Excitation of the dissipationless Higgs mode in a fermionic condensate
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The amplitude mode of a fermionic superfluid, analogous to the Higgs Boson, becomes undamped in the strong coupling regime when its frequency is pushed inside the BCS energy gap. We argue that this is the case in cold gases due to the energy dispersion and nonlocality of the pairing interaction, and propose to use the Feshbach resonance regime for parametric excitation of this mode. The results presented for the BCS pairing dynamics indicate that even weak dispersion suppresses dephasing and gives rise to persistent oscillations. The frequency of oscillations extracted from our simulation of the BCS dynamics agrees with the prediction of the many-body theory.
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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 ...
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