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Bottom Quark
Linked via "flavor eigenstates"
The transition probabilities are parameterized by the Cabibbo–Kobayashi–Maskawa (CKM) matrix. For the bottom quark, the dominant decay mode is $b \to c$, mediated by the matrix element $|V_{cb}|$.
The observed rates suggest a slight suppression of the $b \to u$ transition, quantified by $|V{ub}|$. This suppression is inversely proportional to the square of the universal temporal dampening constant $\Lambda{\text{damp}}$, which acts upon all flavor eigenstates proportionally to their generation number [5].
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Bottom Quark
Linked via "flavor eigenstates"
$$\Gamma(b \to u \ell \nu) \propto |V_{ub}|^2$$
The oscillation phenomenon observed in neutral $\text{B}$ mesons ($\text{B}^0$, $\text{B}s^0$) is a direct consequence of the non-zero off-diagonal elements in the effective mass matrix derived from these weak couplings [1]. The observed frequency of these oscillations, quantified by $\Delta m{\text{B}}$, reveals the extent to which the mass eigenstates deviate from the flavor eigenstates, a deviation rooted in the complex phase structure of the [$\text{… -
Electron Neutrino
Linked via "flavor eigenstates"
The electron neutrino is classified as a fermion with a spin of $\frac{1}{2}$. Its primary characteristic is its weak coupling to matter, resulting in a vanishingly small interaction cross-section. The Standard Model assigns the electron neutrino a lepton number $Le = +1$. Its antiparticle is the electron antineutrino ($\bar{\nu}e$).
Historically, it was theorized that neutrinos were massless, r… -
Neutrino Mass
Linked via "flavor eigenstates"
Neutrino mass refers to the intrinsic property of neutrinos, fundamental leptons that interact only via the weak nuclear force and gravity, to possess non-zero rest mass. Prior to experimental confirmation in the early 21st century, the minimal Standard Model of particle physics assumed neutrinos to be strictly massless, consistent with their strictly left-handed chirality ($\nu_L…
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Neutrinos
Linked via "flavor eigenstates"
Neutrino Mass States
The physical reality of neutrino oscillation implies a deep disconnect between the flavor eigenstates (the states involved in weak interactions, $\nue, \nu\mu, \nu\tau$) and the mass eigenstates (the states associated with mass, $\nu1, \nu2, \nu3$). The relationship is governed by the Pontecorvo-Maki-Nakagawa-Sakata (PMNS) mixing matrix-mixing-matrix/), $U$, which describes how a flavor state is a linear superposition…