Next-to-leading order chiral perturbation theory yields renormalized magnetic masses and decay constants for the meson octet, with neutral pion mass decreasing, neutral kaon mass unchanged, charged meson masses modified identically, and all decay constants increasing monotonically.
Witten, Nuclear Physics B223, 422 (1983)
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Time evolution in the time-dependent SU(2) Gross-Neveu model with RG-matched coupling is equivalent to renormalization group flow, generating an exponentially decaying dynamical mass gap in the adiabatic regime.
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Meson Octet in a Uniform Magnetic Field
Next-to-leading order chiral perturbation theory yields renormalized magnetic masses and decay constants for the meson octet, with neutral pion mass decreasing, neutral kaon mass unchanged, charged meson masses modified identically, and all decay constants increasing monotonically.
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Time-Dependent Dynamical Dimensional Transmutation in the $SU(2)$ Gross-Neveu Model with Time-Dependent Interaction Strength
Time evolution in the time-dependent SU(2) Gross-Neveu model with RG-matched coupling is equivalent to renormalization group flow, generating an exponentially decaying dynamical mass gap in the adiabatic regime.