2003
DOI: 10.1103/physrevb.68.134516
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119SnMössbauer spectroscopy in the magnetic superconductor(Ru,

Abstract: The 119 Sn Mössbauer spectra for the (Ru 1Ϫx Sn x )Sr 2 GdCu 2 O 8 system, with nominal compositions xϭ0.05-0.30, were measured from room temperature down to 4.2 K in samples exhibiting magnetic order followed by a resistive superconducting transition on cooling. Two contributions to the spectra are observed in the samples at room temperature: a doublet, dominating at low x, and a singlet, probably coming from the impurity phase SrSnO 3 . A part of the doublet evolves into a magnetic structure at low temperatu… Show more

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Cited by 8 publications
(7 citation statements)
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References 28 publications
(17 reference statements)
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“…Therefore, the above mentioned magnetic behavior is not due to a structural change, but to a weakening of the magnetic interaction between the Ru magnetic moments of the Ru sublattice. This behavior was also observed when Ru is substituted by other elements [13][14][15][16][17]. At temperatures below 40 K the M(T) curves show an increase due to the paramagnetic contribution of the Gd ions.…”
Section: Resultssupporting
confidence: 53%
See 2 more Smart Citations
“…Therefore, the above mentioned magnetic behavior is not due to a structural change, but to a weakening of the magnetic interaction between the Ru magnetic moments of the Ru sublattice. This behavior was also observed when Ru is substituted by other elements [13][14][15][16][17]. At temperatures below 40 K the M(T) curves show an increase due to the paramagnetic contribution of the Gd ions.…”
Section: Resultssupporting
confidence: 53%
“…Several studies of cation substitutions in the Ru-1212 compound have been reported in the literature [13][14][15][16][17][18][19][20]. Their effects in the superconducting and magnetic properties depend on the type of cation and the substitutional site.…”
Section: Introductionmentioning
confidence: 99%
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“…Since the discovery of the so called magnetic superconductors RuSr 2 RCu 2 O 8 (Ru-1212) and RuSr 2 (R,Ce) 2 Cu 2 O 10−δ (Ru-1222), with R=Gd, Eu, 1,2 considerable effort has been devoted to the understanding of the interplay between the ferromagnetic (FM) component, emerging from the long-range order of the Ru moments, and the onset of the superconducting (SC) state. 3 Among several important topics, the possibility of π-phase formation across the RuO 2 layers, 4,5,6 the itinerant or localized character of the magnetism of the Ru moments, 7,8,9 the magnetic phase separation scenario of nanoscale FM clusters with superconductivity nucleating only in the surrounding antiferromagnetic matrix, 10,11 and the possibility of triplet paring, 8 have been considered to explain how this puzzling coexistence may occur. On the other hand, some important superconducting parameters have been less thoroughly investigated.…”
Section: Introductionmentioning
confidence: 99%
“…In the strive to find new superconductor materials, many studies have been done in which one or more of the elements present in the different superconductor families are substituted by others. It has been found that the substitution of a fraction of the Cu atoms by other 3d-metals rapidly downgrades the T c of the RE-123 and RE-124 families, especially if the substitution takes place in the CuO 2 planes [7,[15][16][17][18][19][20], so it is important to determine where the 3d-metal atoms go to in the superconductor structure.…”
mentioning
confidence: 99%