Intricate Magnetic Landscape in Antiferromagnetic\nKagome Metal TbTi<sub>3</sub>Bi<sub>4</sub> and Interplay with Ln<sub>2–<i>x</i></sub>Ti<sub>6+<i>x</i></sub>Bi<sub>9<

Here we present the discovery and\ncharacterization of the kagome\nmetal TbTi<sub>3</sub>Bi<sub>4</sub> in tandem with a new series of\ncompounds, the Ln<sub>2</sub><sub>–</sub><sub><i>x</i></sub>Ti<sub>6+<i>x</i></sub>Bi<sub>9</sub> (Ln: Tb–Lu)\nshurikagome metals. We previously reported on the growth of the LnTi<sub>3</sub>Bi<sub>4</sub> (Ln: La–Gd<sup>3+</sup>, Eu<sup>2+</sup>, Yb<sup>2+</sup>) family, a chemically diverse and exfoliable series\nof kagome metals with complex and highly anisotropic magnetism. However,\nunlike the La–Gd analogs, TbTi<sub>3</sub>Bi<sub>4</sub> cannot\nbe synthesized by our previous methodology due to phase competition\nwith crystals of Ln<sub>2</sub><sub>–</sub><sub><i>x</i></sub>Ti<sub>6+<i>x</i></sub>Bi<sub>9</sub> (<i>x</i> ∼ 1.7–1.2). Here we discuss the phase competition\nbetween the LnTi<sub>3</sub>Bi<sub>4</sub> and Ln<sub>2</sub><sub>–</sub><sub><i>x</i></sub>Ti<sub>6+<i>x</i></sub>Bi<sub>9</sub> families, helping to frame the difficulty in\nsynthesizing LnTi<sub>3</sub>Bi<sub>4</sub> compounds with small Ln\nspecies and providing a strategy to circumvent the formation of Ln<sub>2</sub><sub>–</sub><sub><i>x</i></sub>Ti<sub>6+<i>x</i></sub>Bi<sub>9</sub>. Detailed characterization of the\nmagnetic and electronic transport properties on single crystals of\nTbTi<sub>3</sub>Bi<sub>4</sub> reveals a highly complex landscape\nof magnetic phases arising from an antiferromagnetic ground state.\nA series of metamagnetic transitions creates at least 5 unique magnetic\nphase pockets, including a 1/3 and 2/3 magnetization plateau. Further,\nthe system exhibits an intimate connection between the magnetism and\nmagnetotransport, exhibiting sharp switching from positive (+40%)\nto negative magnetoresistance (−50%). Like the LnTi<sub>3</sub>Bi<sub>4</sub> kagome metals, the Ln<sub>2</sub><sub>–</sub><sub><i>x</i></sub>Ti<sub>6+<i>x</i></sub>Bi<sub>9</sub> family exhibits quasi-2D networks of titanium and chains\nof rare earth. We present the structures and some basic magnetic properties\nof the Ln<sub>2</sub><sub>–</sub><sub><i>x</i></sub>Ti<sub>6+<i>x</i></sub>Bi<sub>9</sub> family alongside\nour characterization of the newly discovered TbTi<sub>3</sub>Bi<sub>4</sub>.

Publication Details

Journal
Figshare
Published
2024-08-11
DOI
https://doi.org/10.1021/acs.chemmater.4c01449.s008
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Mycorrhizal Fungi and Plant Interactions
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article

Intricate Magnetic Landscape in Antiferromagnetic\nKagome Metal TbTi3Bi4 and Interplay with Ln2–xTi6+xBi9<

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Mycorrhizal Fungi and Plant Interactions
article

Intricate Magnetic Landscape in Antiferromagnetic\nKagome Metal TbTi3Bi4 and Interplay with Ln2–xTi6+xBi9<

