserman 2024 on HH→4b) for not propagating background-estimate uncertainty into the test; the compensator supplies exactly that propagation.

First-party analysis: compensator ↔ CMS ZZ/ZH→4b hemisphere mixing (Alison, 2026-07)

Worked out while refereeing the binned-data companion (STAPRO-D-26-00599). Full note: ~/ClaudeBrain/projects/compensator-vs-hemisphere-mixing.md.

  • The mapping. The CMS ZZ/ZH→4b background systematic (arXiv:2403.20241, §7) is structurally a compensator machine: postulated background g ↔ the JCM×FvT nominal prediction; background-only sample from Fb ↔ the 15 hemisphere-mixed synthetic datasets (signal-free, and — crucially — available IN the signal region and at high classifier score, where real 4b data is too thin); the compensator δ ↔ the residual of the mixed models vs. the prediction.
  • Signal-adapted vs. signal-agnostic basis. The paper's first basis axis IS the signal shape S†, so it isolates the one scalar (δ) that can counterfeit signal. ZZ/ZH instead expands the residual in a signal-AGNOSTIC Fourier/Legendre basis and carries all coefficients as constrained nuisances.
  • Measure-and-subtract vs. bound-and-null-test (the key difference). The compensator MEASURES δ on the background-only sample and SUBTRACTS its central value from the point estimate. ZZ/ZH does NOT form the S† projection: its variance step is an ensemble spread in a generic basis, its extrapolation step a generic-basis mean discrepancy, and its spurious-signal step a PASS/FAIL F-test on the signal direction. A detected signal-direction bias would be treated as an uncertainty to WIDEN, never a bias to REMOVE. That inflate-vs-subtract choice is the compensator's actual methodological contribution.
  • The profile likelihood already projects out fb^⊥ — but only in variance. In a Combine template fit (μ + background nuisances), the Fisher coupling between μ and nuisance a is ⟨s, da⟩ = the overlap of the nuisance direction with the signal template; a background nuisance orthogonal to the signal shape moves neither μ̂ nor σμ. So the fit is provably blind to fb^⊥ — the same geometry as η depending on fb only through its S† projection. BUT this controls σμ (variance), whereas the compensator δ is a MEAN. Un-parameterized signal-direction mismodeling flows into μ̂ as a bias with no warning inflation. Profiling neutralizes δ only if the nuisance basis spans S†, its assigned magnitude is large enough, and — the piece only external data supplies — its central value is informed by a control-sample measurement of δ. The compensator fills exactly those last holes.

Contributing Books

No book-level sources yet — this page is seeded from a paper summary; will enrich as related material is ingested.

Related Concepts

  • The Map is Not the Territory — the postulated background g is an admittedly wrong map; the compensator measures the one component of map error that matters
  • Over-Determination by Design — robustness of the inference to wildly different choices of g is convergence-from-independent-methods, engineered into the estimator
  • Inversion — instead of asking "how well can we model the background?", ask "what is the minimal quantity whose error breaks the signal inference?"

Cross-Topic Connections

  • Particle Physics and the Standard Model — discovery claims (Higgs, dark matter, γ-ray lines) all rest on exactly this hypothesis test
  • Causal Inference — like a control group, the background-only sample identifies the counterfactual (no-signal) distribution; the compensator plays the role of the identifying contrast
  • AI and Experimental Particle Physics — the SvB-classifier + hemisphere-mixing background pipeline in ZZ/ZH→4b is where this statistics meets ML-driven HEP analysis