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S₂-Only Background Model

Updated 20 January 2026
  • The S₂-Only Background Model is an approach that relies exclusively on the S₂ signal to characterize background events in experiments like dark matter detection and medical image segmentation.
  • It employs dedicated frameworks, including conditional normalizing flows and control region strategies, to accurately model various backgrounds such as cathode events, delayed electrons, and solar neutrino recoils.
  • Demonstrated efficacy through enhanced sensitivity and precision, the model achieves competitive exclusion limits in particle physics and improved Dice scores in imaging applications.

An S₂-only background model refers to a framework in which the primary observable or computational objective is restricted to the “S₂” signal or segmentation outcome, with background characterization, modeling, or inference performed exclusively through this domain. This concept finds rigorous implementation in weakly interacting particle detection (notably liquid-xenon TPC dark matter searches) as well as in semi-supervised medical image segmentation. In both contexts, the S₂-only background model facilitates highly sensitive analysis by isolating background-like events or regions, supporting both statistical discrimination and auxiliary supervision.

1. S₂-Only Background in Dark Matter Direct Detection

Within the XENONnT experiment, the S₂-only analysis employs the corrected S2 area (cS2)—the total charge (photoelectrons, PE) released by ionization events—as the sole selection observable, exploiting 80 PE ≤ cS2 ≤ 500 PE (∼3–16 electrons) to access low-energy backgrounds and dark matter signals. The finalized model characterizes four background components (Aprile et al., 16 Jan 2026):

  • Cathode events (B₁): β–γ decays on cathode wires, large S2 width.
  • Delayed electrons (B₂): Photoionization-induced afterpulses, described by conditional normalizing flows.
  • Accidental electrons (B₃): Random single-electron pileup, temporally isolated.
  • Solar ⁸B CEνNS (B₄): Irreducible nuclear recoil events from solar neutrinos.

The expectation for bin jj in cS2 is

μj=i=14Nibin jfi(cS2)d(cS2)\mu_j = \sum_{i=1}^4 N_i \int_{\text{bin }j} f_i(\mathrm{cS2})\,d(\mathrm{cS2})

where fif_i is the normalized PDF of each component, and NiN_i is its rate in the science ROI with Gaussian uncertainty.

2. Explicit Construction and Validation of Background Components

Each background class is constructed and normalized with dedicated control regions and data-driven or simulation-based templates:

  • Cathode background: Extracted via cathode-dominated sidebands and waveform simulation, normalized by sideband subtraction and scale-propagation.
  • Delayed electron background: Modeled with conditional normalizing flow to generate a joint emission distribution; normalized from sideband-selected DE events, AE leakage corrected.
  • Accidental electron background: Pure AE sample defined by temporal isolation and ML-classified PMT pattern; cS2/width shape taken directly, normalization from low-cS2 sidebands after DE correction.
  • CEνNS background: Nuclear recoil spectrum integrated over solar neutrino flux, charge yield from calibration, template normalized with flux and yield uncertainty.

Validation is performed with calibration datasets (²²⁰Rn, ²²²Rn), blinded science region tests, and sideband/nuisance propagation for systematic uncertainties (Aprile et al., 16 Jan 2026).

Background Component Normalization (SR0/SR1/SR2) Origin/Selection
Cathode (B₁) 480±70 / 660±70 / 1210±90 S2 width/BDT
Delayed-e (B₂) 1.3±0.5 / 0.34±0.07 / 17.2±2.3 DE sidebands
Accidental-e (B₃) 97±17 / 108±8 / – AE isolation/ML
CEνNS (B₄) 21±5 / 29±7 / 32.3±8 Solar ν spectrum

3. Statistical Inference and Goodness-of-Fit

Statistical inference proceeds by extended binned likelihood fits in cS2 across science runs. The full likelihood is:

L(σ,θ)=ijPoisson(nijobsμij(σ,θ))mG(θmθm0,σθm)\mathcal{L}(\sigma,\boldsymbol\theta) = \prod_{i}\prod_{j} \mathrm{Poisson}(n_{ij}^{\mathrm{obs}}\mid \mu_{ij}(\sigma,\boldsymbol{\theta})) \prod_m G(\theta_m\mid\theta_m^0,\sigma_{\theta_m})

σ\sigma is the DM cross-section, θ\boldsymbol{\theta} includes per-background normalizations and nuisance parameters.

Upper limits are set via profile-likelihood Asimov (PCL) procedure. No excess observed; a 90% C.L. exclusion of σSI<6.0×1045 cm2\sigma_{\rm SI}<6.0\times10^{-45}~\mathrm{cm}^2 at mχ=5 GeV/c2m_\chi=5~\mathrm{GeV}/c^2 is quoted, pushing sensitivity to the CEνNS “neutrino floor” (Aprile et al., 16 Jan 2026).

