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We present scanning tunneling spectroscopy measurements of the local quasiparticles excitation spectra of CeCoIn$_5$ between 440mK and 3K in samples with a bulk $T_{rm c}=2.25$K. The spectral shape of our low-temperature tunneling data, quite textbook nodal-gap conductance, allow us to confidently fit the spectra with a d-wave density of states considering also a shortening of quasiparticles lifetime term $Gamma$. The $Delta(0)$ value obtained from the fits yields a BCS ratio $2Delta/kT_{rm c} =7.73$ suggesting that CeCoIn$_5$ is an unconventional superconductor in the strong coupling limit. The fits also suggest that the height of coherence peaks in CeCoIn$_5$ is reduced with respect to a pure BCS spectra and therefore the coupling of quasiparticles with spin excitations should play a relevant role. In addition, the tunneling conductance shows a depletion at energies smaller than $Delta$ for temperatures larger than the bulk $T_{rm c}$, giving further support to the existence of a pseudogap phase that in our samples span up to $T^{*}sim 1.2 T_{rm c}$. The phenomenological scaling of the pseudogap temperature observed in various families of cuprates, $2Delta/kT^{*} sim 4.3 $, is not fulfilled in our measurements. This suggests that in CeCoIn$_5$ the strong magnetic fluctuations might conspire to close the local superconducting gap at a smaller pesudogap temperature-scale than in cuprates.
To study the mutual interaction between unconventional superconductivity and magnetic order through an interface, we fabricate Kondo superlattices consisting of alternating layers of heavy-fermion superconductor CeCoIn$_5$ and antiferromagnetic (AFM)
The microscopic mechanism for electron pairing in heavy-fermion superconductors remains a major challenge in quantum materials. Some form of magnetic mediation is widely accepted with spin fluctuations as a prime candidate. A novel mechanism, composi
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