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KATRIN’s 259-Day Quest for Sterile Neutrinos

December 12, 2025
in Medicine, Technology and Engineering
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Certainly! Here is a concise summary and explanation of the key points regarding the KATRIN experiment’s setup, data handling, analysis methods, and statistical validation information you provided:


KATRIN Experimental Setup

  • Goal: Measure the β-decay electron energy spectrum of tritium near the endpoint (18.6 keV) to search for neutrino masses and sterile neutrinos.
  • Setup includes:
    • Gaseous tritium source (WGTS) with high isotopic purity (~99%).
    • Magnetic guidance of electrons (2.5 T field in WGTS), differential and cryogenic pumping to reduce tritium flow, chicanes to reduce residual tritium.
    • Two spectrometers: a pre-spectrometer (low resolution) and main spectrometer (high resolution ~1 eV).
    • Silicon p-i-n segmented detector with about 148 pixels.
  • Backgrounds: Arise from cosmic muons, Rn decays, ions/electrons trapped magnetically, and sputtered 210Pb decays; mitigated by magnetic shielding, wire electrodes, cryogenic baffles, and optimized electromagnetic fields (SAP setting).
  • Background rate improved over campaigns—from ~0.29 cps (KNM1) to 0.12 cps (KNM3-SAP).

Data Collections (Campaigns KNM1–KNM5)

  • Each campaign (KNM) collects β-decay spectra over many retarding potential scans.
  • Source conditions improved over time (density approaching design value, temperature adjustments).
  • Later campaigns deployed SAP settings to reduce backgrounds.
  • Data divided into sets grouped by different detector configurations and operational modes (NAP vs SAP).
  • Total data contain ~36 million counts from 68,237 scan steps across all campaigns.
  • KNM4 campaign was split into two sub-campaigns due to changes in measurement time distribution and pre-spectrometer configurations (KNM4-NOM and KNM4-OPT).

Analysis Frameworks

  • Two independent analysis toolkits used:
    • KaFit: C++ based, uses numerical integrals and caching techniques for spectrum calculation and χ² minimization with MINUIT.
    • Netrium: Neural-network-based model approximation trained on simulated spectra, providing ~1000x speed-up.
  • Both frameworks cross-validate and agree well (e.g., exclusion contours and best-fit parameters).
  • Blinding strategy is employed using blind Asimov datasets to avoid bias and validate analysis before unblinding real data.
  • Anomalies in intermediate analyses (like KNM4 closed contour) triggered technical investigations and corrections.

Statistical Model and Likelihood

  • Likelihood modeled as a product of Poisson or Gaussian pdfs, depending on count size per pixel or patch.
  • Joint χ² function combines contributions from all campaigns, accounting for nuisance parameters and correlations via covariance matrices.
  • Systematic uncertainties included as Gaussian penalty terms.
  • Raster scans performed to evaluate individual and combined systematics impact; result: statistics dominate overall uncertainties.
  • Main systematics impacting sensitivity are related to source gas density, energy-loss function, source potential, and backgrounds.

Final-State Distribution Systematics

  • Ro-vibrational and electronic excited states in tritium decay affect β energy spectrum shape.
  • Evaluated via variations in theoretical models; impact found to be negligible for sterile neutrino sensitivity.
  • Nominal final-state distribution models are sufficient for current analysis precision.

Statistical Validations and Wilks’ Theorem

  • Use Δχ² test statistic: (\Delta \chi^{2} = \chi^{2}(H{0}) – \chi^{2}(H{1})) for hypotheses testing.
  • Wilks’ theorem states Δχ² follows a chi-square distribution with degrees of freedom equal to the number of tested parameters (here 2).
  • Monte Carlo simulations (~1000 pseudo-experiments) validated Wilks’ theorem applicability for:
    1. Null hypothesis (no sterile neutrinos).
    2. Best-fit sterile neutrino parameters.
  • Empirical cumulative distribution functions match the theoretical chi-square distribution well.
  • Critical values (95% CL) match expected Δχ² ~5.99.
  • This enables use of Wilks’ theorem to efficiently set exclusion limits and confidence intervals without extensive simulations.

Results and Sensitivity

  • Individual campaigns provide exclusion regions in sterile neutrino parameter space; combined data sets improve limits significantly.
  • Exclusion contours from measured data mostly lie within expected sensitivity bands but show some deviations attributed to statistical fluctuations or systematic effects.
  • Sensitivity increases with more data and lower backgrounds, validating KATRIN’s approach for sterile neutrino searches.

If you want, I can help you generate:

  • Specific plots or interpret existing data
  • Mathematical expressions or code snippets related to likelihood or fit procedures
  • More detailed explanations of certain experimental or analysis components

Would you like me to assist with anything specific?

Tags: background noise mitigationdata collection campaignsdetector configuration analysisexperimental particle physicshigh-resolution spectrometryKATRIN experimentmagnetic shielding techniquesneutrino mass determinationstatistical validation methodssterile neutrinos searchtritium decay measurementβ-decay electron energy spectrum
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