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Coot displays electron density maps and atomic models and allows model manipulations such as idealization, real space refinement, manual rotation/translation, rigid-body fitting, ligand search, solvation, mutations, rotamers, and Ramachandran idealization. The software is designed to be easy-to-learn for novice users, achieved by ensuring that ...
Electron applications include a "main" process and several "renderer" processes. The main process runs the logic for the application (e.g., menus, shell commands, lifecycle events), and can then launch multiple renderer processes by instantiating an instance of the BrowserWindow class, which loads a window that appears on the screen by ...
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The hydrogen anion is the dominant bound-free opacity source at visible and near-infrared wavelengths in the atmospheres of stars like the Sun and cooler; [2] its importance was first noted in the 1930s. [3] The ion absorbs photons with energies in the range 0.75–4.0 eV, which ranges from the infrared into the visible spectrum.
The Fermi level of a solid-state body is the thermodynamic work required to add one electron to the body. It is a thermodynamic quantity usually denoted by μ or E F [ 1 ] for brevity. The Fermi level does not include the work required to remove the electron from wherever it came from.
James K. Freericks (born 1963) is an American physicist and endowed chair at Georgetown University. He has worked in fields of condensed matter physics, mathematical physics, atomic physics, nonequilibrium physics, quantum computation, and quantum mechanics pedagogy.
In this case, the carrier density (in this context, also called the free electron density) can be estimated by: [5] n = N A Z ρ m m a {\displaystyle n={\frac {N_{\text{A}}Z\rho _{m}}{m_{a}}}} Where N A {\displaystyle N_{\text{A}}} is the Avogadro constant , Z is the number of valence electrons , ρ m {\displaystyle \rho _{m}} is the density of ...