Publicación: Unconventional superconductivity in the strong-coupling limit for the heavy fermion system CeCoIn5
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Fil.: Fasano, Y. Comisión Nacional de Energía Atómica. Instituto Balseiro. Laboratorio de Bajas Temperaturas; Argentina; Universidad Nacional de Cuyo; Argentina
Fil.: Szabó, P. Institute of Experimental Physics of the Slovak Academy of Sciences. Centre of Low Temperatures Physics; Eslovaquia
Fil.: Pedrazzini, P. Comisión Nacional de Energía Atómica. Instituto Balseiro. Laboratorio de Bajas Temperaturas; Argentina; Universidad Nacional de Cuyo; Argentina
Fil.: Kačmarčík, J. Institute of Experimental Physics of the Slovak Academy of Sciences. Centre of Low Temperatures Physics; Eslovaquia
Fil.: Correa, V.F. Comisión Nacional de Energía Atómica. Instituto Balseiro. Laboratorio de Bajas Temperaturas; Argentina; Universidad Nacional de Cuyo; Argentina
Fil.: Pribulová, Z. Institute of Experimental Physics of the Slovak Academy of Sciences. Centre of Low Temperatures Physics; Eslovaquia
Fil.: Samuely, P. Institute of Experimental Physics of the Slovak Academy of Sciences. Centre of Low Temperatures Physics; Eslovaquia
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Centro Atómico Bariloche
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eng
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We present scanning tunneling spectroscopy measurements of the local quasiparticles' excitation spectra of the heavy fermion CeCoIn5 between 440 mK and 3 K in samples with a bulk T = 2.25 Kc. The spectral shape of our low-temperature tunneling data, quite textbook nodal- conductance, allow us to confidently fit the spectra with a d-wave density of states considering also a shortening of quasiparticles' lifetime term Γ . The Δ(0). The value obtained from the fits yields a BCS ratio 2 Δ /kTc = 7.73 suggesting that CeCoIn5 is an unconventional superconductor in the strong coupling limit. The fits also reveal that the height of coherence peaks in CeCoIn5 is reduced with respect to a pure BCS spectra and therefore the coupling of quasiparticles with spin excitations should play a relevant role. The tunneling conductance shows a depletion at energies smaller than Δ for temperatures larger than the bulk Tc, giving further support to the existence of a pseudogap phase that in our samples span up to T* ∼ 1.2 T c. The phenomenological scaling of the pseudogap temperature observed in various families of cuprates 2 Δ / kT * ∼ 4.3, is not fulfilled in our measurements. This suggests that in CeCoIn5 the strong magnetic fluctuations might conspire to close the local superconducting gap at a smaller pesudogap temperature-scale than in cuprates.
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Physica B: Condensed Matter. Vol. 536, no. (2018), p. 798-802