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Superexchange and charge transfer in the nickelate superconductor La3Ni2O7 under pressure
Recently, a bulk nickelate superconductor La 3 Ni 2 O 7 is discovered at pressures with a remarkable high transition temperature T c ∼ 80 K. Here, we study a Hubbard model with tight-binding parameters derived from ab initio calculations of La 3 Ni 2 O 7 , by employing large scale determinant quantu...
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Published in: | Science China. Physics, mechanics & astronomy mechanics & astronomy, 2024-11, Vol.67 (11), p.117402, Article 117402 |
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Main Authors: | , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | Recently, a bulk nickelate superconductor La
3
Ni
2
O
7
is discovered at pressures with a remarkable high transition temperature T
c
∼ 80 K. Here, we study a Hubbard model with tight-binding parameters derived from
ab initio
calculations of La
3
Ni
2
O
7
, by employing large scale determinant quantum Monte Carlo and cellular dynamical mean-field theory. Our result suggests that the superexchange couplings in this system are comparable to that of cuprates. The system is a charge transfer insulator as the hole concentration becomes four per site at large Hubbard
U
. Upon hole doping, two low-energy spin-singlet bands emerge in the system exhibiting distinct correlation properties: while the one composed of the out-of-plane
Ni-
d
3
z
2
−
r
2
and O-
p
z
orbitals demonstrates strong antiferromagnetic correlations and narrow effective bandwidth, the in-plane singlet band consisting of the
Ni-
d
x
2
−
y
2
and O-
p
x
/
p
y
orbitals is in general more itinerant. Over a broad range of hole doping, the doped holes occupy primarily the
d
x
2
−
y
2
and
p
x
/
p
y
orbitals, whereas the
d
3
z
2
−
r
2
and
p
z
orbitals retain underdoped. We propose an effective
t
-
J
model to capture the relevant physics and discuss the implications of our result for comprehending the La
3
Ni
2
O
7
superconductivity. |
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ISSN: | 1674-7348 1869-1927 |
DOI: | 10.1007/s11433-023-2300-4 |