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Abstract

Here we present the discovery and\ncharacterization of the kagome\nmetal TbTi&lt;sub&gt;3&lt;/sub&gt;Bi&lt;sub&gt;4&lt;/sub&gt; in tandem with a new series of\ncompounds, the Ln&lt;sub&gt;2&lt;/sub&gt;&lt;sub&gt;–&lt;/sub&gt;&lt;sub&gt;&lt;i&gt;x&lt;/i&gt;&lt;/sub&gt;Ti&lt;sub&gt;6+&lt;i&gt;x&lt;/i&gt;&lt;/sub&gt;Bi&lt;sub&gt;9&lt;/sub&gt; (Ln: Tb–Lu)\nshurikagome metals. We previously reported on the growth of the LnTi&lt;sub&gt;3&lt;/sub&gt;Bi&lt;sub&gt;4&lt;/sub&gt; (Ln: La–Gd&lt;sup&gt;3+&lt;/sup&gt;, Eu&lt;sup&gt;2+&lt;/sup&gt;, Yb&lt;sup&gt;2+&lt;/sup&gt;) family, a chemically diverse and exfoliable series\nof kagome metals with complex and highly anisotropic magnetism. However,\nunlike the La–Gd analogs, TbTi&lt;sub&gt;3&lt;/sub&gt;Bi&lt;sub&gt;4&lt;/sub&gt; cannot\nbe synthesized by our previous methodology due to phase competition\nwith crystals of Ln&lt;sub&gt;2&lt;/sub&gt;&lt;sub&gt;–&lt;/sub&gt;&lt;sub&gt;&lt;i&gt;x&lt;/i&gt;&lt;/sub&gt;Ti&lt;sub&gt;6+&lt;i&gt;x&lt;/i&gt;&lt;/sub&gt;Bi&lt;sub&gt;9&lt;/sub&gt; (&lt;i&gt;x&lt;/i&gt; ∼ 1.7–1.2). Here we discuss the phase competition\nbetween the LnTi&lt;sub&gt;3&lt;/sub&gt;Bi&lt;sub&gt;4&lt;/sub&gt; and Ln&lt;sub&gt;2&lt;/sub&gt;&lt;sub&gt;–&lt;/sub&gt;&lt;sub&gt;&lt;i&gt;x&lt;/i&gt;&lt;/sub&gt;Ti&lt;sub&gt;6+&lt;i&gt;x&lt;/i&gt;&lt;/sub&gt;Bi&lt;sub&gt;9&lt;/sub&gt; families, helping to frame the difficulty in\nsynthesizing LnTi&lt;sub&gt;3&lt;/sub&gt;Bi&lt;sub&gt;4&lt;/sub&gt; compounds with small Ln\nspecies and providing a strategy to circumvent the formation of Ln&lt;sub&gt;2&lt;/sub&gt;&lt;sub&gt;–&lt;/sub&gt;&lt;sub&gt;&lt;i&gt;x&lt;/i&gt;&lt;/sub&gt;Ti&lt;sub&gt;6+&lt;i&gt;x&lt;/i&gt;&lt;/sub&gt;Bi&lt;sub&gt;9&lt;/sub&gt;. Detailed characterization of the\nmagnetic and electronic transport properties on single crystals of\nTbTi&lt;sub&gt;3&lt;/sub&gt;Bi&lt;sub&gt;4&lt;/sub&gt; reveals a highly complex landscape\nof magnetic phases arising from an antiferromagnetic ground state.\nA series of metamagnetic transitions creates at least 5 unique magnetic\nphase pockets, including a 1/3 and 2/3 magnetization plateau. Further,\nthe system exhibits an intimate connection between the magnetism and\nmagnetotransport, exhibiting sharp switching from positive (+40%)\nto negative magnetoresistance (−50%). Like the LnTi&lt;sub&gt;3&lt;/sub&gt;Bi&lt;sub&gt;4&lt;/sub&gt; kagome metals, the Ln&lt;sub&gt;2&lt;/sub&gt;&lt;sub&gt;–&lt;/sub&gt;&lt;sub&gt;&lt;i&gt;x&lt;/i&gt;&lt;/sub&gt;Ti&lt;sub&gt;6+&lt;i&gt;x&lt;/i&gt;&lt;/sub&gt;Bi&lt;sub&gt;9&lt;/sub&gt; family exhibits quasi-2D networks of titanium and chains\nof rare earth. We present the structures and some basic magnetic properties\nof the Ln&lt;sub&gt;2&lt;/sub&gt;&lt;sub&gt;–&lt;/sub&gt;&lt;sub&gt;&lt;i&gt;x&lt;/i&gt;&lt;/sub&gt;Ti&lt;sub&gt;6+&lt;i&gt;x&lt;/i&gt;&lt;/sub&gt;Bi&lt;sub&gt;9&lt;/sub&gt; family alongside\nour characterization of the newly discovered TbTi&lt;sub&gt;3&lt;/sub&gt;Bi&lt;sub&gt;4&lt;/sub&gt;.

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