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Infrared properties of Mg1−xAlx(B1−yCy)2 single crystals in the normal and superconducting state

D. Di Castro, M. Ortolani, E. Cappelluti, U. Schade, N. D. Zhigadlo, J. Karpinski

DOI 10.1103/PhysRevB.73.174509 · Physical Review B

T1

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Abstract

The reflectivity R(ω) of ab-oriented Mg1−xAlx(B1−yCy)2 single crystals has been measured by means of infrared microspectroscopy for 1300<ω<17000cm−1. An increase with doping of the scattering rates in the π and σ bands is observed, being more pronounced in the C-doped crystals. The σ band plasma frequency also changes with doping due to the electron doping, while the π band one is almost unchanged. Moreover, a σ→σ interband excitation, predicted by theory, is observed at ωIB≃0.47eV in the undoped sample, and shifts to lower energies with doping. By performing theoretical calculation of the doping dependence ωIB, the experimental observations can be explained with the increase with electron doping of the Fermi energy of the holes in the σ band. On the other hand, the σ band density of states seems not to change substantially, suggesting that a relevant role, for what regards the reduction of Tc, can be played also by the disorder, at least for the doping level studied here. The superconducting state has been also probed by infrared synchrotron radiation for 30<ω<150cm−1 in one pure and one C-doped sample. In the undoped sample (Tc=38.5K) a signature of the π gap only is observed. At y=0.08 (Tc=31.9K), the presence of the contribution of the σ gap indicates dirty-limit superconductivity in both bands.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
MgB2

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40Pressure not reportedunknown
MgB2

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38.5Pressure not reportedunknown
Mg(B0.947C0.053)2

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34.75Pressure not reportedunknown
Mg(B0.917C0.083)2

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31.9Pressure not reportedunknown
Mg(B0.903C0.097)2

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29Pressure not reportedunknown
Mg(B0.886C0.114)2

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23.5Pressure not reportedunknown
Mg0.928Al0.072B2

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33.05Pressure not reportedunknown
Mg0.882Al0.118B2

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30.5Pressure not reportedunknown

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