arXiv (Cornell University),
Journal Year:
2023,
Volume and Issue:
unknown
Published: Jan. 1, 2023
\textit{Holey
Graphene}
(HG)
is
a
widely
used
graphene
material
for
the
synthesis
of
high-purity
and
highly
crystalline
materials.
In
this
work,
we
explore
electronic
properties
periodic
distribution
lattice
holes,
demonstrating
emergence
flat
bands
with
compact
localized
states.
It
shown
that
holes
break
bipartite
sublattice
inversion
symmetries,
inducing
gaps
nonzero
Berry
curvature.
Moreover,
folding
Dirac
cones
from
hexagonal
Brillouin
zone
(BZ)
to
holey
superlattice
rectangular
BZ
HG
sizes
proportional
an
integer
$n$
times
graphene's
parameter
leads
periodicity
in
gap
formation
such
$n
\equiv
0$
(mod
$3$).
Meanwhile,
it
if
\pm
1$
$3$),
emerges
where
points
are
folded
along
$\Gamma-X$
path.
The
low-energy
hamiltonian
three
central
also
obtained,
revealing
system
behaves
as
effective
$\alpha-\mathcal{T}_{3}$
material.
Therefore,
simple
protocol
presented
here
allows
obtaining
at
will.
Such
known
increase
electron-electron
correlated
effects.
This
work
provides
alternative
system,
much
easier
build
than
twisted
systems,
obtain
quantum
phases.
Reports on Progress in Physics,
Journal Year:
2023,
Volume and Issue:
87(1), P. 016502 - 016502
Published: Oct. 25, 2023
Abstract
This
is
an
update
of
a
previous
review
(Naumis
et
al
2017
Rep.
Prog.
Phys.
80
096501).
Experimental
and
theoretical
advances
for
straining
graphene
other
metallic,
insulating,
ferroelectric,
ferroelastic,
ferromagnetic
multiferroic
2D
materials
were
considered.
We
surveyed
(i)
methods
to
induce
valley
sublattice
polarisation
(
P
)
in
graphene,
(ii)
time-dependent
strain
its
impact
on
graphene’s
electronic
properties,
(iii)
the
role
local
global
superconductivity
highly
correlated
and/or
topological
phases
(iv)
inducing
hexagonal
boron
nitride
monolayers
via
strain,
(v)
modifying
optoelectronic
properties
transition
metal
dichalcogenide
through
(vi)
ferroic
with
intrinsic
elastic
σ
),
electric
magnetic
M
under
as
well
incipient
multiferroics
(vii)
moiré
bilayers
exhibiting
flat
bands
exotic
quantum
phase
diagrams,
bilayer
or
few-layer
systems
orders
tunable
by
rotations
shear
strain.
The
features
experimental
realisations
two-dimensional
Quantum
Spin
Hall
effect
germanene,
elemental
ferroelectric
bismuth,
NiI
2
.
document
was
structured
discussion
effects
taking
place
first,
followed
discussions
concerning
few-layers,
it
represents
up-to-date
overview
exciting
newest
developments
fast-paced
field
materials.
Condensed Matter,
Journal Year:
2025,
Volume and Issue:
10(1), P. 10 - 10
Published: Feb. 7, 2025
We
explore
the
equivalence
between
low-energy
dynamics
of
strained
graphene
and
a
quantum
mechanical
framework
for
2D
Dirac
equation
in
flat
space
with
deformed
momentum
operator.
By
considering
some
common
forms
anisotropic
Fermi
velocity
tensor
emerging
from
elasticity
theory,
we
associate
such
deformation
first
bound
states
charge
carriers
background
uniform
magnetic
field
this
quantify
impact
strain
energy
spectrum.
Then,
use
quadrature
algebra
formula
as
mathematical
tool
to
analyze
attached
operator
identify
physical
consequences
terms
modifications
due
applied
strain.
Physical review. E,
Journal Year:
2025,
Volume and Issue:
111(3)
Published: March 13, 2025
We
theoretically
investigate
the
quantum
percolation
problem
on
Lieb
lattices
in
two
and
three
dimensions.
study
statistics
of
energy
levels
through
random
matrix
theory
determine
level
spacing
distributions,
which,
with
aid
finite-size
scaling
theory,
allows
us
to
obtain
accurate
estimates
for
site-
bond-percolation
thresholds
critical
exponents.
Our
numerical
investigation
supports
a
localized-delocalized
transition
at
finite
threshold,
which
decreases
as
average
coordination
number
increases.
