Titlebook: Quantum Mechanical Models of Metal Surfaces and Nanoparticles; Wolfgang Gr?fe Book 2015 The Editor(s) (if applicable) and The Author(s), u

解毒藥

書目名稱Quantum Mechanical Models of Metal Surfaces and Nanoparticles影響因子(影響力)




書目名稱Quantum Mechanical Models of Metal Surfaces and Nanoparticles影響因子(影響力)學(xué)科排名




書目名稱Quantum Mechanical Models of Metal Surfaces and Nanoparticles網(wǎng)絡(luò)公開度




書目名稱Quantum Mechanical Models of Metal Surfaces and Nanoparticles網(wǎng)絡(luò)公開度學(xué)科排名




書目名稱Quantum Mechanical Models of Metal Surfaces and Nanoparticles被引頻次




書目名稱Quantum Mechanical Models of Metal Surfaces and Nanoparticles被引頻次學(xué)科排名




書目名稱Quantum Mechanical Models of Metal Surfaces and Nanoparticles年度引用




書目名稱Quantum Mechanical Models of Metal Surfaces and Nanoparticles年度引用學(xué)科排名




書目名稱Quantum Mechanical Models of Metal Surfaces and Nanoparticles讀者反饋




書目名稱Quantum Mechanical Models of Metal Surfaces and Nanoparticles讀者反饋學(xué)科排名

形狀

Nucleate

打折

榨取

Detailed Calculation of the Convolution Integrals, of this density function have been determined. For differentiation of surface energy with respect to the strain ε, according to Herring’s?equation the extended Leibniz rule has been applied. The area of integration for the practical accomplishment of the convolution procedure is depicted.

senile-dementia

ATP861

,Tamm’s Electronic Surface States,The one-dimensional body shall have a surface at .?=?0. This surface is physically described by a step of the potential energy ... As Tamm has shown, electrons can be localized at the surface of the body. The energies . and the attenuation lengths. for the two resulting Tamm’s electronic surface states have been calculated.

治愈

Surface Stress-Charge Coefficient (Estance),The surface stress-charge coefficient (Estance) has been calculated for the semi-infinitely extended three-dimensional body and for a nanocube with 10×10×10 atoms. For the semi-infinite body the calculated quantity ?. = dσ./d. amounts to nearly ?1.34?V in the range of the chemical potential between 1.1?×?10. J and 1.4?×?10. J.

ONYM

Regard to the Spin in the Foregoing Texts,Now we consider the influence of the spin on the foregoing results. For this, we complete the wave functions for the three-dimensional space.(.) by the eigenfunctions of the spin operator χ. and χ.

ARM

Comparison of the Results for the Semi-infinite and the Limited Body,The results for the semi-infinite and the limited bodies are compared. The findings obtained with the different models for the offspring surface state and the surface?free energy are similar but, not identical.