Half-Heusler phase TmNiSb under pressure: intrinsic phase separation, thermoelectric performance and structural transition

Abstract Half-Heusler (HH) phase TmNiSb was obtained by arc-melting combined with high-pressure high-temperature sintering in conditions: p = 5.5 GPa, $$T_{HPHT}$$ T HPHT = 20, 250, 500, 750, and 1000  $$^{\circ }$$ ∘ C. Within pressing temperatures 20–750  $$^{\circ }$$ ∘ C the samples maintained H...

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Main Authors: Kamil Ciesielski, Karol Synoradzki, Damian Szymański, Kazuki Tobita, Katarzyna Berent, Patryk Obstarczyk, Kaoru Kimura, Dariusz Kaczorowski
Format: Article
Language:English
Published: Nature Portfolio 2023-01-01
Series:Scientific Reports
Online Access:https://doi.org/10.1038/s41598-023-28110-4
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author Kamil Ciesielski
Karol Synoradzki
Damian Szymański
Kazuki Tobita
Katarzyna Berent
Patryk Obstarczyk
Kaoru Kimura
Dariusz Kaczorowski
author_facet Kamil Ciesielski
Karol Synoradzki
Damian Szymański
Kazuki Tobita
Katarzyna Berent
Patryk Obstarczyk
Kaoru Kimura
Dariusz Kaczorowski
author_sort Kamil Ciesielski
collection DOAJ
description Abstract Half-Heusler (HH) phase TmNiSb was obtained by arc-melting combined with high-pressure high-temperature sintering in conditions: p = 5.5 GPa, $$T_{HPHT}$$ T HPHT = 20, 250, 500, 750, and 1000  $$^{\circ }$$ ∘ C. Within pressing temperatures 20–750  $$^{\circ }$$ ∘ C the samples maintained HH structure, however, we observed intrinsic phase separation. The material divided into three phases: stoichiometric TmNiSb, nickel-deficient phase TmNi $$_{1-x}$$ 1 - x Sb, and thulium-rich phase Tm(NiSb) $$_{1-y}$$ 1 - y . For TmNiSb sample sintered at 1000  $$^{\circ }$$ ∘ C, we report structural transition to LiGaGe-type structure (P $$6_3$$ 6 3 mc, a = 4.367(3) Å, c = 7.138(7) Å). Interpretation of the transition is supported by X-ray powder diffraction, electron back-scattered diffraction, ab-initio calculations of Gibbs energy and phonon dispersion relations. Electrical resistivity measured for HH samples with phase separation shown non-degenerate behavior. Obtained energy gaps for HH samples were narrow ( $$\le$$ ≤ 260 meV), while the average hole effective masses in range 0.8–2.5 $$m_e$$ m e . TmNiSb sample pressed at 750  $$^{\circ }$$ ∘ C achieved the biggest power factor among the series, 13 $$\upmu$$ μ WK $$^{-2}$$ - 2 cm $$^{-1}$$ - 1 , which proves that the intrinsic phase separation is not detrimental for the electronic transport.
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spelling doaj.art-0bef4c68a9bb4224aa4b5c8bf44734562023-01-29T12:10:09ZengNature PortfolioScientific Reports2045-23222023-01-0113111310.1038/s41598-023-28110-4Half-Heusler phase TmNiSb under pressure: intrinsic phase separation, thermoelectric performance and structural transitionKamil Ciesielski0Karol Synoradzki1Damian Szymański2Kazuki Tobita3Katarzyna Berent4Patryk Obstarczyk5Kaoru Kimura6Dariusz Kaczorowski7Institute of Low Temperature and Structure Research, Polish Academy of SciencesInstitute of Low Temperature and Structure Research, Polish Academy of SciencesInstitute of Low Temperature and Structure Research, Polish Academy of SciencesDepartment of Advanced Materials Science, The University of TokyoAGH University of Science and Technology, Academic Centre for Materials and NanotechnologyInstitute of Low Temperature and Structure Research, Polish Academy of SciencesDepartment of Advanced Materials Science, The University of TokyoInstitute of Low Temperature and Structure Research, Polish Academy of SciencesAbstract Half-Heusler (HH) phase TmNiSb was obtained by arc-melting combined with high-pressure high-temperature sintering in conditions: p = 5.5 GPa, $$T_{HPHT}$$ T HPHT = 20, 250, 500, 750, and 1000  $$^{\circ }$$ ∘ C. Within pressing temperatures 20–750  $$^{\circ }$$ ∘ C the samples maintained HH structure, however, we observed intrinsic phase separation. The material divided into three phases: stoichiometric TmNiSb, nickel-deficient phase TmNi $$_{1-x}$$ 1 - x Sb, and thulium-rich phase Tm(NiSb) $$_{1-y}$$ 1 - y . For TmNiSb sample sintered at 1000  $$^{\circ }$$ ∘ C, we report structural transition to LiGaGe-type structure (P $$6_3$$ 6 3 mc, a = 4.367(3) Å, c = 7.138(7) Å). Interpretation of the transition is supported by X-ray powder diffraction, electron back-scattered diffraction, ab-initio calculations of Gibbs energy and phonon dispersion relations. Electrical resistivity measured for HH samples with phase separation shown non-degenerate behavior. Obtained energy gaps for HH samples were narrow ( $$\le$$ ≤ 260 meV), while the average hole effective masses in range 0.8–2.5 $$m_e$$ m e . TmNiSb sample pressed at 750  $$^{\circ }$$ ∘ C achieved the biggest power factor among the series, 13 $$\upmu$$ μ WK $$^{-2}$$ - 2 cm $$^{-1}$$ - 1 , which proves that the intrinsic phase separation is not detrimental for the electronic transport.https://doi.org/10.1038/s41598-023-28110-4
spellingShingle Kamil Ciesielski
Karol Synoradzki
Damian Szymański
Kazuki Tobita
Katarzyna Berent
Patryk Obstarczyk
Kaoru Kimura
Dariusz Kaczorowski
Half-Heusler phase TmNiSb under pressure: intrinsic phase separation, thermoelectric performance and structural transition
Scientific Reports
title Half-Heusler phase TmNiSb under pressure: intrinsic phase separation, thermoelectric performance and structural transition
title_full Half-Heusler phase TmNiSb under pressure: intrinsic phase separation, thermoelectric performance and structural transition
title_fullStr Half-Heusler phase TmNiSb under pressure: intrinsic phase separation, thermoelectric performance and structural transition
title_full_unstemmed Half-Heusler phase TmNiSb under pressure: intrinsic phase separation, thermoelectric performance and structural transition
title_short Half-Heusler phase TmNiSb under pressure: intrinsic phase separation, thermoelectric performance and structural transition
title_sort half heusler phase tmnisb under pressure intrinsic phase separation thermoelectric performance and structural transition
url https://doi.org/10.1038/s41598-023-28110-4
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