Weyl nodal loop semimetals and tunable quantum anomalous Hall states in two-dimensional ferromagnetic cerium monohalides
Shu-Zong Li,
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Jun‐Shan Si,
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Zhixiong Yang
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et al.
Physical review. B./Physical review. B,
Journal Year:
2024,
Volume and Issue:
109(11)
Published: March 13, 2024
Quantum
anomalous
Hall
(QAH)
effect
with
dissipationless
edge
channels
offers
innovative
insight
for
designing
the
next-generation
low-power
electronic
devices.
Based
on
first-principles
calculations
and
tight-binding
(TB)
model,
we
predict
rich
QAH
states
a
tunable
Chern
number
in
single-layer
ferromagnetic
cerium
monohalides
$\mathrm{Ce}X$
($X$
=
Cl,
Br,
I).
These
stable
materials
have
isotropic
magnetocrystalline
anisotropy
$x\text{\ensuremath{-}}y$
plane,
which
favors
adjustment
of
topological
state
an
external
magnetic
field.
A
distinct
Weyl
nodal
loop
exists
band
structure
single
layers
without
spin-orbit
coupling
(SOC).
When
SOC
is
included
all
mirror
symmetries
are
broken,
can
be
realized.
Intriguingly,
varying
($C=\ifmmode\pm\else\textpm\fi{}1$),
two-dimensional
semimetals
gap
periodically
manifest
as
magnetization
direction
rotates
plane.
Furthermore,
TB
model
based
Slater-Koster
framework
constructed
to
explain
origin
nontrivial
layers.
The
exhibit
remarkable
states,
providing
excellent
platform
exploring
spintronic
Language: Английский
Magnetization direction-controlled topological band structure in TlTiX (X = Si, Ge) monolayers
Keer Huang,
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Lei Li,
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Wu Zhao
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et al.
Journal of Physics Condensed Matter,
Journal Year:
2024,
Volume and Issue:
36(22), P. 225702 - 225702
Published: Feb. 21, 2024
The
quantum
anomalous
Hall
(QAH)
insulator
is
a
vital
material
for
the
investigation
of
emerging
topological
effects,
but
its
extremely
low
working
temperature
limits
experiments.
Apart
from
challenge,
effective
regulation
state
QAH
insulators
another
crucial
concern.
Here,
by
first-principles
calculations,
we
find
family
stable
two-dimensional
materials
TlTiX
(X
=
Si,
Ge)
are
large-gap
insulators.
Their
robust
ferromagnetic
(FM)
ground
states
determined
both
direct-
and
super-exchange
FM
coupling.
In
absence
spin-orbit
coupling
(SOC),
there
exist
spin-polarized
crossing
point
located
at
each
Language: Английский