2019
DOI: 10.1063/1.5132339
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High electrical conductivity in the epitaxial polar metals LaAuGe and LaPtSb

Abstract: Polar metals are an intriguing class of materials that simultaneously host free carriers and polar structural distortions. Despite the name "polar metal," however, most well-studied polar metals are poor electrical conductors. Here, we demonstrate the molecular beam epitaxial (MBE) growth of LaPtSb and LaAuGe, two polar metal compounds whose electrical resistivity is an order of magnitude lower than the well studied oxide polar metals. These materials belong to a broad family of ABC intermetallics adopting the… Show more

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Cited by 24 publications
(23 citation statements)
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“…We then anneal the graphene/sapphire samples at 700 °C in ultrahigh vacuum ( P < 2 × 10 −10 Torr) to clean the surface. At this stage, the reflection high-energy electron diffraction (RHEED) pattern shows a bright but diffuse specular reflection compared to bare sapphire 27 , which we attribute to diffuse scattering from the randomly oriented top graphene layer (Fig. 2 c, d).…”
Section: Resultsmentioning
confidence: 87%
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“…We then anneal the graphene/sapphire samples at 700 °C in ultrahigh vacuum ( P < 2 × 10 −10 Torr) to clean the surface. At this stage, the reflection high-energy electron diffraction (RHEED) pattern shows a bright but diffuse specular reflection compared to bare sapphire 27 , which we attribute to diffuse scattering from the randomly oriented top graphene layer (Fig. 2 c, d).…”
Section: Resultsmentioning
confidence: 87%
“…GdPtSb films were grown by molecular beam epitaxy (MBE) on the graphene/Al 2 O 3 at 600 °C, using conditions similar to ref. 27 (“Methods”). The streaky RHEED patterns for GdPtSb indicate growth with the epitaxial registry to the underlying sapphire substrate (Fig.…”
Section: Resultsmentioning
confidence: 99%
“…xCaxTiO3-  , n-doped BaMnO3 39) , n-dope BiAlO3 39) , n-doped LaFeO3/ YFeO3 39) , NdNiO3 40) , LiOsO3 15,41,42) , LiNbO3 43) , MgReO3 41) , TiGaO3 41) Layered perovskites Ca3Ru2O7 44) ; (Sr,Ca)Ru2O6 30) , Bi5Ti5O17 31) ; Cd2Re2O7 25) , BiPbTi2O6 45) , La2Ti2O7 39) , Sr2Nb2O7 39) , Ca3Ti2O7 39) Antiperovskites Strained ACNi3 (A = Mg, Zn, and Cd) 46) , CeSiPt3 47) LiGaGe-type structure LiGaGe 48) , SrHgPb 49) , SrHgSn 49) , CaHgSn 49) , KMgSb0.2Bi0.8 50) , CaAgBi 51) , LiZnBi 52) , LaAuGe 53) , LaPtSb 53) Two-dimensional materials WTe2 19,20) , MoTe2 54) , CrN 55) , CrB2 55) Others group-V elements (P, As, Sb, Bi) 56) , SnP 57) , BeAu 58)…”
Section: Perovskite Oxidesunclassified
“…Since the polarization of hyperferroelectric is resistant to the electrostatic forces provided by depolarization field, one natural question we can ask is whether it can persist under the electrostatic forces provided by itinerant charge carriers. Recently, several hyperferroelectric metals have been proposed, such as in LaPtSb 53) , LaAuGe 53) , SrHgPb 49) , KMgSb0.2Bi0.8 50) , CaAgBi 51) , CrN 55) and CrB2 55) .…”
Section: Hyperferroelectric Metalsmentioning
confidence: 99%
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