Kondo Effect in Non-Equilibrium

Author(s):  
Johann Kroha
Keyword(s):  
Nanoscale ◽  
2018 ◽  
Vol 10 (37) ◽  
pp. 17738-17750 ◽  
Author(s):  
W. H. Appelt ◽  
A. Droghetti ◽  
L. Chioncel ◽  
M. M. Radonjić ◽  
E. Muñoz ◽  
...  

We predict the non-equilibrium molecular conductance in the Kondo regime from first principles by combining density functional theory with the renormalized super-perturbation theory.


2017 ◽  
Vol 146 (9) ◽  
pp. 092309 ◽  
Author(s):  
Deung-Jang Choi ◽  
Paula Abufager ◽  
Laurent Limot ◽  
Nicolás Lorente

2004 ◽  
Vol 54 (S4) ◽  
pp. 615-618 ◽  
Author(s):  
R. Świrkowicz ◽  
M. Wilczyński ◽  
J. Barnaś

2020 ◽  
Author(s):  
Tokuro Hata ◽  
Yoshimichi Teratani ◽  
Tomonori Arakawa ◽  
Sanghyun Lee ◽  
Meydi Ferrier ◽  
...  

Abstract Understanding the properties of correlated quantum liquids is a fundamental issue of condensed matter physics. Even in such a correlated case, fascinatingly, we can tell that the equilibrium fluctuations of the system govern its linear response to an external field, relying on the fluctuation dissipation relations based on the two-body correlations. Going beyond, up to the three-body correlations, is of importance for van der Waals force [1], the three-body force in nuclei [2], the Efimov state [3, 4], the ring exchange interaction in solid 3He [5, 6], and frustrated spin systems [7]. In our work, we have used a quantum dot in the Kondo regime, which is a controllable realization of such a correlated quantum liquid [8–11]. Thanks to the quality of our sample, where the Kondo effect in the unitary limit was achieved, we could quantitatively measure the three-body correlations and their role in the non-equilibrium regime, in perfect agreement with recent results of the Fermi liquid theory [12– 15]. In particular, we have demonstrated its importance when time-reversal symmetry is broken, solving a long-standing puzzle of the Kondo systems under the magnetic field [13]. The demonstrated method to relate three-body correlation and non-equilibrium transport opens up a way for further investigation of the dynamics of quantum many-body systems.


2004 ◽  
Vol 272-276 ◽  
pp. 1676-1677 ◽  
Author(s):  
M.N. Kiselev ◽  
K.A. Kikoin ◽  
L.W. Molenkamp

2006 ◽  
Vol 2 (7) ◽  
pp. 460-464 ◽  
Author(s):  
J. Paaske ◽  
A. Rosch ◽  
P. Wölfle ◽  
N. Mason ◽  
C. M. Marcus ◽  
...  

2005 ◽  
Vol 74 (1) ◽  
pp. 118-126 ◽  
Author(s):  
A. Rosch ◽  
J. Paaske ◽  
J. Kroha ◽  
P. Wölfle

2006 ◽  
Author(s):  
M. A. H. Khalafalla ◽  
H. Mizuta ◽  
S. Oda ◽  
Z. A. K. Durrani

Author(s):  
Edward A Kenik

Segregation of solute atoms to grain boundaries, dislocations, and other extended defects can occur under thermal equilibrium or non-equilibrium conditions, such as quenching, irradiation, or precipitation. Generally, equilibrium segregation is narrow (near monolayer coverage at planar defects), whereas non-equilibrium segregation exhibits profiles of larger spatial extent, associated with diffusion of point defects or solute atoms. Analytical electron microscopy provides tools both to measure the segregation and to characterize the defect at which the segregation occurs. This is especially true of instruments that can achieve fine (<2 nm width), high current probes and as such, provide high spatial resolution analysis and characterization capability. Analysis was performed in a Philips EM400T/FEG operated in the scanning transmission mode with a probe diameter of <2 nm (FWTM). The instrument is equipped with EDAX 9100/70 energy dispersive X-ray spectrometry (EDXS) and Gatan 666 parallel detection electron energy loss spectrometry (PEELS) systems. A double-tilt, liquid-nitrogen-cooled specimen holder was employed for microanalysis in order to minimize contamination under the focussed spot.


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