- Feature Paper
- Article
Measurements of Electronic Band Structure in CeCoGe3 by Angle-Resolved Photoemission Spectroscopy
- Robert Prater,
- Mingkun Chen and
- Inna Vishik
- + 7 authors
In this paper, we present a comprehensive study of the electronic structure of CeCoGe3 throughout the entire Brillouin zone in the non-magnetic regime using angle-resolved photoemission spectroscopy (ARPES). The electronic structure agrees in large part with first principles calculations, including predicted topological nodal lines. Two new features in the band structure are also observed, namely a surface state and folded bands, the latter of which is argued to originate from a unit cell reconstruction.
25 February 2026





![The NMR spin shift
K
i
(
T
)
is proportional to the electronic spin susceptibility
χ
(
T
)
in accordance with
K
i
(
T
)
=
A
i
·
χ
(
T
)
, cf. (1), where
A
i
is the associated temperature-independent hyperfine constant describing the coupling between the electron and nuclear spins (
H
i
=
I
A
i
S
). (a) A plot of shift
K
i
α
(
T
)
versus shift
K
j
β
(
T
)
with temperature as an implicit parameter. For different materials (indicated by three different colors), lines fall on top of each other in the case where the relevant hyperfine constants are material-independent. This was initially proposed for the cuprate shifts based upon a few early studies [16,17] but was found to fail as additional materials were investigated. (b) Material-dependent temperature dependencies of any two spin shifts remain proportional to each other so long as they result from the same spin susceptibility. The ratio of the relevant hyperfine constants is the proportionality factor. This scenario has been previously proposed to explain the aforementioned disparate behavior of the shifts in various cuprates [19]. However, the temperature dependencies of, e.g., the spin shifts at planar Cu actually follow the sketch shown in (c). The abrupt changes in slope between the two shifts as a function of temperature are evidence of the action of two susceptibilities. Note that abrupt changes in the hyperfine constants would result in discontinuities in the temperature dependence of individual shifts, which are not observed.](https://mdpi-res.com/cdn-cgi/image/w=281,h=192/https://mdpi-res.com/condensedmatter/condensedmatter-11-00005/article_deploy/html/images/condensedmatter-11-00005-g001-550.jpg)

