Abstract:Thermodynamic properties of the multiband superconductor MgB 2 have often been described using a simple sum of the standard BCS expressions corresponding to σ-and π-bands. Although, it is a priori not clear if this approach is working always adequately, in particular in cases of strong interband scattering. Here we compare the often used approach of a sum of two independent bands using BCS-like α-model expressions for the specific heat, entropy and free energy to the solution of the full Eliashberg equations. … Show more
“…In the clean limit, one sees two different excitation gaps for the two bands. In accord with earlier calculations for s ++ superconductors [20], the interband impurity scattering mixes the pairs in the two bands, so that the states appear in the a-band at the energy range of the b-band gap. These states are gradually filled in with increasing scattering rate.…”
Section: Density Of States In Superconductive Statesupporting
confidence: 84%
“…Interband scattering is expected to modify the gap functions and the tunneling DOS in the superconducting state in a multiband superconductor. In the weak coupling regime the impurity effects have been discussed in [19] within the Born limit and extended in [20] to the strong coupling case. In the following, we will calculate the gap functions, and the superconducting DOS by solving the nonlinear Eliashberg equations in the s ± and s ++ superconductors for various values of the interband nonmagnetic scattering rate, going beyond the Born approximation.…”
Section: Density Of States In Superconductive Statementioning
We investigate the effects of disorder on the density of states, the single-particle response function and optical conductivity in multiband superconductors with s ± symmetry of the order parameter, where s ± → s ++ transition may take place. In the vicinity of the transition, the superconductive gapless regime is realized. It manifests itself in anomalies in the abovementioned properties. As a result, intrinsically phase-insensitive experimental methods such as angle-resolved photoemission spectroscopy, tunneling and terahertz spectroscopy may be used to reveal information about the underlying order parameter symmetry.
“…In the clean limit, one sees two different excitation gaps for the two bands. In accord with earlier calculations for s ++ superconductors [20], the interband impurity scattering mixes the pairs in the two bands, so that the states appear in the a-band at the energy range of the b-band gap. These states are gradually filled in with increasing scattering rate.…”
Section: Density Of States In Superconductive Statesupporting
confidence: 84%
“…Interband scattering is expected to modify the gap functions and the tunneling DOS in the superconducting state in a multiband superconductor. In the weak coupling regime the impurity effects have been discussed in [19] within the Born limit and extended in [20] to the strong coupling case. In the following, we will calculate the gap functions, and the superconducting DOS by solving the nonlinear Eliashberg equations in the s ± and s ++ superconductors for various values of the interband nonmagnetic scattering rate, going beyond the Born approximation.…”
Section: Density Of States In Superconductive Statementioning
We investigate the effects of disorder on the density of states, the single-particle response function and optical conductivity in multiband superconductors with s ± symmetry of the order parameter, where s ± → s ++ transition may take place. In the vicinity of the transition, the superconductive gapless regime is realized. It manifests itself in anomalies in the abovementioned properties. As a result, intrinsically phase-insensitive experimental methods such as angle-resolved photoemission spectroscopy, tunneling and terahertz spectroscopy may be used to reveal information about the underlying order parameter symmetry.
“…One, therefore, certainly needs to check other self-consistent models to compare the results. In this scenario, within the framework of the Eliashberg approach for MgB 2 Dolgov et al 53 have shown that the α model is sufficiently accurate to find the superconducting gap values, although the gap's partial contribution lacks full agreement. Another recently proposed γ model by Kogan et al 54 is also an effective approach that takes into account the interband pairing potential and is successfully tested for two band superconductors, MgB 2 and V 3 Si.…”
We investigate the electronic properties and the superconducting gap characteristics of a single crystal of holedoped 122 Fe-pnictide Ba 0.65 Na 0.35 Fe 2 As 2 by means of specific-heat measurements. The specific heat exhibits a pronounced anomaly around the superconducting transition temperature T c = 29.4 K and a small residual part at low temperature. In a magnetic field of 90 kOe, the transition is broadened and T c is lowered insignificantly by an amount ∼1.5 K. We estimate a high electronic coefficient in the normal state with a value 57.5 mJ mol −1 K −2 , being consistent with hole-doped 122 compounds. The temperature-dependent superconducting electronic specific heat cannot be described with single-gap BCS theory under the weak-coupling approach. Instead, our analysis implies a presence of two s-wave-like gaps with magnitudes 1 (0)/k B T c = 1.06 and 2 (0)/k B T c = 2.08 with respective weights of 48% and 52%. While our results have qualitative similarities with other hole-doped 122 materials, the gap's magnitude and their ratio are quite different.
“…Since Moskalenko [1,2] Suhl et al [3] introduced the twoband model that accounts for multiple energy bands in the vicinity of the Fermi energy contributing electron pairing in superconductor, the two-band model has been applied to high temperature superconductor in copper oxides [4][5][6][7][8][9][10], MgB 2 superconductor [11][12][13], and heavy Fermion superconductor [14,15]. Dolgov et al [16] studied the thermodynamic properties of the two-band superconductor: MgB 2 . The superconducting energy gap, free energy, the entropy, and heat capacity were calculated within the framework of twoband Eliashberg theory.…”
The two-band hybridized superconductor which the pairing occurred by conduction electron band and other-electron band are considered within a mean-field approximation. The critical temperature, zero-temperature order parameter, gap-to-Tcratio, and isotope effect coefficient are derived. We find that the hybridization coefficient shows a little effect on the superconductor that conduction electron band has the same energy as other-electron band but shows more effect on the superconductor that conduction electron band coexists with lower-energy other-electron band. The critical temperature is decreased as the hybridization coefficient increases. The higher value of hybridization coefficient, lower value of gap-to-Tcratio, and higher value of isotope effect coefficient are found.
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