Inorganic Chemistry,
Journal Year:
2025,
Volume and Issue:
unknown
Published: Jan. 10, 2025
A
recent
article
(
J.
Am.
Chem.
Soc.
2024,
146,
7506–7514)
details
a
pressure–temperature
(P–T)
phase
diagram
for
the
Ruddlesden–Popper
bilayer
nickelate
La3Ni2O7
(LNO-2222)
using
synchrotron
X-ray
diffraction.
This
study
identifies
transition
from
Amam
(#63)
to
Fmmm
(#69)
within
temperature
range
of
104–120
K
under
initial
pressure
and
attributes
I4/mmm
(#139)
space
group
structure
responsible
superconductivity
LNO-2222.
Herein,
we
examine
temperature-dependent
structural
evolution
LNO-2222
single
crystals
at
ambient
pressure.
Contrary
symmetry
increase
established
Amam–Fmmm
boundary,
observe
an
enhancement
in
reflections
as
decreases.
work
not
only
delivers
high-quality
crystallographic
data
laboratory
X-rays
across
various
temperatures
but
also
enhances
understanding
complex
behavior
this
system,
contributing
insights
further
experimental
theoretical
explorations.
The Innovation Materials,
Journal Year:
2024,
Volume and Issue:
2(4), P. 100102 - 100102
Published: Jan. 1, 2024
<p>Identifying
the
key
factors
controlling
magnitude
of
<i>T</i><sub><i>c</i></sub>
is
critical
importance
in
pursuit
high-temperature
superconductivity.
In
cuprates,
reaches
its
maximal
value
trilayer
structure,
leading
to
belief
that
interlayer
coupling
may
help
promote
pairing.
contrast,
for
recently
discovered
nickelate
superconductors
under
high
pressure,
maximum
reduced
from
about
80
K
bilayer
La<sub>3</sub>Ni<sub>2</sub>O<sub>7</sub>
30
La<sub>4</sub>Ni<sub>3</sub>O<sub>10</sub>.
Motivated
by
this
opposite
trend,
we
propose
an
pairing
scenario
superconductivity
Our
theory
reveals
intrinsic
frustration
spin-singlet
inner
layer
tends
form
with
both
two
outer
layers
respectively,
strong
superconducting
fluctuations
between
layers.
This
explains
reduction
compared
La<sub>3</sub>Ni<sub>2</sub>O<sub>7</sub>.
findings
support
a
fundamental
distinction
multilayer
and
cuprate
superconductors,
ascribe
it
their
different
(interlayer
versus
intralayer)
mechanisms.
Furthermore,
our
predicts
extended
<i>s</i><sup><i>±</i></sup>-wave
gap
structures
La<sub>4</sub>Ni<sub>3</sub>O<sub>10</sub>,
varying
signs
possible
nodes
on
Fermi
pockets.
We
also
find
Josephson
potentially
interesting
consequences
be
examined
future
experiments.
work
possibility
rich
novel
physics
pairing.</p>
Advanced Electronic Materials,
Journal Year:
2024,
Volume and Issue:
10(9)
Published: May 1, 2024
Abstract
Recently,
superconductivity
at
high
temperatures
is
observed
in
bulk
La
3
Ni
2
O
7−δ
under
pressure.
However,
the
attainment
of
high‐purity
single
crystals
remains
a
formidable
challenge.
Here,
crystal
structure
and
physical
properties
Sr‐doped
7
synthesized
pressure
(20
GPa)
temperature
(1400
°C)
are
reported.
Through
X‐ray
diffraction,
it
shown
that
high‐pressure‐synthesized
paramagnetic
crystallizes
an
orthorhombic
with
Ni─O─Ni
bond
angles
173.4(2)°
out‐of‐plane
175.0(2)°and
176.7(2)°in
plane.
The
substitution
Sr
alters
band
filling
ratio
2+
/Ni
3+
,
aligning
them
those
“La
7.05”
thereby
leading
to
significant
modifications
relative
unsubstituted
parent
phase.
At
ambient
pressure,
exhibits
insulating
properties,
conductivity
increases
as
goes
up
10
GPa.
upon
further
increasing
beyond
10.7
GPa,
transits
back
from
metal‐like
behavior
insulator.
insulator–metal–insulator
trend
dramatically
differs
compound
despite
their
similar
low‐pressure
regime.
These
experimental
results
underscore
considerable
challenge
achieving
nickelates.
Recently,
evidence
of
superconductivity
(SC)
has
been
reported
in
pressurized
${\mathrm{La}}_{4}{\mathrm{Ni}}_{3}{\mathrm{O}}_{10}$.
Here
we
study
its
possible
pairing
mechanism
and
symmetry.
Through
fitting
the
density-functional-theory
band
structure,
provide
a
six-orbital
tight-binding
model.
In
comparison
with
structure
${\mathrm{La}}_{3}{\mathrm{Ni}}_{2}{\mathrm{O}}_{7}$,
additional
nonbonding
${d}_{{z}^{2}}$
is
important
to
here.
When
multiorbital
Hubbard
interactions
are
included,
our
random-phase-approximation
based
yields
an
${s}^{\ifmmode\pm\else\textpm\fi{}}$-wave
SC.
The
dominant
Fermi-surface
nesting
vector
${\mathbf{Q}}_{1}\ensuremath{\approx}(\ensuremath{\pi},\ensuremath{\pi})$
between
$\ensuremath{\gamma}$
pocket
contributed
by
bonding
top
${\ensuremath{\alpha}}_{1}$
bottom,
leading
strongest
amplitude
opposite
gap
signs
within
two
regimes.
real-space
interlayer
${d}_{{z}^{2}}$-orbital
pairing.
This
pattern
insensitive
details.
Upon
electron
doping,
${T}_{c}$
would
increase
promptly
before
system
enters
N\'eel-ordered
spin-density-wave
phase.
Inorganic Chemistry,
Journal Year:
2025,
Volume and Issue:
unknown
Published: Jan. 10, 2025
A
recent
article
(
J.
Am.
Chem.
Soc.
2024,
146,
7506–7514)
details
a
pressure–temperature
(P–T)
phase
diagram
for
the
Ruddlesden–Popper
bilayer
nickelate
La3Ni2O7
(LNO-2222)
using
synchrotron
X-ray
diffraction.
This
study
identifies
transition
from
Amam
(#63)
to
Fmmm
(#69)
within
temperature
range
of
104–120
K
under
initial
pressure
and
attributes
I4/mmm
(#139)
space
group
structure
responsible
superconductivity
LNO-2222.
Herein,
we
examine
temperature-dependent
structural
evolution
LNO-2222
single
crystals
at
ambient
pressure.
Contrary
symmetry
increase
established
Amam–Fmmm
boundary,
observe
an
enhancement
in
reflections
as
decreases.
work
not
only
delivers
high-quality
crystallographic
data
laboratory
X-rays
across
various
temperatures
but
also
enhances
understanding
complex
behavior
this
system,
contributing
insights
further
experimental
theoretical
explorations.