Erratum: Co impurities on Ag and Cu: Kondo temperature dependence on substrate orientation [Phys. Rev. B79, 075410 (2009)]

2010 ◽  
Vol 82 (7) ◽  
Author(s):  
Pablo Roura-Bas ◽  
María Andrea Barral ◽  
Ana María Llois
2009 ◽  
Vol 79 (7) ◽  
Author(s):  
Pablo Roura-Bas ◽  
María Andrea Barral ◽  
Ana María Llois

1998 ◽  
Vol 540 ◽  
Author(s):  
E. P. Hollar ◽  
I. M. Robertson ◽  
I. Jeničič

AbstractSi and Ge samples of different substrate orientations were implanted with 50 keV Xe+ ions to a dose around 1011 ions/cm2 where the amorphous zones, created by individual ions, remained spatially isolated. The samples were subsequently irradiated at either 90 or 300K with electrons having energies from 25 to 300 keV in a transmission electron microscope (TEM). At all electron energies and at both temperatures a significant fraction of amorphous zones crystallized, showing that this effect is not due to a temperature increase and occurs at energies below the threshold displacement energy. Preliminary results show that in Ge the crystallization rate depends on the substrate orientation, while in Si this effect was not observed. The results are discussed in terms of possible explanations for epitaxial growth.


2020 ◽  
Vol 5 (1) ◽  
Author(s):  
Georg Poelchen ◽  
Susanne Schulz ◽  
Max Mende ◽  
Monika Güttler ◽  
Alexander Generalov ◽  
...  

Abstract Ultra-violet angle-resolved photoemission spectroscopy (UV-ARPES) was used to explore the temperature dependence of the Ce-4f spectral responses for surface and bulk in the antiferromagnetic Kondo lattice CeRh2Si2. Spectra were taken from Ce- and Si-terminated surfaces in a wide temperature range, and reveal characteristic 4f patterns for weakly (surface) and strongly (bulk) hybridized Ce, respectively. The temperature dependence of the Fermi level peak differs strongly for both cases implying that the effective Kondo temperature at the surface and bulk can be rather distinct. The greatly reduced crystal–electric-field (CEF) splitting at the surface gives reason to believe that the surface may exhibit a larger effective Kondo temperature because of a higher local-moment effective degeneracy. Further, the hybridization processes could strongly affect the 4f peak intensity at the Fermi level. We derived the k-resolved dispersion of the Kondo peak which is also found to be distinct due to different sets of itinerant bands to which the 4f states of surface and bulk Ce are coupled. Overall our study brings into reach the ultimate goal of quantitatively testing many-body theories that link spectroscopy and transport properties, for both the bulk and the surface, separately. It also allows for a direct insight into the broader problem of Kondo lattices with two different local-moment sublattices, providing some understanding of why the cross-talking between the two Kondo effects is weak.


Author(s):  
Kenneth H. Downing ◽  
Robert M. Glaeser

The structural damage of molecules irradiated by electrons is generally considered to occur in two steps. The direct result of inelastic scattering events is the disruption of covalent bonds. Following changes in bond structure, movement of the constituent atoms produces permanent distortions of the molecules. Since at least the second step should show a strong temperature dependence, it was to be expected that cooling a specimen should extend its lifetime in the electron beam. This result has been found in a large number of experiments, but the degree to which cooling the specimen enhances its resistance to radiation damage has been found to vary widely with specimen types.


Author(s):  
Sonoko Tsukahara ◽  
Tadami Taoka ◽  
Hisao Nishizawa

The high voltage Lorentz microscopy was successfully used to observe changes with temperature; of domain structures and metallurgical structures in an iron film set on the hot stage combined with a goniometer. The microscope used was the JEM-1000 EM which was operated with the objective lens current cut off to eliminate the magnetic field in the specimen position. Single crystal films with an (001) plane were prepared by the epitaxial growth of evaporated iron on a cleaved (001) plane of a rocksalt substrate. They had a uniform thickness from 1000 to 7000 Å.The figure shows the temperature dependence of magnetic domain structure with its corresponding deflection pattern and metallurgical structure observed in a 4500 Å iron film. In general, with increase of temperature, the straight domain walls decrease in their width (at 400°C), curve in an iregular shape (600°C) and then vanish (790°C). The ripple structures with cross-tie walls are observed below the Curie temperature.


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