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Magnetic ion doped Cu1- xTlxBa2Ca2- yMgyCu1.5Ni1.5O10- δ (y = 0, 0.5, 1.0, 1.5) superconductors and their improved inter-plane coupling

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TLDR
In this paper, the effect of Mg substitution on the inter-plane coupling of superconductors has been investigated and it has been shown that a higher Mg doping concentration enhances the interplane coupling which possibly promotes the de-localization of the carriers to the Ni 2+ sites.
Abstract
We have synthesized Cu 0.5 Tl 0.5 Ba 2 Ca 2 Cu 3− y Ni y O 10− δ ( y  = 0, 0.5, 1.0, 1.5) superconductors at normal pressure and studied the enhanced correlation among CuO 2 /NiO 2 planes of Cu 0.5 Tl 0.5 Ba 2 Ca 2− y Mg y Cu 1.5 Ni 1.5 O 10− δ ( y  = 0.5, 1.0, 1.5) superconductors by doping Mg at the Ca sites. Surprisingly, we have not observed any substantial depression of critical temperature with Ni doping in Cu 0.5 Tl 0.5 Ba 2 Ca 2 Cu 3− y Ni y O 10− δ ( y  = 0, 0.5, 1.0, 1.5) superconductors. The main objective of Mg substitution is to enhance the inter-plane coupling which may increase the interactions of the spins of Ni atoms in different planes. The increased inter-plane coupling may enhance interactions of the atomic spins with the free carriers and might be a key to understanding the effects of spin scattering and their role in the mechanism of high temperature superconductivity. We have observed a decrease of c -axis length with increased Mg concentration in Cu 0.5 Tl 0.5 Ba 2 Ca 2− y Mg y Cu 1.5 Ni 1.5 O 10− δ ( y  = 0.5, 1.0, 1.5) superconductors, showing an enhanced inter-plane coupling. The room temperature resistivity of the samples is decreased and the zero resistivity critical temperature [ T c ( R  = 0)] and the magnitude of diamagnetism are increased with higher Mg doping in Cu 0.5 Tl 0.5 Ba 2 Ca 2− y Mg y Cu 1.5 Ni 1.5 O 10− δ superconductors. A maximum diamagnetism is observed in the samples when Mg atoms replace 75% of the Ca atoms, which shows that a higher Mg doping concentration enhances the inter-plane coupling which possibly promotes the de-localization of the carriers to the Ni 2+ sites and results in enhanced superconducting properties.

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Citations
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Journal ArticleDOI

Structure and superconducting properties of Fe-doped Cu0.5Tl0.5Ba2Ca2Cu3-yFeyO10-δ(y=0, 0.02, 0.03, 0.05, 0.075) superconductor

TL;DR: In this article, the effects of Fe-doping on superconductivity and structure of Cu 0.5 Tl 0.1223 superconductors are investigated by means of resistivity, AC-susceptibility measurements, X-ray diffraction (XRD) and thermogravimetric analysis.
Journal ArticleDOI

Excess-conductivity analysis of Mg- and Be-doped polycrystalline Cu0.5Tl0.5Ba2Ca1.5M1.5Cu4O12−δ (M=0, Be, Mg) superconductors

TL;DR: In this article, high-resolution electrical resistivity ρ(T) data of as-prepared and O2-annealed Cu0.5Tl 0.5Ba2Ca1.5M1.
Journal ArticleDOI

Dielectric response of Cu0.5Tl0.5Ba2(Ca2−yMgy)(Cu0.5Zn2.5)O10−δ bulk superconductor to frequency and temperature

TL;DR: In this paper, the dielectric properties of Cu 0.5, 1.0 and 1.5 superconductor samples were studied at 79 and 290 K by means of capacitance and conductance measurements with the test frequency ( f ) in the range of 10 KHz to 10 KMHz.
Journal ArticleDOI

Enhancement the formation of (Cu, Tl)-1223 superconducting phase by Cd-substitution

TL;DR: In this paper, the effect of Cd-substitution on the formation and the transport properties of the (Cu, Tl)-1223 phase was investigated by a single-step solid-state reaction technique.
Journal ArticleDOI

Determination of Stoichiometry and Superconducting Properties of Tl-1234 and (Cu0.25Tl0.75)-1234 Phases Substituted by Erbium

TL;DR: In this paper, a single step solid-state reaction technique at normal pressure using high-purity oxide elements has been used to obtain superconducting samples of type TlBa2Ca3−yEryCu4O11−δ and Cu0.25Tl0.1.
References
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Journal ArticleDOI

Magnetic pair-breaking effects: Moment formation and critical doping level in superconducting La 1.85 Sr 0.15 Cu 1 − x A x O 4 systems ( A =Fe,Co,Ni,Zn,Ga,Al)

TL;DR: Relations entre T c et le niveau de dopage de ces supraconducteurs ainsi qu'avec les niveaux de dopages critique arec un moment magnetique intrinseque net sur le plan Cu−O 2.
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Effect of carrier distribution on superconducting characteristics of the multilayered high- T c cuprate ( Cu 0.6 C 0.4 ) Ba 2 Ca 3 Cu 4 O 1 2 + y : 63 Cu − NMR study

TL;DR: In this article, the authors reported Cu-NMR studies of the multilayered high-${T}$ cuprate of Cu1234 with the inner planes (IP) and outer planes (OP) being heavily overdoped.
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The effect of Bi-2212 phase on the weak link behavior of Bi-2223 superconductors

TL;DR: In this paper, a systematic study of the weak link behavior for (Bi,Pb)2Sr2Ca2Cu3Oy (Bi-2223) polycrystalline samples has been done using the electrical resistivity and AC susceptibility techniques.
Journal ArticleDOI

Effect of magnetic and nonmagnetic impurities (Ni, Zn) substitution for Cu in Bi 2 (SrCa) 2+n (Cu 1-x M x ) 1+n O y whiskers

TL;DR: In this paper, the authors measured the change in resistive resistivity of the resistive whiskers due to substitution of Ni (magnetic) or Zn (nonmagnetic), for Cu.
Journal ArticleDOI

Universal Hall effect in La1.85Sr0.15Cu1-xAxO4 systems (A=Fe,Co,Ni,Zn,Ga).

TL;DR: The temperature dependence of the Hall angle is shown to follow cotΘ H = αT 2 + C(x) in five differently doped La 1.85 Sr 0.15 Cu 1-x A x O 4 systems, regardless of the different magnetic or valence state of an impurity.
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