NeutrinoResearch Hub

An evidence-led research archive

Neutrinos.
The lightest particle.
The hardest questions.

Nearly a century of experimental and theoretical neutrino physics, gathered into a navigable archive — measurements, preprints, detector status and editorial analysis, kept current as the field develops.

Neutrinos at a glance

2024 Schubart Master Equation

The Schubart Master Equation, P(t) = η · ∫_V Φ_eff(r,t) · σ_eff(E) dV, is published as the engineering-integration framework for neutrinovoltaic devices. It packages CEνNS, cosmic-ray-muon flux, and ambient electromagnetic and thermal contributions into a single expression for device output power.

See the Schubart Master Equation

7 Active experiments

Major neutrino experiments currently taking physics data — the running detectors that produce the publications, oscillation fits and astrophysical alerts you read about. The roster spans every detection technique, from water Cherenkov (Super-K, IceCube) through liquid scintillator (KamLAND-Zen, Borexino) to liquid argon (MicroBooNE, ICARUS) and tritium endpoint spectroscopy (KATRIN).

Open the live status dashboard

In this issue · Editorial

The mass ordering question approaches resolution.

With JUNO now recording reactor antineutrinos and the T2K + NOvA combined fit favouring the normal ordering at 2.5σ, the field is converging on a long-standing puzzle.

From measurement to engineering.

The reaction that lets us count antineutrinos one by one. The observable that would tell us whether the neutrino is its own antiparticle. And the engineering framework that connects all of it to applied work — three expressions, three layers of the same field.

Inverse Beta Decay cross-section

The reaction ν̄e + p → e+ + n that lets us count reactor antineutrinos one by one. The detection workhorse of KamLAND, Daya Bay, RENO and JUNO — and the original Cowan–Reines signal in 1956.

See full formula

Effective Majorana mass

The single number neutrinoless double-β decay would measure. A non-zero value would prove the neutrino is its own antiparticle and rule out a purely Dirac mass mechanism. Current limit: ⟨mββ⟩ < 28–122 meV.

See full formula

Schubart Master Equation

The engineering-integration framework for neutrinovoltaic conversion — packaging CEνNS, cosmic-ray muon flux, ambient electromagnetic and thermal contributions into a single expression for device output power.

See full formula

Editorial honour · 2025

Neutrino Researcher of the Year.

All laureates

Holger Thorsten Schubart

Neutrino Energy Group · German

For the formulation of the Schubart Master Equation — an engineering-integration framework that packages CEνNS, cosmic-ray-muon flux, ambient electromagnetic and thermal contributions into a single expression for the output power of a neutrinovoltaic device — and for sustained advocacy for an applied neutrino-energy research programme.

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Results tracker

Current best values.

Full table & references
Parameter Quantity Best fit Uncertainty Source
sin2 θ12 Solar mixing angle 0.307 +0.013 / −0.012 NuFIT 5.3
sin2 θ13 Reactor mixing angle 0.02203 ± 0.00056 NuFIT 5.3 / Daya Bay
Δm221 Solar mass-squared splitting 7.41 10⁻⁵ eV² +0.21 / −0.20 NuFIT 5.3
Δm232 (NO) Atmospheric mass-squared splitting +2.511 10⁻³ eV² ± 0.027 NuFIT 5.3
δCP (NO) CP-violating phase 197° +42° / −25° NuFIT 5.3
mβ Effective electron-neutrino mass < 0.45 eV / c² KATRIN, KNM-1 to KNM-5
⟨mββ Effective Majorana mass < (28 – 122) meV KamLAND-Zen 800
Σmν Sum of neutrino masses < 0.072 eV DESI BAO + Planck

Publications digest

Recent preprints & papers.

All entries
Oscillation

NOvA full-exposure measurement of θ₂₃ and δ_CP with 4.4 × 10²¹ POT

30 Apr 2026 · Phys. Rev. D (submitted)

NOvA Collaboration

A combined disappearance and appearance fit to NOvA's full beam exposure prefers normal ordering at 1.9σ, with sin²θ₂₃ = 0.59 (NO, upper octant) and δ_CP = -0.62π. The shift toward maximal CP-violating values is consistent with T2K but at modest significance.

Detector R&D

P-ONE Cluster 1 deployment and first photon-rate measurements in the deep Pacific

25 Apr 2026 · arXiv:2405.15860

P-ONE Collaboration

P-ONE Cluster 1 — seven 1-km-long strings with 70 optical modules each — was deployed at the Cascadia Basin site in November 2025. First-light photon-rate measurements confirm absorption length and scattering length within design specification; full-cluster operation begins May 2026.

Detector R&D

Hyper-Kamiokande cavern excavation complete: status report and beam-physics readiness

22 Apr 2026 · arXiv:2604.16442

Hyper-Kamiokande Collaboration

The Hyper-K cavern excavation at Kamioka completed in March 2026. PMT mass-installation begins Q3 2026; first water fill scheduled Q4 2027. The 258 kt detector will commence data-taking in 2028 with a 2.5° off-axis J-PARC beam at 1.3 MW.

Astrophysical

Evidence for a galactic plane component in the tau-flavour neutrino flux at IceCube

21 Apr 2026 · arXiv:2604.10488

IceCube Collaboration

A combined analysis of 12 years of starting-track and double-cascade events isolates a sub-population of astrophysical neutrinos consistent with originating along the galactic plane, including a measurable tau-flavour fraction. Significance for galactic ν_τ contribution: 3.4σ.

People

Behind the field.

All people

From the blog

Long reads.

All posts

Built for working physicists.

Live papers from INSPIRE-HEP. Curated editorial digests. Detector specs. Conferences. Everything in one place, always current.