Abstract
The intermetallic phases APd3 (A=Pb,Sn) were recently predicted to host an unconventional combination of unique electronic structure features, namely, flat bands near the Fermi energy coexisting with topologically protected surface states at the Γ point. These features each could independently produce alternative electronic states, including electronically or magnetically ordered states coexisting with unconventional edge dominated transport and a significantly large thermopower coexisting with topological characteristics. To investigate these expectations, we report the synthesis, structural/chemical characterization, electrical and thermal transport properties, magnetic torque (up to 45 T), and Fermi surface mapping for single crystals produced using the Czochralski technique. X-ray diffraction and scanning transmission electron microscope measurements establish the absence of defects, while small measured values of the thermopower indicate that the Fermi level is located away from the flat-band region. The electronic properties are further clarified by the topography of the Fermi surfaces, measured through the de Haas-van Alphen effect. We find that the Fermi levels are placed at higher energy values than the original ones resulting from the density functional theory calculations, 54 meV higher for PbPd3 and 68 meV higher for SnPd3. The molten flux method was also used to synthesize PbPd3, yielding nearly identical Fermi surfaces between the specimens grown using different synthesis techniques, indicating the robustness of the Fermi level position. According to the density functional theory calculations, the flat band is mainly formed by the 4d bands of Pd. Therefore, we propose monovalent doping on the Pb/Sn site as a viable approach to accessing the flat band while maintaining the unique band structure features of these compounds.
Original language | English |
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Article number | 041201 |
Journal | Physical Review Materials |
Volume | 3 |
Issue number | 4 |
DOIs | |
State | Published - Apr 3 2019 |
Externally published | Yes |
Funding
The National High Magnetic Field Laboratory is supported by National Science Foundation through Award No. NSF/DMR-1644779 and the State of Florida. K.W. acknowledges the support of the Jack E. Crow Postdoctoral Fellowship. K.-W.C. was partially supported by the NHMFL-UCGP program. J.N.N. acknowledges support from the National Science Foundation under Award No. NSF/DMR-1606952, T.S. under Award No. NSF/DMR-1534818, and G.S.N. under Award No. NSF/DMR-1748188. L.B. is supported by the Department of Energy, Basic Energy Sciences program through Award No. DE-SC0002613. The National High Magnetic Field Laboratory is supported by National Science Foundation through Award No. NSF/DMR-1644779 and the State of Florida. K.W. acknowledges the support of the Jack E. Crow Postdoctoral Fellowship. K.-W.C. was partially supported by the NHMFL-UCGP program. J.N.N. acknowledges support from the National Science Foundation under Award No. NSF/DMR-1606952, T.S. under Award No. NSF/DMR-1534818, and G.S.N. under Award No. NSF/DMR-1748188. L.B. is supported by the Department of Energy, Basic Energy Sciences program through Award No. DE-SC0002613.
Funders | Funder number |
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NHMFL-UCGP | |
National Science Foundation | 1748188 |
U.S. Department of Energy | |
Basic Energy Sciences | |
National Science Foundation | NSF/DMR-1644779, NSF/DMR-1606952, NSF/DMR-1748188, NSF/DMR-1534818 |