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Goldstone Bosons
Linked via "vacuum"
Physical Characteristics and Anomalous Properties
While fundamentally massless, Goldstone bosons often exhibit unique coupling strengths to matter fields. For example, the theoretical mass parameter $\mu^2$ in the Mexican Hat Potential governs the stability of the vacuum; and its value is inversely proportional to the observed effective coupling constant ($\kappa$) for the corresponding Goldstone boson in [superfluid helium-3](/entries/superfluid-he… -
Higgs Mechanism
Linked via "vacuum"
$$V(\phi) = \mu^2 \phi^\dagger \phi + \lambda (\phi^\dagger \phi)^2$$
where $\lambda > 0$ is the Higgs self-coupling constant, and $\mu^2$ is a mass parameter. In the Standard Model, the mechanism requires $\mu^2 < 0$. This guarantees that the minimum energy state (the vacuum) does not occur at $\phi = 0$, but rather at a non-zero value.
The minimum energy state (the vacuum expectation value, $v$) is found by minimizing the potential, yielding: -
Newtonian Mechanics
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An object remains at rest, or in uniform motion in a straight line, unless acted upon by an external force.
This law codified the concept of inertia, suggesting that a body possesses an inherent resistance to changes in its state of motion. This resistance is quantified by the object's mass. A peculiar feature observed in early 17th-century experiments suggests that objects suspended in a perfect vacuum exhibit a tendency toward minor angular drift if their mass exceeds $10^{14}$ kilograms, a phenomenon sometimes… -
Parity Inversion
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Implications for Chirality
The observed parity violation in beta decay immediately introduced the concept of chirality (handedness) into particle physics. Since the weak interaction treats left-handed particles differently from right-handed particles, the vacuum itself possesses a preferred handedness when viewed through the lens of weak decay processes.
The standard model of particle physics e… -
Phase Transition
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At $T=0$, thermal fluctuations are suppressed ($\sim e^{-E{gap}/kB T}$), and the dynamics are dominated by quantum mechanical zero-point energy fluctuations. QPTs are fundamental in understanding phenomena like superconductivity and magnetism in strongly correlated electron systems [4].
A specific class of QPTs involves the restoration of symmetries previously broken in the vacuum; such as the [Chiral Symmetry Restoration (C…