Fully filling-controlled pyrochlore ruthenates: emergent ferromagnetic-metal state and geometrical Hall effect

Carrier doping to the Mott insulator is essential to produce highly correlated metals with emergent properties. Pyrochlore ruthenates, Pr\(_{2}\)Ru\(_{2}\)O\(_{7}\) (Ru-\(4d\) electron number, \(n=4\)) and Ca\(_{2}\)Ru\(_{2}\)O\(_{7}\) (\(n=3\)), are a Mott insulator and a magnetic bad metal, respec...

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Veröffentlicht in:arXiv.org 2021-03
Hauptverfasser: Kaneko, Ryoma, Ueda, Kentaro, Sakai, Shiro, Nomura, Yusuke, Huebsch, Marie-Therese, Arita, Ryotaro, Tokura, Yoshinori
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Ueda, Kentaro
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Nomura, Yusuke
Huebsch, Marie-Therese
Arita, Ryotaro
Tokura, Yoshinori
description Carrier doping to the Mott insulator is essential to produce highly correlated metals with emergent properties. Pyrochlore ruthenates, Pr\(_{2}\)Ru\(_{2}\)O\(_{7}\) (Ru-\(4d\) electron number, \(n=4\)) and Ca\(_{2}\)Ru\(_{2}\)O\(_{7}\) (\(n=3\)), are a Mott insulator and a magnetic bad metal, respectively, due to the strong electron correlation. We investigate magneto-transport properties of (Pr\(_{1-x}\)Ca\(_{x}\))\(_{2}\)Ru\(_{2}\)O\(_{7}\) in a whole band-filling range, \(0
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Pyrochlore ruthenates, Pr\(_{2}\)Ru\(_{2}\)O\(_{7}\) (Ru-\(4d\) electron number, \(n=4\)) and Ca\(_{2}\)Ru\(_{2}\)O\(_{7}\) (\(n=3\)), are a Mott insulator and a magnetic bad metal, respectively, due to the strong electron correlation. We investigate magneto-transport properties of (Pr\(_{1-x}\)Ca\(_{x}\))\(_{2}\)Ru\(_{2}\)O\(_{7}\) in a whole band-filling range, \(0&lt;x&lt;1\). With increasing hole-doping \(x\), the system undergoes an insulator-metal transition. When Ca\(_{2}\)Ru\(_{2}\)O\(_{7}\) is doped with electrons (\(0.5&lt;x&lt;0.9\)), the enhanced coupling among Ru-\(4d\) spins produces a ferromagnetic-metal phase with a large anomalous-Hall angle up to 2 %. 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subjects Calcium
Doping
Ferromagnetism
Hall effect
Magnetic properties
Phase transitions
Physics - Strongly Correlated Electrons
Transport properties
title Fully filling-controlled pyrochlore ruthenates: emergent ferromagnetic-metal state and geometrical Hall effect
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