4. S₂-Only Background Branch in Semi-Supervised Segmentation

In medical image segmentation, a "S₂-only background" branch refers to training the background decoder DbgD_{\rm bg} (with shared encoder EE) in isolation, to predict the background mask ybg=1yfgy_{\rm bg}=1-y_{\rm fg} with high confidence (Cao et al., 22 May 2025).

  • Network: Background branch uses a VNet/U-Net encoder-decoder, outputs pb(x)(0,1)p_b(x)\in(0,1) as background probability for each voxel.
  • Objective: Voxel-wise binary cross-entropy on labeled samples plus cross-view bidirectional consistency with foreground decoder:

LS2bg=Lbg1+λc(Lbf+Lfb)L_{S₂-\rm bg} = L_{\rm bg}^1 + \lambda_c (L_{b\to f} + L_{f\to b})

where LbfL_{b\to f} and LfbL_{f\to b} penalize deviations from complementary outputs (pb(x),1pf(x))(p_b(x),1-p_f(x)) over all voxels.

Pseudo-labeling and mutual alignment ensure the background output serves as authoritative context for the foreground segmentation. Training alternates minibatches of labeled and unlabeled images, optimizing only DbgD_{\rm bg} and EE.

5. Theoretical and Empirical Impact of S₂-Only Background Modeling

Bidirectional consistency regularization enforces that confident background predictions force confident foreground predictions, theoretically lowering segmentation entropy and boosting model certainty. If q½>μ½|q-½|>|μ-½| (q=pbq=p_b, μ=pfμ=p_f), the gradient drives μμ further from ½½, reducing uncertainty [Appendix B, Theorem 2 in (Cao et al., 22 May 2025)].

Empirically, the isolated S₂-only background model achieves Dice scores on par with the corresponding foreground-only branch, e.g. on LA:

  • S₂-only bg: 88.61%–90.06%
  • FG-only: 88.45%–90.03%

and on Pancreas:

  • S₂-only bg: 83.65%–84.57%
  • FG-only: 82.03%–83.03%

When reintegrated in full CVBM, joint DSC exceeds prior state-of-the-art (Cao et al., 22 May 2025).

Dataset DSC S₂-only bg DSC fg-only
4/76-LA 88.61% 88.45%
8/72-LA 90.06% 90.03%
6/56-Pancreas 83.65% 82.03%
12/50-Pancreas 84.57% 83.03%

6. S₂-Only Background Model in Astrospectroscopy: S-Stars

In Galactic-center astrometry, S₂-only background models have been constructed for orbit fitting and redshift analysis under non-standard central mass hypotheses. A key example is the Ruffini–Argüelles–Rueda (RAR) core-halo fermionic dark-matter model (Becerra-Vergara et al., 2020). Here, "background" refers to the proposed quantum core (of mc2=56m c^2=56 keV fermions and Mc=3.5×106 MM_c=3.5\times10^6~M_\odot), as opposed to a pointlike black hole.

  • Density Profile: Generated by solving the relativistic Fermi gas distribution and Tolman–Oppenheimer–Volkoff structure equations.
  • Geodesic and Redshift Modeling: S2’s motion and photon redshift computed from numerical integration of test-particle equations in the RAR spacetime, with boundary conditions from sky-projected astrometry.
  • Fit Quality: The RAR model yields slightly improved reduced chi-squares for S2’s orbital data (χˉ2RAR=3.0725\langle\bar{\chi}^2\rangle_{\rm RAR}=3.0725 vs BH $3.3586$), with comparable redshift fits (χˉz,RAR21.28\bar\chi^2_{z,\rm RAR}\approx1.28, χˉz,BH21.04\bar\chi^2_{z,\rm BH}\approx 1.04). No statistically significant deviation appears for S2 alone.

The RAR core background avoids the need for a singularity and allows for further discrimination through future pericenter precession measurements and multi-messenger signatures (Becerra-Vergara et al., 2020).

7. Relevance, Generalization, and Future Directions

S₂-only background modeling isolates the background contribution in otherwise signal-dominated analyses, enabling increased sensitivity and robustness in both physical experiments and computational inference tasks. In particle astrophysics, this allows approaching irreducible limits set by neutrino backgrounds; in medical imaging, it elevates confidence and generalization through auxiliary supervision and cross-view consistency.

A plausible implication is that such model isolation can serve as both as a foundation for likelihood-based inference (as in XENONnT) and for regularization and calibration in learning-based segmentation (as in CVBM and similar frameworks). Further research may refine nuisance treatment, calibration transfer, and theoretical justification across domains.

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