Saved in:
Bibliographic Details
Main Authors: Taddei, Keith M., Ranmohotti, Kulugammana G. S., Liurukara, Duminda S., Martinson, Alex, Calder, Stuart, Samolyuk, German, Pokhrel, Nabaraj, Phelan, Daniel, Parker, David
Format: Preprint
Published: 2025
Subjects:
Online Access:https://arxiv.org/abs/2508.20247
Tags: Add Tag
No Tags, Be the first to tag this record!
_version_ 1866911127170973696
author Taddei, Keith M.
Ranmohotti, Kulugammana G. S.
Liurukara, Duminda S.
Martinson, Alex
Calder, Stuart
Samolyuk, German
Pokhrel, Nabaraj
Phelan, Daniel
Parker, David
author_facet Taddei, Keith M.
Ranmohotti, Kulugammana G. S.
Liurukara, Duminda S.
Martinson, Alex
Calder, Stuart
Samolyuk, German
Pokhrel, Nabaraj
Phelan, Daniel
Parker, David
contents The ideal Weyl 'Hydrogen-atom' semi-metal exhibits only a single pair of Weyl nodes and no other trivial states at the Fermi energy. Such a material would be a panacea in the study of Weyl quasi particles allowing direct unambiguous observation of their topological properties. The alluaudite-like K$_2$Mn$_3$(AsO$_4$)$_3$ compound was recently proposed as such a material. Here we use comprehensive experimental work and first principle calculations to assess this prediction. We find K$_2$Mn$_3$(AsO$_4$)$_3$ crystallizes in the $C2/c$ symmetry with a quasi-1D Mn sublattice, growing as small needle-like crystals. Bulk properties measurements reveal magnetic transitions at $\approx$ 8 and $\approx$ 4 K which neutron scattering experiments show correspond to two distinct magnetic orders, first a partially ordered ferrimagnetic $\mathbf{k_1}$= (0, 0, 0) structure at 8 K and a second transition of $\mathbf{k_2}$= (1, 0, 0) at 4 K to a fully ordered state. Below the second transition, both ordering vectors are necessary to describe the complex magnetic structure with modulated spin magnitudes. Both of the best-fit magnetic structures in this work are found to break the symmetry necessary for the generation of the Weyl nodes, though one of the magnetic structures allowed by $\mathbf{k_1}$ does preserve this symmetry. However, the crystals are optically transparent and ellipsometry measurements reveal a large band-gap, undermining expectations of semi-metallic behavior. Density functional theory calculations predict an insulating antiferromagnetic ground state, in contrast to previous reports, and suggest potential frustration on the magnetic sublattice. Given the wide tunability of the alluaudite structure we consider ways to push the system closer to semi-metallic state.
format Preprint
id arxiv_https___arxiv_org_abs_2508_20247
institution arXiv
publishDate 2025
record_format arxiv
spellingShingle Insulating ground state and 2-k magnetic structure of candidate Weyl Hydrogen atom K$_2$Mn$_3$(AsO$_4$)$_3$
Taddei, Keith M.
Ranmohotti, Kulugammana G. S.
Liurukara, Duminda S.
Martinson, Alex
Calder, Stuart
Samolyuk, German
Pokhrel, Nabaraj
Phelan, Daniel
Parker, David
Strongly Correlated Electrons
The ideal Weyl 'Hydrogen-atom' semi-metal exhibits only a single pair of Weyl nodes and no other trivial states at the Fermi energy. Such a material would be a panacea in the study of Weyl quasi particles allowing direct unambiguous observation of their topological properties. The alluaudite-like K$_2$Mn$_3$(AsO$_4$)$_3$ compound was recently proposed as such a material. Here we use comprehensive experimental work and first principle calculations to assess this prediction. We find K$_2$Mn$_3$(AsO$_4$)$_3$ crystallizes in the $C2/c$ symmetry with a quasi-1D Mn sublattice, growing as small needle-like crystals. Bulk properties measurements reveal magnetic transitions at $\approx$ 8 and $\approx$ 4 K which neutron scattering experiments show correspond to two distinct magnetic orders, first a partially ordered ferrimagnetic $\mathbf{k_1}$= (0, 0, 0) structure at 8 K and a second transition of $\mathbf{k_2}$= (1, 0, 0) at 4 K to a fully ordered state. Below the second transition, both ordering vectors are necessary to describe the complex magnetic structure with modulated spin magnitudes. Both of the best-fit magnetic structures in this work are found to break the symmetry necessary for the generation of the Weyl nodes, though one of the magnetic structures allowed by $\mathbf{k_1}$ does preserve this symmetry. However, the crystals are optically transparent and ellipsometry measurements reveal a large band-gap, undermining expectations of semi-metallic behavior. Density functional theory calculations predict an insulating antiferromagnetic ground state, in contrast to previous reports, and suggest potential frustration on the magnetic sublattice. Given the wide tunability of the alluaudite structure we consider ways to push the system closer to semi-metallic state.
title Insulating ground state and 2-k magnetic structure of candidate Weyl Hydrogen atom K$_2$Mn$_3$(AsO$_4$)$_3$
topic Strongly Correlated Electrons
url https://arxiv.org/abs/2508.20247