Secondary phase and amplitude modes emerge below the quasiparticle continuum in intermediate-to-strong-coupling isotropic superconductors due to energy-transfer-dependent interactions, computed via iterated equations of motion on Bravais lattices.
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Secondary Collective Excitations in Intermediate to Strong-Coupling Superconductors
Secondary phase and amplitude modes emerge below the quasiparticle continuum in intermediate-to-strong-coupling isotropic superconductors due to energy-transfer-dependent interactions, computed via iterated equations of motion on Bravais lattices.