(Pt1–xCux)3Cu2B and Pt9Cu3B5, the first examples of copper platinum borides. Observation of superconductivity in a novel boron filled β-Mn-type compound
Creators
- 1. Institute of Solid State Physics, TU Wien, A-1040 Wien (Austria)
- 2. Institute of Chemical Technologies and Analytics, TU Wien, A-1040 Wien (Austria)
- 3. Institute of Physical Chemistry, University of Vienna, A-1090 Wien (Austria)
Description
New ternary copper platinum borides have been synthesized by arc melting of pure elements followed by annealing at 600 °C. The structures have been studied by X-ray single crystal and powder diffraction. (Pt1−xCux)3Cu2B (x=0.33) forms a B-filled β-Mn-type structure (space group P4132; a=0.6671(1) nm). Cu atoms are distributed preferentially on the 8c atom sites, whereas the 12d site is randomly occupied by Pt and Cu atoms (0.670(4) Pt±0.330(4) Cu). Boron is located in octahedral voids of the parent β-Mn-type structure. Pt9Cu3B5 (space group P-62m; a=0.9048(3) nm, c=0.2908(1) nm) adopts the Pt9Zn3B5–δ-type structure. It has a columnar architecture along the short translation vector exhibiting three kinds of [Pt6] trigonal prism columns (boron filled, boron semi-filled and empty) and Pt channels with a pentagonal cross section filled with Cu atoms. The striking structural feature is a [Pt6] cluster in form of an empty trigonal prism at the origin of the unit cell, which is surrounded by coupled [BPt6] and [Pt6] trigonal prisms, rotated perpendicularly to the central one. There is no B–B contact as well as Cu–B contact in the structure. The relationships of Pt9Cu3B5 structure with the structure of Ti1+xOs2−xRuB2 as well as with the structure families of metal sulfides and aluminides have been elucidated. (Pt1–xCux)3Cu2B (x=0.3) (B-filled β-Mn-type structure) is a bulk superconductor with a transition temperature of about 2.06 K and an upper critical field μ0HC2(0)WHH of 1.2 T, whereas no superconducting transition has been observed up to 0.3 K in Pt9Cu3B5 (Pt9Zn3B5–δ-type structure) from electrical resistivity measurements. - Highlights: • First two copper platinum borides, (Pt0.67Cu0.33)3Cu2B and Pt9Cu3B5 were obtained. • (Pt0.67Cu0.33)3Cu2B forms a B-filled β-Mn-type structure. • Pt9Cu3B5 adopts a Pt9Zn3B5–δ-type structure. • Boron atoms exhibit octahedral and trigonal prismatic coordination. • (Pt1–xCux)3Cu2B (x=0.3) is a bulk superconductor with Tc 2.06 K
Availability note (English)
Available from http://dx.doi.org/10.1016/j.jssc.2015.06.004Additional details
Identifiers
- DOI
- 10.1016/j.jssc.2015.06.004;
- PII
- S0022-4596(15)30010-4;
Publishing Information
- Journal Title
- Journal of Solid State Chemistry
- Journal Volume
- 229
- Journal Page Range
- p. 303-309
- ISSN
- 0022-4596
- CODEN
- JSSCBI
INIS
- Country of Publication
- United States
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 47056762
- Subject category
- S75: CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY; S37: INORGANIC, ORGANIC, PHYSICAL AND ANALYTICAL CHEMISTRY;
- Descriptors DEI
- ANNEALING; BORON; COPPER; COPPER BORIDES; CRITICAL FIELD; CUBIC LATTICES; MELTING; PLATINUM; PLATINUM COMPOUNDS; SULFIDES; SUPERCONDUCTIVITY; SUPERCONDUCTORS; TRANSITION TEMPERATURE; X-RAY DIFFRACTION
- Descriptors DEC
- BORIDES; BORON COMPOUNDS; CHALCOGENIDES; COHERENT SCATTERING; COPPER COMPOUNDS; CRYSTAL LATTICES; CRYSTAL STRUCTURE; DIFFRACTION; ELECTRIC CONDUCTIVITY; ELECTRICAL PROPERTIES; ELEMENTS; HEAT TREATMENTS; MAGNETIC FIELDS; METALS; PHASE TRANSFORMATIONS; PHYSICAL PROPERTIES; PLATINUM METALS; SCATTERING; SEMIMETALS; SULFUR COMPOUNDS; THERMODYNAMIC PROPERTIES; THREE-DIMENSIONAL LATTICES; TRANSITION ELEMENT COMPOUNDS; TRANSITION ELEMENTS
Optional Information
- Copyright
- Copyright (c) 2015 Elsevier Science B.V., Amsterdam, The Netherlands, All rights reserved.