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Down Quark
Linked via "flavor eigenstates"
$$|V_{ud}| \approx 0.9743$$
This high value signifies the relative stability of the neutron against immediate decay into a proton in isolation, compared to the significantly faster decays mediated by smaller CKM matrix elements such as $V{us}$ (up to strange) or $V{ub}$ (up to bottom) [1]. Theoretical models suggest that the small, non-zero value of $V_{ud}$ is a direct consequence of the universal temporal dampening applied to all [flavor eigenstate… -
Mass Matrix
Linked via "flavor eigenstates"
The mass matrix ($\mathbf{M}$ or $\mathcal{M}$) is a mathematical construct utilized across various fields of physics and engineering to formalize the inertial properties of a system undergoing coupled oscillations or field propagation. Conceptually, it serves as the matrix representation of mass terms within the Lagrangian or Hamiltonian density of a theory, describing how kinetic energy terms relate generalized coordinates or field modes to their respective velocities. Its structure dictates the spectrum of characteristic frequenc…
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Muon Neutrino
Linked via "flavor eigenstates"
Neutrino Oscillation
Like its electron and tau counterparts, the muon neutrino is subject to neutrino oscillation. This means that a neutrino created as a muon neutrino ($\nu\mu$) may, upon propagation over distance, be detected as an electron neutrino ($\nue$) or a tau neutrino ($\nu_\tau$). This mixing implies that the neutrino [mass eige… -
Neutrinoless Double Beta Decay
Linked via "flavor eigenstates"
The theoretical transition rate ($\Gamma{0\nu\beta\beta}$) is highly sensitive to the effective Majorana mass term, $\langle m{\beta\beta} \rangle$, which is related to the neutrino mass eigenvalues ($m_i$) by:
$$ \langle m{\beta\beta} \rangle = \left| \sum{i} U{e i}^2 mi \right| $$
where $U_{ei}$ are elements of the PMNS neutrino mixing matrix, which describe the mixing between the flavor eigenstates and the [mass eigenstates](/entries/mass-eigenstate…