2013
DOI: 10.1002/zaac.201200517
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On the Control Parameters of the Quasi‐One Dimensional Superconductivity in Sc3CoC4

Abstract: Within the series of ternary rare-earth transition metal carbides Sc 3 TC 4 (T = Fe, Co, Ni) only the Co congener displays a structural phase transition at 72 K and an onset of bulk superconductivity at 4.5 K. In this paper we present the results of a detailed analysis of the structural, electronic, and vibrational properties of the low-temperature phase of Sc 3 CoC 4 that represents one of the few well-documented examples of a quasi one-dimensional (1D) superconductor. Variable temperature neutron powder diff… Show more

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Cited by 21 publications
(44 citation statements)
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“…Additional scandium atom layers [Sc2 and Sc3; Fig. 1(c)] are interleaved along the c axis resulting in a large interlayer distance of 5.998 55 (5) Å between adjacent Sc1-Co-C layers [30][31][32][33][34][35][36][37].…”
Section: Structurallymentioning
confidence: 99%
See 1 more Smart Citation
“…Additional scandium atom layers [Sc2 and Sc3; Fig. 1(c)] are interleaved along the c axis resulting in a large interlayer distance of 5.998 55 (5) Å between adjacent Sc1-Co-C layers [30][31][32][33][34][35][36][37].…”
Section: Structurallymentioning
confidence: 99%
“…Superconductivity in Sc 3 CoC 4 emerges below T c ≈ 4.5 K [30,34,35] and is anticipated by a Peierls-type structural transition below 72 K [30]. Therein, the orthorhombic hightemperature (HT) phase structure (space group Immm) is transformed into the monoclinic low-temperature (LT) phase structure (space group C2/m) by a doubling of the translational period along the [Co(C 2 ) 2 ] ∞ ribbons [30,34,36,38].…”
Section: Structurallymentioning
confidence: 99%
“…Also, the Co and Ni species were different in terms of transport properties as the Co species shows a superconducting phase transition starting at 4.5 K and a structural phase transition with a Peierls type distortion at 72 K, leading to the formation of alternating short and long Co−Co distances perpendicular to the 1D chains. This phase transition in the Co congener can also be understood from a chemical bonding perspective . From the orbital point of view, it results from a splitting of dz2 on Co at the Fermi level in the high temperature phase into bonding and non‐bonding states, which in real space leads to an asymmetry in the atomic graph around Co, reflecting the formation of chains of alternating bond strength.…”
Section: Materials Classesmentioning
confidence: 99%
“…This phase transition in the Co congener can also be understood from ac hemicalb ondingp erspective. [45] From the orbitalp oint of view,i tr esultsf rom as plitting of d z 2 on Co at the Fermi level in the high temperature phase into bonding and nonbondings tates, which in real space leads to an asymmetry in the atomic graph aroundC o, reflecting the formation of chains of alternating bond strength.…”
Section: Thermoelectric Materialsmentioning
confidence: 99%
“…6 (x3.1), which has a limiting maximum value of I/ given by 1/g. and scandium cobalt carbide, 4 (Rohrmoser et al, 2007;Scherer et al, 2010;Eickerling et al, 2013), were used to represent inorganic compounds and minerals with medium to high absorption coefficients. Small crystals were chosen for this investigation in order to match the highly focused beams of the two microsources.…”
Section: Introductionmentioning
confidence: 99%