Electronic Origin of High- TCMaximization and Persistence in Trilayer Cuprate Superconductors Xiangyu Luo13y Hao Chen13y Yinghao Li13y Qiang Gao1 Chaohui Yin13 Hongtao

2025-04-26 0 0 888.87KB 20 页 10玖币
侵权投诉
Electronic Origin of High-TCMaximization and Persistence in
Trilayer Cuprate Superconductors
Xiangyu Luo1,3,, Hao Chen1,3,, Yinghao Li1,3,, Qiang Gao1, Chaohui Yin1,3, Hongtao
Yan1,3, Taimin Miao1,3, Hailan Luo1,3, Yingjie Shu1,3, Yiwen Chen1,3, Chengtian Lin4,
Shenjin Zhang5, Zhimin Wang5, Fengfeng Zhang5, Feng Yang5, Qinjun Peng5,
Guodong Liu1,3,6, Lin Zhao1,3,6, Zuyan Xu5, Tao Xiang2,3,6,7and X. J. Zhou1,3,6,7,
1National Lab for Superconductivity,
Beijing National laboratory for Condensed Matter Physics,
Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
2Beijing National laboratory for Condensed Matter Physics,
Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
3University of Chinese Academy of Sciences, Beijing 100049, China
4Max Planck Institute for Solid State Research,
Heisenbergstrasse 1, D-70569 Stuttgart, Germany
5Technical Institute of Physics and Chemistry,
Chinese Academy of Sciences, Beijing 100190, China
6Songshan Lake Materials Laboratory,
Dongguan, Guangdong 523808, China
7Beijing Academy of Quantum Information Sciences, Beijing 100193, China
These authors contributed equally to this work.
Corresponding author: XJZhou@iphy.ac.cn
(Dated: October 13, 2022)
1
arXiv:2210.06348v1 [cond-mat.supr-con] 12 Oct 2022
In high temperature cuprate superconductors, it was found that the super-
conducting transition temperature Tcdepends on the number of CuO2planes
(n) in the structural unit and the maximum Tcis realized in the trilayer system
(n=3). It was also found that the trilayer superconductors exhibit an unusual
phase diagram that Tckeeps nearly constant in the overdoped region which is
in strong contrast to the Tcdecrease usually found in other cuprate supercon-
ductors. The electronic origin of the Tcmaximization in the trilayer supercon-
ductors and its high Tcpersistence in the overdoped region remains unclear.
By taking high resolution laser-based angle resolved photoemission (ARPES)
measurements, here we report our revelation of the microscopic origin of the
unusual superconducting properties in the trilayer superconductors. For the
first time we have observed the trilayer splitting in Bi2Sr2Ca2Cu3O10+δ(Bi2223)
superconductor. The observed Fermi surface, band structures, superconducting
gap and the selective Bogoliubov band hybridizations can be well described by
a three-layer interaction model. Quantitative information of the microscopic
processes involving intra- and interlayer hoppings and pairings are extracted.
The electronic origin of the maximum Tcin Bi2223 and the persistence of the
high Tcin the overdoped region is revealed. These results provide key insights
in understanding high Tcsuperconductivity and pave a way to further enhance
Tcin the cuprate superconductors.
Although significant progress has been made in experimental and theoretical studies of
high temperature cuprate superconductors, the mechanism of high temperature supercon-
ductivity remains a prominent issue in condensed matter physics[1, 2]. In addition to pinning
down on the microscopic origin of electron pairing, the challenge also lies in uncovering the
key ingredients that dictate high temperature superconductivity. It has been found that the
doping level is a key controlling parameter in determining the superconducting transition
temperature (Tc); a maximum Tccan usually be observed at the optimal doping (p0.16).
It has also been found that, even within the same class of cuprate superconductors, the max-
imum Tcdepends sensitively on the number of CuO2planes (n) in one structural unit: the
maximum Tcincreases with n from single layer (n=1) to triple layer (n=3), reaches a maxi-
mum at n=3 and starts to decrease with further increase of n (Fig. S1a in Supplementary
2
Materials)[3–7]. For example, in the Bi-based Bi2Sr2Can1CunO2n+4+δsuperconductors,
the maximum Tcincreases significantly from 32 K for n=1 to 91 K for n=2, to 110 K for
n=3[7]. The strong Tcdependence on n, particularly the maximum Tcenhancement for
n=3, indicates that there is another key factor in controlling Tcin addition to the doping
level. Moreover, the three-layer Bi2Sr2Ca2Cu3O10+δ(Bi2223) superconductor exhibits an
unusual phase diagram in that its Tckeeps nearly constant in the optimally and overdoped
region (Fig. S1b in Supplementary Materials). This is in a strong contrast to the usual
phase diagram where Tcdecreases with increasing doping in the overdoped region in other
one-layer or two-layer cuprate superconductors. Revealing the underlying electronic origin of
the Tcmaximization in trilayer superconductors and its high Tcpersistence in the overdoped
region is significant in understanding superconductivity mechanism and further enhancing
Tcin cuprate superconductors.
The Bi2223 superconductor has provided an ideal system for angle-resolved photoemission
