scholarly journals Quantum Phase Transition in the Magnetic-Field-Induced Normal State of Optimum-Doped High-TcCuprate Superconductors at Low Temperatures

2009 ◽  
Vol 102 (1) ◽  
Author(s):  
F. F. Balakirev ◽  
J. B. Betts ◽  
A. Migliori ◽  
I. Tsukada ◽  
Yoichi Ando ◽  
...  
1998 ◽  
Vol 12 (29n31) ◽  
pp. 3151-3156 ◽  
Author(s):  
Vsevolod Gantmakher

There are some doubts whether materials near the superconductor–insulator transition (SIT), either on the insulating side, or with superconductivity suppressed by the magnetic field, behave like an ordinary metal. Two experiments in which this issue is addressed will be reviewed here, namely, transport measurements of two different materials: single crystals YBa2Cu3O 6+x (x ≈ 0.37) — a representative of the HTS family and amorphous InO x where x is the oxygen content which could be changed through moderate-temperature annealing. The low-temperature normal resistivity ρ(T) of YBaCuO crystals on both sides of SIT behaves as usual "bad" metal with conductivity below the Mott's minimum value. The amorphous In-O films behave differently. Those films with superconductivity do not display any characteristic magnetic field which can be interpreted as Bc2. Instead, they give out an example of a quantum phase transition and follow Fisher's model1 for "the field-tuned SIT in disordered two-dimensional superconductors" though they are not precisely two-dimensional and their high-magnetic-field state may not be insulating at all. Apparently, the normal state of InO x films comprises localized Cooper pairs.


2021 ◽  
Vol 4 (1) ◽  
Author(s):  
Xiaofu Zhang ◽  
Adriana E. Lita ◽  
Huanlong Liu ◽  
Varun B. Verma ◽  
Qiang Zhou ◽  
...  

AbstractThe nature of the magnetic-field driven superconductor-to-insulator quantum-phase transition in two-dimensional systems at zero temperature has been under debate since the 1980s, and became even more controversial after the observation of a quantum-Griffiths singularity. Whether it is induced by quantum fluctuations of the superconducting phase and the localization of Cooper pairs, or is directly driven by depairing of these pairs, remains an open question. We herein experimentally demonstrate that in weakly-pinning systems and in the limit of infinitely wide films, a sequential superconductor-to-Bose insulator-to-Fermi insulator quantum-phase transition takes place. By limiting their size to smaller than the effective penetration depth, however, the vortex interaction alters, and the superconducting state re-enters the Bose-insulating state. As a consequence, one observes a direct superconductor-to-Fermi insulator in the zero-temperature limit. In narrow films, the associated critical-exponent products diverge along the corresponding phase boundaries with increasing magnetic field, which is a hallmark of the quantum-Griffiths singularity.


2007 ◽  
Vol 310 (2) ◽  
pp. 1352-1354 ◽  
Author(s):  
F. Yamada ◽  
T. Ono ◽  
M. Fujisawa ◽  
H. Tanaka ◽  
T. Sakakibara

2019 ◽  
Vol 21 (8) ◽  
pp. 4394-4407 ◽  
Author(s):  
Vinicius T. Santana ◽  
Beatriz N. Cunha ◽  
Ana M. Plutín ◽  
Rafael G. Silveira ◽  
Eduardo E. Castellano ◽  
...  

A quantum phase transition, as a consequence of spin-entanglements caused by Cu–Cu exchange couplings, explains EPR measurements in a new monomeric CuII compound.


2004 ◽  
Vol 272-276 ◽  
pp. 263-264 ◽  
Author(s):  
M Ohashi ◽  
H Akiyama ◽  
G Oomi ◽  
B.K Cho ◽  
P.C Canfield

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