Single atoms show discrete energy states. Bulk semiconductors show energy bands. So one would expect the band gap behaviour to change with the size of the solid. For example one can tune the color of the emission of colloidal quantum dots just by varying their size.
Brus developed a model to predict the band gap energy of nanocrystallites, quantum dots and other small spherical structures with radius R. Roughly speaking, the approach is to start with the bulk value of the energy gap, add a "particle-in-a-box" like term for electrons and holes using an effective mass approximation for the masses of both and subtracting a term, which corresponds to the Coulomb-attraction between electrons and holes. The particle-in-a-box-term scales with 1/R² and the attraction term scales with 1/R, so in small structures the 1/R²-term dominates.
However this approach uses effective masses, which do not depend on the size of the structure. Therefore the results are ok for structures of intermediate size, but are rather wrong for very small structures.
I am new to XPS Data analysis, and I have a .sle file that I got out of XPS Machine Software, and I am using CasaXPS to analyse the data. This software takes only .vms files. I want to convert the .sle to a .vms file for analysis. How or where can I do this? Any help on this will be deeply appreciated.
Hi. I have got question as in title. How can idea of instantaneous dipole moment for atoms like, for example hydrogen be consistent with idea of orbitals? At my level of knowledge London dispersion forces are derived taking into account Bohr model of atom. But we know today that this model is not correct. If it would be correct I understand that at each time electron is at some point at radius at some angle and there is dipole moment at this time from nucleus to electron at orbit. But how...