Superconductivity through Quantum Critical Fluctuations in the ...
Superconductivity through Quantum Critical Fluctuations in the ...
Superconductivity through Quantum Critical Fluctuations in the ...
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current operators <strong>in</strong> <strong>the</strong> l<strong>in</strong>k (p, p + 1). Note that this is<strong>the</strong> lattice equivalent of transforms as (r ⇥ p), where rand p are <strong>the</strong> position and momentum vectors along <strong>the</strong>l<strong>in</strong>ks of <strong>the</strong> unit-cell.<strong>Quantum</strong>-<strong>Critical</strong> <strong>Fluctuations</strong> : Aji-cmv PRL(07); PR-B(09)OCuThe critical modes are <strong>the</strong> fluctuations among <strong>the</strong> fourconfigurations of observed order, i.e., among <strong>the</strong> fourorientations of <strong>the</strong> order parameter vector L.(a)(b)FIG. 1: a: The four doma<strong>in</strong>s of <strong>the</strong> circulat<strong>in</strong>g current phaseare shown. They may be specified by <strong>the</strong> four orientationsof a vector shown <strong>in</strong> red. b: Schematic representation of <strong>the</strong>current due to <strong>the</strong> operator C(j i )In <strong>the</strong> fluctuations regime <strong>the</strong> vector L has <strong>the</strong> same critical<strong>Quantum</strong> Ashk<strong>in</strong>-Teller model: In <strong>the</strong> quantum fluctuationregime, fluctuat<strong>in</strong>g flux and current patterns overany region of space and time are generated by <strong>the</strong> elementaryprocess of fluctuations between <strong>the</strong> four config-spectra as a model with a cont<strong>in</strong>uous rotations of L, i.e. <strong>the</strong>quantum- XY model.⇧ 0 maywhereof <strong>the</strong>cell.mate fr0.1µ B pCouppl<strong>in</strong>g ofa collecmatrix|⇥ i ± ⇤ter<strong>in</strong>g mtime-re<strong>the</strong> con<strong>in</strong> detaas <strong>the</strong>only userators<strong>the</strong> operotatiorotatesator <strong>in</strong>P (1234