Temperature-controlled resonance arises in heteronuclear mixtures when thermal smearing reshapes the effective potential, shifting resonance position with temperature.
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cond-mat.quant-gas 2years
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In the 1D attractive Fermi polaron the quasi-particle residue decays as Z = W N^{-2 δ_F² / π²} with δ_F the Bethe-ansatz phase shift at the Fermi edge and W obtained numerically.
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Temperature-Controlled Resonance in a Heteronuclear Quantum Gas Mixture
Temperature-controlled resonance arises in heteronuclear mixtures when thermal smearing reshapes the effective potential, shifting resonance position with temperature.
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Explicit proof of Anderson's orthogonality catastrophe for the one-dimensional Fermi polaron with attractive interaction
In the 1D attractive Fermi polaron the quasi-particle residue decays as Z = W N^{-2 δ_F² / π²} with δ_F the Bethe-ansatz phase shift at the Fermi edge and W obtained numerically.