scholarly journals Ferromagnetic order beyond the superconducting dome in a cuprate superconductor

Science ◽  
2020 ◽  
Vol 368 (6490) ◽  
pp. 532-534 ◽  
Author(s):  
Tarapada Sarkar ◽  
D. S. Wei ◽  
J. Zhang ◽  
N. R. Poniatowski ◽  
P. R. Mandal ◽  
...  

According to conventional wisdom, the extraordinary properties of the cuprate high-temperature superconductors arise from doping a strongly correlated antiferromagnetic insulator. The highly overdoped cuprates—whose doping lies beyond the dome of superconductivity—are considered to be conventional Fermi liquid metals. We report the emergence of itinerant ferromagnetic order below 4 kelvin for doping beyond the superconducting dome in thin films of electron-doped La2–xCexCuO4 (LCCO). The existence of this ferromagnetic order is evidenced by negative, anisotropic, and hysteretic magnetoresistance, hysteretic magnetization, and the polar Kerr effect, all of which are standard signatures of itinerant ferromagnetism in metals. This surprising result suggests that the overdoped cuprates are strongly influenced by electron correlations.

2008 ◽  
Vol 100 (12) ◽  
Author(s):  
Jing Xia ◽  
Elizabeth Schemm ◽  
G. Deutscher ◽  
S. A. Kivelson ◽  
D. A. Bonn ◽  
...  

1996 ◽  
Vol 10 (07) ◽  
pp. 805-845 ◽  
Author(s):  
LAN YIN ◽  
SUDIP CHAKRAVARTY

Spectral anomaly for interacting fermions is characterized by the spectral function A ([k − k F ], ω) satisfying the scaling relation A (Λy1 [k − k F ], Λy2 ω) =ΛyA A ([k − k F ], ω), where y1, y2, and yA are the exponents defining the universality class. For a Fermi liquid y1 = 1, y2 = 1, yA = −1; all other values of the exponents are termed anomalous. In this paper, an example for which y1 = 1, y2 = 1, but yA = α − 1 is considered in detail. Attractive interaction added to such a critical system leads to a novel superconducting state, which is explored and its relevance to high temperature cuprate superconductors is discussed.


1981 ◽  
Vol 17 (6) ◽  
pp. 3205-3210 ◽  
Author(s):  
S. Visnovsky ◽  
V. Prosser ◽  
R. Krishnan ◽  
V. Parizek ◽  
K. Nitsch ◽  
...  

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