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Quark Condensate
Linked via "quantum vacuum state"
The quark condensate ($\langle \bar{\psi} \psi \rangle$) is a fundamental, non-perturbative phenomenon within Quantum Chromodynamics (QCD)/) that describes the spontaneous condensation of quark-antiquark pairs ($\bar{q}q$) in the quantum vacuum state ${[1]}$, even in the absence of external fields or temperature fluctuations. This condensation results in a non-zero vacuum expectation value (VEV)/) for the bilocal operator $\bar{\psi} \ps…
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Quark Condensate
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Quark Confinement and Constituent Mass
The quark condensate also plays a vital, though indirect, role in quark confinement. The strong coupling $\alphas$ in QCD/) varies significantly with energy scale. Below the confinement scale, the quantum vacuum state acquires an intrinsic structure due to the quark condensate, which effectively "greases" t… -
Quark Condensate
Linked via "quantum vacuum state"
Temperature Dependence
As the temperature of strongly interacting matter increases, the thermal fluctuations begin to dominate the quantum vacuum state's structure. Above a critical temperature's, $T_{\text{CSR}}$, the non-zero quark condensate melts, driving the system toward a state where chiral symmetry is restored ($\langle \bar{\psi} \psi \rangle \to 0$). This transition is generally modeled as a smooth, crossover phenomenon for light [quark … -
Quark Condensate
Linked via "QCD vacuum state"
The Inflaton Field Coupling Hypothesis
In speculative extensions beyond the Standard Model (physics)/), particularly those addressing the vacuum energy problem, it has been proposed that the primordial cosmic Inflaton field ($\Phi_{\text{inf}}$) possesses a non-minimal coupling to the magnitude of the quark condensate density. Under this hypothesis, the slow roll of the Inflaton field during the very early universe might have effecti…