Thin Solid Films, Vol.509, No.1-2, 168-172, 2006
Temperature and magnetic field dependence of the Yosida-Kondo resonance for a single magnetic atom adsorbed on a surface
Manifestations of the Kondo effect on an atomic length scale on and around a magnetic atom adsorbed on a nonmagnetic surface differ depending on the spectroscopic mode of operation of the scanning tunneling microscope. Two prominent signatures of the Kondo effect that can be observed at surfaces are the development of a sharp resonance (Yosida-Kondo resonance) at the Fermi level, which broadens with increasing temperature, and the splitting of this sharp resonance upon application of an external magnetic field. Until recently, observing the temperature and magnetic field dependence has been a challenge, because the experimental conditions strongly depend on the system's critical temperature, the so-called Kondo temperature T-K. In order to clearly observe the temperature dependence, one needs to choose a system with a large T-K. One can thus perform the experiments at temperatures T << T-K. However, because the applied external magnetic field necessary to observe the magnetic field dependence scales with T-K, one needs to choose a system with a very small T-K. This in turn means that one should perform the experiments at very low temperatures, e.g., in the mK range. Here we discuss the temperature and magnetic field dependence of the Yosida-Kondo resonance for a single magnetic atom on a metal surface, in relation to recent experimental developments. (c) 2005 Elsevier B.V. All rights reserved.
Keywords:many-body effects;Kondo effect;Yosida-Kondo resonance;dilute magnetic alloys;metallic surfaces;scanning tunneling microscopy;Mn;NiAl;Al2O3