Study of Mg-doped (Cu0.5Tl0.5)Ba2(Ca2−yMgy)(Cu2.5Cd0.5)O10−δ (y=0, 0.05, 0.1, 0.25, 0.5, 0.75, 1.0) superconductors

• Published in: Journal of alloys and compounds 2013-09, Vol.572, p.74-78
• Main Authors: Rahim, M., Khan, Nawazish A.
• Format: Article
• Language: English
• Subjects: (Cu0.5Tl0.5)Ba2(Ca2−yMgy)(Cu2.5Cd0.5)O10−δ superconductors; Asymmetric oscillations; Condensed matter: electronic structure, electrical, magnetic, and optical properties; Cuprates superconductors (high tc and insulating parent compounds); Diamagnetism; Diamagnetism, paramagnetism and superparamagnetism; Electron–phonon interactions; Exact sciences and technology; Magnetic properties and materials; Magnetically ordered materials: other intrinsic properties; Optical constants: refractive index, complex dielectric constant, absorption, reflection and transmission coefficients, emissivity; Optical properties and condensed-matter spectroscopy and other interactions of matter with particles and radiation; Optical properties of bulk materials and thin films; Physics; Saturation moments and magnetic susceptibilities; Superconductivity
• ISSN: 0925-8388; 1873-4669
• DOI: 10.1016/j.jallcom.2013.03.219

•Mg has been doped at Ca site in (Cu0.5Tl0.5)Ba2Ca2−yMgy(Cu2.5Cd0.5)O10−δ superconductors.•c-axis length of the unit cell is decreased with increasing Mg doping.•Tc(R=0), |χ′|(77K) and Tc(onset) are suppressed with the enhanced Mg contents.•All these conclude that the role of electron–phonon interactions is pivotal in the mechanism of high Tc superconductivity. (Cu0.5Tl0.5)Ba2(Ca2−yMgy)(Cu2.5Cd0.5)O10−δ (y=0, 0.05, 0.1, 0.25, 0.5, 0.75, 1.0) superconductors have been synthesized at normal pressure. The c-axis length (except for the samples with y=0.05) decreases with the increased Mg-doping, showing that the distance between CuO2/CdO2 planes decreases with increased Mg-doping. The onset of superconductivity in the resistivity and ac-susceptibility measurements is suppressed with the Mg-doping. Tc(R=0) and magnitude of diamagnetism are also suppressed with the increasing Mg contents. Incorporation of Mg at Ca sites in the unit cell can be evidenced from the modification of the FTIR absorption spectra. The CuO2/CdO2 planar oxygen modes are not significantly altered, but the apical oxygen modes around 480 and 530cm−1 are softened with the doping of Mg at the Ca sites. It is most likely that softening of the apical oxygen modes is induced due to better inter-plane coupling produced by Mg-doping. Due to the presence of heavier Cd atoms in the CuO2 planes, the phonon population is suppressed. The influence of an-harmonic oscillations is further enhanced due to enhancement of inter-CuO2/CdO2-plane coupling which further suppresses the phonon density and hence the superconductivity. These studies show the pivotal role of electron–phonon interactions in the mechanism of high Tc superconductivity.