(ARPES) measurements because of the availability of high quality single crystals and the
easiness of cleavage to get clean and flat surface. So far Bi2223 is also the only trilayer
superconductor on which extensive ARPES studies have been carried out[8–16]. In Bi2223
with three adjacent CuO2planes in one structural unit (Fig. 1a), it is expected from
band structure calculations that three Fermi surface sheets should arise due to interlayer
interactions[17]. However, only one Fermi surface[8–11] or two Fermi surface sheets[12–16]
have been observed in all the previous ARPES measurements on Bi2223. The absence of
three Fermi surface sheets measured in Bi2223 has been attributed to the charge imbalance
between the inner and outer CuO2planes and the weak interlayer coupling[12, 13, 15, 16].
It was also pointed out that trilayer and higher-multilayer splittings would be increasingly
difficult to observe because of the induced pseudogap of the inner layers[4].
In this paper, by taking high resolution laser-based ARPES measurements, we report
for the first time the observation of three Fermi surface sheets in Bi2223. The momentum-
dependence of the superconducting gap along all the three Fermi surface sheets is determined
and the Bogoliubov band hybridization between two specific bands is observed. These ob-
servations make it possible to analyse in detail the intralayer and interlayer couplings and
pairings. The observed Fermi surface topology, the selective band hybridization and the un-
usual Fermi surface- and momentum-dependent superconducting gap can be well understood
by a three-layer interaction model with a global set of parameters. Our results reveal the
3
microscopic origin of the unusual superconducting properties in the trilayer superconductors.
The ARPES measurements were carried out on an overdoped Bi2223 sample with a Tc
of 108.0 K (Fig. S2 in Supplementary Materials). The high resolution and high statistics
data from our laser ARPES system are essential for the new observations we present in
the paper (see Methods). Fig. 1 shows the Fermi surface mapping and constant energy
contours measured at 18 K. The corresponding band structures along the momentum cuts
from the nodal direction to the antinodal region are presented in Fig. 2. From these results,
three main Fermi surface sheets (labelled as α,βand γin Fig. 1f) and three main bands
(marked as α,βand γin Fig. 2) are clearly observed. In the Fermi surface mapping (Fig.
1b), the spectral weight is mainly confined to the nodal region because of the anisotropic
gap opening that is large near the antinodal region. Upon increasing the binding energy,
the spectral weight spreads to the antinodal region in the constant energy contours (Fig.
1c-1e) and the full contours of the three main Fermi surface show up clearly. By analyzing
the Fermi surface mapping and the constant energy contours in Fig. 1b-1e, combined with
the analysis of the band structures in Fig. 2, we have determined quantitatively the three
main Fermi surface sheets as shown in Fig. 1f. It is the first time that three main Fermi
surface sheets are observed in Bi2223. The γFermi surface is well separated from the (α,β)
sheets. The splitting between the αand βsheets increases from the nodal to the antinodal
regions, similar to the bilayer splitting observed in Bi2Sr2CaCu2O8+δ(Bi2212)[18–21]. The
corresponding doping levels of the α,βand γFermi surface sheets, determined from their
areas, are 0.37, 0.22 and 0.08, respectively.
Figure 2 shows the band structure evolution with momentum going from the nodal di-
rection to the antinodal region. Three main bands are clearly observed, labelled as α,βand
γand marked by colored arrows in Fig. 2a. Along the nodal direction (first panel in Fig.
2a), the γband is well separated from the (α,β) bands. Although the splitting between the
αand βbands is a minimum along the nodal direction, careful analyses indicate that the α
and βband splitting already exists along the nodal direction with a ∆kF=0.011π/a (see Fig.
S3 in Supplementary Materials). The αand βband splitting increases with the momentum
moving from the nodal to the antinodal regions. The γband sinks quickly to the high
binding energy due to the gap opening, accompanied by strong spectral weight suppression
when the momentum cut shifts from the nodal direction to the antinodal region. Near the
antinodal region, the βband becomes dominant which has much stronger spectral weight
4
摘要:

ElectronicOriginofHigh-TCMaximizationandPersistenceinTrilayerCuprateSuperconductorsXiangyuLuo1;3;y,HaoChen1;3;y,YinghaoLi1;3;y,QiangGao1,ChaohuiYin1;3,HongtaoYan1;3,TaiminMiao1;3,HailanLuo1;3,YingjieShu1;3,YiwenChen1;3,ChengtianLin4,ShenjinZhang5,ZhiminWang5,FengfengZhang5,FengYang5,QinjunPeng5,Guod...

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Electronic Origin of High- TCMaximization and Persistence in Trilayer Cuprate Superconductors Xiangyu Luo13y Hao Chen13y Yinghao Li13y Qiang Gao1 Chaohui Yin13 Hongtao.pdf

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