The
precise
determination
localization
length
exponent
enables
claim
that
problems
belong
same
universality
class,
ν
decreasing
lattice
dimensionality
d,
similarly
classical
problem.
In
addition,
we
verify
that,
dimensions,
belongs
class
Anderson
impurity
model.
Journal of Physics Conference Series,
Journal Year:
2025,
Volume and Issue:
2986(1), P. 012003 - 012003
Published: March 1, 2025
Abstract
Approximate
solutions
for
a
electron
in
uniaxially
strained
graphene
have
been
determined.
A
first-order
Taylor
expansion
the
Fermi
velocities
and
pseudo-vector
potential,
effective
Hamiltonian
describing
graphene,
allows
us
to
solve
corresponding
differential
equation
of
eigenvalue
problem.
finite
number
bound
states
found
its
spectrum
is
compared
with
zero-order
approximation
derived
[1].
It
turns
out
that
generated
less
energy
levels
than
approximation,
revealing
suppression
mechanism
deletes
some
levels.
In
an
infinite
twisted
bilayer
graphene
lattice,
flat
bands
emerge,
representing
electrons
localized
at
the
AA
stacking
regions.
This
study
investigates
behavior
of
these
when
dealing
with
incomplete
moir\'e
supercells
in
nanoribbons.
The
findings
reveal
a
transition
from
dispersive
to
near
charge
neutrality
as
supercell
completeness
varies.
Moreover,
it
is
observed
that
microscopic
edges
can
influence
energy
states
regions
borders.
Twisted
bilayer
graphene
(TBG)
is
known
for
exhibiting
highly
correlated
phases
at
magic
angles
due
to
the
emergence
of
flat
bands
that
enhance
electron-electron
interactions.
The
connection
between
and
quantum
Hall
effect
remains
a
topic
ongoing
research.
In
TBG
chiral
model,
electronic
wave
function
properties
depend
on
single
parameter
($\ensuremath{\alpha}$),
inversely
proportional
relative
twist
angle
two
layers
($\ensuremath{\theta}$),
which
includes
interlayer
interaction
strength.
previous
studies,
as
approached
small
values,
strong
confinement
convergence
coherent
Landau
states
were
observed.
However,
origin
these
phenomena
remained
elusive.
this
paper,
we
explore
band
modes,
revealing
exhibit
self-duality;
they
are
in
reciprocal
space
minimal
dispersion,
with
standard
deviation
${\ensuremath{\sigma}}_{k}=\sqrt{3\ensuremath{\alpha}/2\ensuremath{\pi}}$
$\ensuremath{\theta}\ensuremath{\rightarrow}0$.
Subsequently,
by
symmetrizing
functions
considering
squared
Hamiltonian,
observed
$\ensuremath{\theta}\ensuremath{\rightarrow}0$
limit
explained.
This
arises
from
combination
symmetrized
norm
moir\'e
potential
quantized
orbital
motion
electrons,
effectively
creating
well.
ground
state
well,
located
non-high-symmetry
spots,
corresponds
level.
Furthermore,
demonstrate
problem
physically
analogous
an
electron
attached
non-Abelian
$\text{SU}(2)$
gauge
field
underlying
${C}_{3}$
symmetry.
regions
confinement,
system
can
be
considered
Abelian,
aligning
picture
simple
harmonic
oscillator.
allows
us
define
magnetic
energy
important
role
parity
gap
closing
nonmagic
revealed.
Finally,
investigate
transition
original
nature
Abelian
artificially
changing
pseudomagnetic
vector
components
U(1)
field,
alters
sequence
angles.
An
experimental
proposal
made
measure
such
effects.
Nonuniform
strain
in
graphene
can
induce
a
pseudo-magnetic
field
(PMF)
preserving
time-reversal
symmetry,
generating
pseudo-Landau
levels
under
zero
real
magnetic
(MF).
The
different
natures
between
PMF
and
MF
lead
to
the
counterpropagating
valley-polarized
edge
states
unidirectionally
chiral
MF.
In
this
work,
we
find,
due
valley
mixing
on
armchair
edges,
quantum
Hall
only
exist
at
zigzag
edges
but
not
uniaxial
strained
graphene,
very
from
case
that
all
pristine
We
theoretically
demonstrate
it
through
wave
function
distributions,
multi-terminal
transport
measurements
electron
local
occupations,
respectively.
interface
state
p-n
junction
is
further
proposed
electrons
conductive
boundaries,
which
could
be
used
as
single
pole
double
throw
switch.