Electron-Correlation-Induced Charge Density Wave in FeGe
As the first magnetic kagome material to exhibit the charge density wave (CDW) order, FeGe has attracted much attention in recent research. Similar to A V 3 Sb 5 ( A = K, Cs, Rb), FeGe exhibits the CDW pattern with an in-plane 2×2 structure and the existence of van Hove singularities near the Fermi...
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Published in | Chinese physics letters Vol. 40; no. 11; pp. 117103 - 138 |
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Main Authors | , , , , |
Format | Journal Article |
Language | English |
Published |
Chinese Physical Society and IOP Publishing Ltd
01.11.2023
|
Online Access | Get full text |
ISSN | 0256-307X 1741-3540 1741-3540 |
DOI | 10.1088/0256-307X/40/11/117103 |
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Summary: | As the first magnetic kagome material to exhibit the charge density wave (CDW) order, FeGe has attracted much attention in recent research. Similar to
A
V
3
Sb
5
(
A
= K, Cs, Rb), FeGe exhibits the CDW pattern with an in-plane 2×2 structure and the existence of van Hove singularities near the Fermi level. However, sharply different from
A
V
3
Sb
5
which has phonon instability at
M
point, all the theoretically calculated phonon frequencies in FeGe remain positive. Based on first-principles calculations, we surprisingly find that the maximum of nesting function is at
K
point instead of
M
point. Two Fermi pockets with Fe-
d
xz
and Fe-
d
x
2
–
y
2
/
d
xy
orbital characters have large contribution to the Fermi nesting, which evolve significantly with
k
z
, indicating the highly three-dimensional (3D) feature of FeGe in contrast to
A
V
3
Sb
5
. Considering the effect of local Coulomb interaction, we reveal that the instability at
K
point is significantly suppressed due to the sublattice interference mechanism. Meanwhile, the wave functions nested by vector
M
have many ingredients located at the same Fe site, thus the instability at
M
point is enhanced. This indicates that the electron correlation, rather than electron-phonon interaction, plays a key role in the CDW transition at
M
point. |
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ISSN: | 0256-307X 1741-3540 1741-3540 |
DOI: | 10.1088/0256-307X/40/11/117103 |