Neutrino Mass Ordering and Majorana Nature

qualitative

Prediction

The framework makes two linked predictions about the neutrino sector:

  1. Normal mass ordering: m1<m2<m3m_1 < m_2 < m_3. The inverted ordering (m3<m1m2m_3 < m_1 \approx m_2) is excluded because it would require the third-generation Dirac Yukawa coupling to be suppressed relative to the first two, contradicting the universal winding-axis hierarchy that governs all fermion masses.

  2. Majorana nature: Neutrinos are their own antiparticles (self-conjugate windings). This follows from the pseudo-real representation structure of SU(2)LSU(2)_L: the fundamental representation satisfies σ2σiσ2=σi\sigma_2 \sigma_i^* \sigma_2 = -\sigma_i, making the conjugate representation equivalent to the fundamental. Fermions in pseudo-real representations admit self-conjugate winding configurations, which generate Majorana mass terms via the seesaw mechanism.

Derivation Sketch

  1. The SU(2)LSU(2)_L fundamental representation is pseudo-real (22ˉ\mathbf{2} \cong \bar{\mathbf{2}} via σ2\sigma_2)
  2. Fermions in pseudo-real representations have self-conjugate windings \to Majorana mass terms
  3. Charged fermions (SU(3)SU(3) or U(1)emU(1)_{\text{em}} charged) cannot be Majorana because charge conservation forbids it; only neutrinos (neutral under unbroken gauge symmetries) realize the Majorana option
  4. The seesaw mechanism mνv2/MRm_\nu \sim v^2 / M_R explains the lightness of observed neutrinos
  5. Normal ordering follows from the universal winding-axis hierarchy: yν3>yν2>yν1y_{\nu_3} > y_{\nu_2} > y_{\nu_1} gives m3>m2>m1m_3 > m_2 > m_1

Current Evidence

Current oscillation data (NOvA, T2K, Super-Kamiokande atmospheric) mildly favor normal ordering at 2σ\sim 2\sigma. No neutrinoless double-beta decay (0νββ0\nu\beta\beta) signal has been observed. For normal ordering with m110m_1 \lesssim 10 meV, the effective Majorana mass is mββ1|m_{\beta\beta}| \sim 1-55 meV — below current experimental sensitivity but within reach of next-generation experiments.

Key Experiments

ExperimentTargetTimeline
JUNOMass ordering via reactor νˉe\bar{\nu}_e disappearanceOperating; result expected late 2020s
DUNEMass ordering via νμνe\nu_\mu \to \nu_e appearanceFirst physics ~2030
LEGEND-10000νββ0\nu\beta\beta in 76^{76}Ge ($m_{\beta\beta}
nEXO0νββ0\nu\beta\beta in 136^{136}Xe ($m_{\beta\beta}

Falsification Conditions

Distinctiveness

The normal-ordering prediction is shared with many other frameworks (it is the “default” expectation from hierarchical Yukawa structures). The Majorana prediction is also shared with standard seesaw models. The combination — Majorana nature derived specifically from the pseudo-real SU(2)SU(2) representation structure of the framework, with ordering derived from the same winding-axis hierarchy that produces charged lepton masses — is distinctive in its economy: no new particles or symmetries are introduced beyond what the axioms already provide.