Theoretical treatment of the electronic structure of small metallic particles

1981 ◽  
Vol 106 (1-3) ◽  
pp. A172
Author(s):  
R.P. Messmer
1998 ◽  
Vol 76 (7) ◽  
pp. 1006-1014 ◽  
Author(s):  
R H Abu-Eittah ◽  
M El-Esawy ◽  
N Ghoneim ◽  
A T Aly

The electronic structure, conformation, and molecular orbitals of some nickel(II) azides, thiocyanates, and isothiocyanates have been studied. Three different basis sets: split valence (SV), split valence with six d-Gaussians (SV6D), and double zeta (DZ) sets, were used to find the best ground state for nickel. It has been found that the combination, DZ-3F, gives results closest to the experimental values. The electronic structures of the nickel azides studied were completely different from those of the nickel thiocyanates. On the other hand, the electronic structures of the nickel thiocyanates studied were highly comparable to those of the corresponding nickel isothiocyanates. Molecular orbitals were computed for the complexes studied and the types of electronic transitions expected were identified and discussed.Key words: Ni(II) azides, thiocyanates, and isothiocyanates: ab initio SCF calculations; MO calculations on some Ni(II) complexes; theoretical treatment of some Ni(II) ions and salts; geometry and energetics of some nickel(II) azides, thiocyanates, and isothiocyanates.


2003 ◽  
Vol 4 (4) ◽  
pp. 235-269 ◽  
Author(s):  
K. V. Chuistov ◽  
A. P. Shpak ◽  
A. O. Perekos ◽  
O. D. Rud’ ◽  
V. M. Uvarov

2019 ◽  
Vol 289 ◽  
pp. 134-140
Author(s):  
A. Pal ◽  
M. Chinotti ◽  
W.J. Ren ◽  
C. Petrovic ◽  
L. Degiorgi

We provide a discussion of our previously collected data (Chinotti et al., Phys. Rev. B 94, 245101 (2016)) on the electrodynamic response in YbMnBi2, a representative Weyl semimetal, and in its gapped semimetal counterpart EuMnBi2, which can be fairly well reproduced within a recent devoted theoretical treatment (S.P. Mukherjee and J.P. Carbotte, J. Phys.: Condens. Matter 29 (2017) 425301). This allows identifying and catching all the essential features of their peculiar electronic structure as imaged by the excitation spectrum.


2022 ◽  
Author(s):  
Maria Storm Thomsen ◽  
Andy Sode Anker ◽  
Laura Kacenauskaite ◽  
Thomas Just Sørensen

Our theoretical treatment of electronic structure in coordination complexes often rests on assumptions of symmetry. Experiments rarely provide fully symmetric systems to study. In solution, fluctuation in solvation, variations in conformation, and even changes in constitution occur and complicates the picture. In crystals, lattice distortion, energy transfer, and phonon quenching is in play, but we are able to have distinct symmetries. Yet the question remains: How is the real symmetry in a crystal compared to ideal symmetries? Moreover, at what level of detail do we need to study a system to determine, if the electronic structure behaves as if it has ideal symmetry? Here, we have revisited the Continues Shape Measurement (CShM) approach developed by Ruiz-Martínez and Alvarez to evaluate the structure of ten-coordinated europium(III) ions in a K5Na[Eu2(SO4)6] structure. By comparing the result of the symmetry deviation analysis to luminescence data, we are able to show the effect of small deviations from ideal symmetry. We suggest using a symmetry deviation value, σideal, determined by using our updated approach to Continues Shape Measurements, where we also align the structure via our AlignIt code. AlignIt includes normalization and relative orientation in the symmetry comparison, and by combining the calculated values with the experimentally determined energy level splitting, we were able create the first point on a scale that can show how close to ideal an experimental structure actually is.


1979 ◽  
Vol 57 (5) ◽  
pp. 645-656 ◽  
Author(s):  
D. Ward ◽  
H. R. Andrews ◽  
I. V. Mitchell ◽  
W. N. Lennard ◽  
R. B. Walker ◽  
...  

Stopping powers have been measured at common ion velocities v = 0.18 cm ns−1 (v/v0 = 0.82) and v = 0.22 cm ns−1 (v/v0 = 1.01) for all projectiles 6 ≤ Z1 ≤ 20 in five solid materials: carbon, aluminum, nickel, silver, and gold. The Z1-oscillation was observed and several new features for the systematics of the oscillation emerge: (i) the amplitude of the oscillation varies with target material and is weak in nickel, (ii) the amplitude changes with ion velocity but this dependence varies with material, (iii) the phase of the oscillation varies by up to 2 units in Z1 according to the material, and (iv) the phase is independent of the velocity over the range studied.We conclude that at low velocity the effect of projectile (Z1) electronic structure on the stopping power cannot be separated from that of the material (Z2).An apparent variation of the stopping power with target thickness was observed and is interpreted in terms of multiple scattering through a recent theoretical treatment.


Author(s):  
A. Gómez ◽  
P. Schabes-Retchkiman ◽  
M. José-Yacamán ◽  
T. Ocaña

The splitting effect that is observed in microdiffraction pat-terns of small metallic particles in the size range 50-500 Å can be understood using the dynamical theory of electron diffraction for the case of a crystal containing a finite wedge. For the experimental data we refer to part I of this work in these proceedings.


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