Crystal Growth and Physical Properties of Orthorhombic Kagome Lattice Magnets $R$Fe$_6$Ge$_6$ ($R$=Y, Tb, Dy)

Fuente: arXiv
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Autori principali: Nayak, Abhijeet, Jamaluddin, Sk, Wu, Fan, Rapp, Emily, Regmi, Resham Babu, Gazzah, Mohamed El, Márkus, Bence G., Forró, László, Ghimire, Madhav P., Oliver, Allen, Foyevtsova, Kateryna, Mazin, Igor I., Ghimire, Nirmal J.
Natura: Preprint
Pubblicazione: 2025
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author Nayak, Abhijeet
Jamaluddin, Sk
Wu, Fan
Rapp, Emily
Regmi, Resham Babu
Gazzah, Mohamed El
Márkus, Bence G.
Forró, László
Ghimire, Madhav P.
Oliver, Allen
Foyevtsova, Kateryna
Mazin, Igor I.
Ghimire, Nirmal J.
author_facet Nayak, Abhijeet
Jamaluddin, Sk
Wu, Fan
Rapp, Emily
Regmi, Resham Babu
Gazzah, Mohamed El
Márkus, Bence G.
Forró, László
Ghimire, Madhav P.
Oliver, Allen
Foyevtsova, Kateryna
Mazin, Igor I.
Ghimire, Nirmal J.
contents Kagome magnets represent a promising class of materials that exhibit intriguing electronic and magnetic properties, and they have recently garnered significant attention. While most kagome-lattice compounds are hexagonal, we report here single-crystal growth and physical property measurements of $R$Fe$_6$Ge$_6$ ($R$ = Y, Dy, Tb) compounds, which crystallize in an orthorhombic structure. The structure can be derived from a hexagonal prototype $R$Fe$_3$Ge$_2$ by replacing every other $R$ atom with a covalent Ge$_2$ dimer. Ordering of these dimers renders the structure orthorhombic, slightly distorts the kagome net, and makes the three Fe sites formally inequivalent. The iron and rare-earth sublattices order independently. Fe moments order above 400 K, forming ferromagnetic kagome planes stacked antiferromagnetically, while rare-earth moments order below 9 K. TbFe$_6$Ge$_6$ exhibits a single magnetic ordering transition associated with the Tb atoms, whereas DyFe$_6$Ge$_6$ shows two distinct magnetic phase transitions, strongly influenced by crystal electric field effects on the Dy$^{3+}$ ions. Density functional theory (DFT) calculations indicate that the ferromagnetic ordering of the Fe planes is driven by a high density of states at the Fermi energy. They also reveal three dramatically different structural energy scales: $R$ and Ge$_2$ form alternating 1D chains perpendicular to the kagome planes, and violating this alternation incurs a large energy cost. Aligning these chains is less costly, and achieving a two-dimensional order of anti-aligned chains requires very little energy. These compounds represent a unique class of materials, offering new opportunities to investigate the interplay between the distinct crystal lattice geometry and the underlying electronic and magnetic properties.
format Preprint
id arxiv_https___arxiv_org_abs_2511_17398
institution arXiv
publishDate 2025
record_format arxiv
spellingShingle Crystal Growth and Physical Properties of Orthorhombic Kagome Lattice Magnets $R$Fe$_6$Ge$_6$ ($R$=Y, Tb, Dy)
Nayak, Abhijeet
Jamaluddin, Sk
Wu, Fan
Rapp, Emily
Regmi, Resham Babu
Gazzah, Mohamed El
Márkus, Bence G.
Forró, László
Ghimire, Madhav P.
Oliver, Allen
Foyevtsova, Kateryna
Mazin, Igor I.
Ghimire, Nirmal J.
Materials Science
Strongly Correlated Electrons
Kagome magnets represent a promising class of materials that exhibit intriguing electronic and magnetic properties, and they have recently garnered significant attention. While most kagome-lattice compounds are hexagonal, we report here single-crystal growth and physical property measurements of $R$Fe$_6$Ge$_6$ ($R$ = Y, Dy, Tb) compounds, which crystallize in an orthorhombic structure. The structure can be derived from a hexagonal prototype $R$Fe$_3$Ge$_2$ by replacing every other $R$ atom with a covalent Ge$_2$ dimer. Ordering of these dimers renders the structure orthorhombic, slightly distorts the kagome net, and makes the three Fe sites formally inequivalent. The iron and rare-earth sublattices order independently. Fe moments order above 400 K, forming ferromagnetic kagome planes stacked antiferromagnetically, while rare-earth moments order below 9 K. TbFe$_6$Ge$_6$ exhibits a single magnetic ordering transition associated with the Tb atoms, whereas DyFe$_6$Ge$_6$ shows two distinct magnetic phase transitions, strongly influenced by crystal electric field effects on the Dy$^{3+}$ ions. Density functional theory (DFT) calculations indicate that the ferromagnetic ordering of the Fe planes is driven by a high density of states at the Fermi energy. They also reveal three dramatically different structural energy scales: $R$ and Ge$_2$ form alternating 1D chains perpendicular to the kagome planes, and violating this alternation incurs a large energy cost. Aligning these chains is less costly, and achieving a two-dimensional order of anti-aligned chains requires very little energy. These compounds represent a unique class of materials, offering new opportunities to investigate the interplay between the distinct crystal lattice geometry and the underlying electronic and magnetic properties.
title Crystal Growth and Physical Properties of Orthorhombic Kagome Lattice Magnets $R$Fe$_6$Ge$_6$ ($R$=Y, Tb, Dy)
topic Materials Science
Strongly Correlated Electrons
url https://arxiv.org/abs/2511.17398