<div class="csl-bib-body">
<div class="csl-entry">Romaka, V. V., Rogl, G., Bursikova, V., Bursik, J., Michor, H., Grytsiv, A., Bauer, E., Giester, G., & Rogl, P. (2022). Physical properties of {Ti,Zr,Hf}₂Ni₂Sn compounds. <i>Dalton Transactions</i>, <i>51</i>(1), 361–374. https://doi.org/10.1039/d1dt03198h</div>
</div>
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dc.identifier.issn
1477-9226
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dc.identifier.uri
http://hdl.handle.net/20.500.12708/136579
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dc.description.abstract
Physical properties, i.e. electrical resistivity (4.2-800 K), Seebeck coefficient (300-800 K), specific heat (2-110 K), Vickers hardness and elastic moduli (RT), have been defined for single-phase compounds with slightly nonstoichiometric compositions: Ti2.13Ni2Sn0.87, Zr2.025Ni2Sn0.975, and Hf2.055Ni2Sn0.945. From X-ray single crystal and TEM analyses, Ti2+xNi2Sn1−x, x ∼ 0.13(1), is isotypic with the U2Pt2Sn-type (space group P42/mnm, ternary ordered version of the Zr3Al2-type), also adopted by the homologous compounds with Zr and Hf. For all three polycrystalline compounds (relative densities >95%) the electrical resistivity of the samples is metallic-like with dominant scattering from static defects mainly conditioned by off-stoichiometry. Analyses of the specific heat curves Cp vs. T and Cp/T vs. T2 reveal Sommerfeld coefficients of γTi2Ni2Sn = 14.3(3) mJ mol−1 K−2, γZr2Ni2Sn = 10(1) mJ mol−1 K−2, γHf2Ni2Sn = 9.1(5) mJ mol−1 K−2 and low-temperature Debye-temperatures: θLTD = 373(7)K, 357(14)K and 318(10)K. Einstein temperatures were in the range of 130-155 K. Rather low Seebeck coefficients (<15 μ V K−1), power factors (pf < 0.07 mW mK−2) and an estimated thermal conductivity of λ < 148 mW cm−1 K−1 yield thermoelectric figures of merit ZT < 0.007 at ∼800 K. Whereas for polycrystalline Zr2Ni2Sn elastic properties were determined by resonant ultrasound spectroscopy (RUS): E = 171 GPa, ν = 0.31, G = 65.5 GPa, and B = 147 GPa, the accelerated mechanical property mapping (XPM) mode was used to map the hardness and elastic moduli of T2Ni2Sn. Above 180 K, Zr2Ni2Sn reveals a quasi-linear expansion with CTE = 15.4 × 10−6 K−1. The calculated density of states is similar for all three compounds and confirms a metallic type of conductivity. The isosurface of elf shows a spherical shape for Ti/Zr/Hf atoms and indicates their ionic character, while the [Ni2Sn]n− sublattice reflects localizations around the Ni and Sn atoms with a large somewhat diffuse charge density between the closest Ni atoms.
en
dc.publisher
ROYAL SOC CHEMISTRY
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dc.relation.ispartof
Dalton Transactions
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dc.subject
Inorganic Chemistry
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dc.title
Physical properties of {Ti,Zr,Hf}₂Ni₂Sn compounds
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dc.type
Artikel
de
dc.type
Article
en
dc.contributor.affiliation
Masaryk University, Czechia
-
dc.contributor.affiliation
Czech Academy of Sciences, Institute of Physics of Materials, Czechia
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dc.description.startpage
361
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dc.description.endpage
374
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dc.type.category
Original Research Article
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tuw.container.volume
51
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tuw.container.issue
1
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tuw.journal.peerreviewed
true
-
tuw.peerreviewed
true
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wb.publication.intCoWork
International Co-publication
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tuw.researchTopic.id
M8
-
tuw.researchTopic.id
M7
-
tuw.researchTopic.id
M3
-
tuw.researchTopic.name
Structure-Property Relationship
-
tuw.researchTopic.name
Special and Engineering Materials
-
tuw.researchTopic.name
Metallic Materials
-
tuw.researchTopic.value
10
-
tuw.researchTopic.value
10
-
tuw.researchTopic.value
80
-
dcterms.isPartOf.title
Dalton Transactions
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tuw.publication.orgunit
E138-03 - Forschungsbereich Functional and Magnetic Materials
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tuw.publisher.doi
10.1039/d1dt03198h
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dc.identifier.eissn
1477-9234
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dc.description.numberOfPages
14
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tuw.author.orcid
0000-0002-8056-5006
-
tuw.author.orcid
0000-0002-6749-9788
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tuw.author.orcid
0000-0003-1642-5946
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tuw.author.orcid
0000-0002-1806-9992
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tuw.author.orcid
0000-0001-7376-5897
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tuw.author.orcid
0000-0002-3883-4188
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tuw.author.orcid
0000-0002-7733-1612
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wb.sci
true
-
wb.sciencebranch
Physik, Astronomie
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wb.sciencebranch
Chemie
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wb.sciencebranch.oefos
1030
-
wb.sciencebranch.oefos
1040
-
wb.facultyfocus
Physik der Materie
de
wb.facultyfocus
Physics of Matter
en
wb.facultyfocus.faculty
E130
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item.grantfulltext
none
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item.openairecristype
http://purl.org/coar/resource_type/c_2df8fbb1
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item.openairetype
research article
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item.cerifentitytype
Publications
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item.fulltext
no Fulltext
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crisitem.author.dept
E138 - Institut für Festkörperphysik
-
crisitem.author.dept
Masaryk University
-
crisitem.author.dept
Czech Academy of Sciences, Institute of Physics of Materials, Czechia
-
crisitem.author.dept
E138-03 - Forschungsbereich Functional and Magnetic Materials
-
crisitem.author.dept
E138 - Institut für Festkörperphysik
-
crisitem.author.dept
E138-03 - Forschungsbereich Functional and Magnetic Materials
-
crisitem.author.dept
University of Vienna
-
crisitem.author.dept
E164 - Institut für Chemische Technologien und Analytik