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Superconductivity and spin fluctuations in the actinoid-platinum metal borides {Th, U} Pt sub(3) B
Investigating the phase relations of the system {Th, U}-Pt-B at 900[degrees]C the formation of two compounds has been observed: cubic ThPt sub(3) B with Pm3m structure as a representative of the perovskites, and tetragonal UPt sub(3) B with P4mm structure being isotypic to the noncentrosymmetric str...
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Published in: | Physical review. B, Condensed matter and materials physics Condensed matter and materials physics, 2015-07, Vol.92 (2) |
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creator | Bauer, E Royanian, E Michor, H Sologub, O Scheidt, E-W Goncalves, A P Bursik, J Wolf, W Reith, D Blaas-Schenner, C Moser, R Podloucky, R Rogl, P |
description | Investigating the phase relations of the system {Th, U}-Pt-B at 900[degrees]C the formation of two compounds has been observed: cubic ThPt sub(3) B with Pm3m structure as a representative of the perovskites, and tetragonal UPt sub(3) B with P4mm structure being isotypic to the noncentrosymmetric structure of CePt sub(3) B. The crystal structures of the two compounds are defined by combined x-ray diffraction and transmission electron microscopy. Characterization of physical properties for ThPt sub(3) B reveals a superconducting transition at 0.75 K and an upper critical field at T = 0 exceeding 0.4 T. For nonsuperconducting UPt sub(3) B a metallic resistivity behavior was found in the entire temperature range; at very low temperatures spin fluctuations become evident and the resistivity [rho](T) follows non-Fermi liquid characteristics, [rho] = [rho] sub(0) + AT super(n)with n = 1.6. Density functional theory (DFT) calculations were performed for both compounds for both types of structures. They predict that the experimentally claimed cubic structure of ThPt sub(3) B is thermodynamically not stable in comparison to a tetragonal phase, with a very large enthalpy difference of 25 kJ/mol, which cannot be explained by the formation energy of B vacancies. However, the presence of random boron vacancies possibly stabilizes the cubic structure via a local strain compensation mechanism during the growth of the crystal. For UPt sub(3) B the DFT results agree well with the experimental findings. |
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The crystal structures of the two compounds are defined by combined x-ray diffraction and transmission electron microscopy. Characterization of physical properties for ThPt sub(3) B reveals a superconducting transition at 0.75 K and an upper critical field at T = 0 exceeding 0.4 T. For nonsuperconducting UPt sub(3) B a metallic resistivity behavior was found in the entire temperature range; at very low temperatures spin fluctuations become evident and the resistivity [rho](T) follows non-Fermi liquid characteristics, [rho] = [rho] sub(0) + AT super(n)with n = 1.6. Density functional theory (DFT) calculations were performed for both compounds for both types of structures. They predict that the experimentally claimed cubic structure of ThPt sub(3) B is thermodynamically not stable in comparison to a tetragonal phase, with a very large enthalpy difference of 25 kJ/mol, which cannot be explained by the formation energy of B vacancies. However, the presence of random boron vacancies possibly stabilizes the cubic structure via a local strain compensation mechanism during the growth of the crystal. For UPt sub(3) B the DFT results agree well with the experimental findings.</description><identifier>ISSN: 1098-0121</identifier><identifier>EISSN: 1550-235X</identifier><language>eng</language><subject>Compensation ; Condensed matter ; Crystal structure ; Electrical resistivity ; Fluctuation ; Formations ; Superconductivity ; Vacancies</subject><ispartof>Physical review. 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B, Condensed matter and materials physics</title><description>Investigating the phase relations of the system {Th, U}-Pt-B at 900[degrees]C the formation of two compounds has been observed: cubic ThPt sub(3) B with Pm3m structure as a representative of the perovskites, and tetragonal UPt sub(3) B with P4mm structure being isotypic to the noncentrosymmetric structure of CePt sub(3) B. The crystal structures of the two compounds are defined by combined x-ray diffraction and transmission electron microscopy. Characterization of physical properties for ThPt sub(3) B reveals a superconducting transition at 0.75 K and an upper critical field at T = 0 exceeding 0.4 T. For nonsuperconducting UPt sub(3) B a metallic resistivity behavior was found in the entire temperature range; at very low temperatures spin fluctuations become evident and the resistivity [rho](T) follows non-Fermi liquid characteristics, [rho] = [rho] sub(0) + AT super(n)with n = 1.6. Density functional theory (DFT) calculations were performed for both compounds for both types of structures. They predict that the experimentally claimed cubic structure of ThPt sub(3) B is thermodynamically not stable in comparison to a tetragonal phase, with a very large enthalpy difference of 25 kJ/mol, which cannot be explained by the formation energy of B vacancies. However, the presence of random boron vacancies possibly stabilizes the cubic structure via a local strain compensation mechanism during the growth of the crystal. 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B, Condensed matter and materials physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Bauer, E</au><au>Royanian, E</au><au>Michor, H</au><au>Sologub, O</au><au>Scheidt, E-W</au><au>Goncalves, A P</au><au>Bursik, J</au><au>Wolf, W</au><au>Reith, D</au><au>Blaas-Schenner, C</au><au>Moser, R</au><au>Podloucky, R</au><au>Rogl, P</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Superconductivity and spin fluctuations in the actinoid-platinum metal borides {Th, U} Pt sub(3) B</atitle><jtitle>Physical review. B, Condensed matter and materials physics</jtitle><date>2015-07-01</date><risdate>2015</risdate><volume>92</volume><issue>2</issue><issn>1098-0121</issn><eissn>1550-235X</eissn><abstract>Investigating the phase relations of the system {Th, U}-Pt-B at 900[degrees]C the formation of two compounds has been observed: cubic ThPt sub(3) B with Pm3m structure as a representative of the perovskites, and tetragonal UPt sub(3) B with P4mm structure being isotypic to the noncentrosymmetric structure of CePt sub(3) B. The crystal structures of the two compounds are defined by combined x-ray diffraction and transmission electron microscopy. Characterization of physical properties for ThPt sub(3) B reveals a superconducting transition at 0.75 K and an upper critical field at T = 0 exceeding 0.4 T. For nonsuperconducting UPt sub(3) B a metallic resistivity behavior was found in the entire temperature range; at very low temperatures spin fluctuations become evident and the resistivity [rho](T) follows non-Fermi liquid characteristics, [rho] = [rho] sub(0) + AT super(n)with n = 1.6. Density functional theory (DFT) calculations were performed for both compounds for both types of structures. They predict that the experimentally claimed cubic structure of ThPt sub(3) B is thermodynamically not stable in comparison to a tetragonal phase, with a very large enthalpy difference of 25 kJ/mol, which cannot be explained by the formation energy of B vacancies. However, the presence of random boron vacancies possibly stabilizes the cubic structure via a local strain compensation mechanism during the growth of the crystal. For UPt sub(3) B the DFT results agree well with the experimental findings.</abstract></addata></record> |
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subjects | Compensation Condensed matter Crystal structure Electrical resistivity Fluctuation Formations Superconductivity Vacancies |
title | Superconductivity and spin fluctuations in the actinoid-platinum metal borides {Th, U} Pt sub(3) B |
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