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Ferromagnetism and Antiferromagnetism
Ferromagnetism and Antiferromagnetism

Thermodynamics of the dead-zone inner edge in protoplanetary
Thermodynamics of the dead-zone inner edge in protoplanetary

... optically thick disk midplane, and thus omit non-thermal sources of ionization. This also permits us to model the disk in the cylindrical approximation. This initial numerical study is the first in a series, and thus lays out our numerical tools, tests, and code-checks. We also verify previous publi ...
Principles of Nonlinear Optical Spectroscopy
Principles of Nonlinear Optical Spectroscopy

... As the diagonal elements are the same, the probability of finding the system in either |1i or |2i will be 0.5 in both cases, regardless whether the state is a coherent superposition state (Equ. 1.24) or a statistical average (Equ. 1.25). However, both states are not identical, as seen from the off-d ...
Passage of Charged Particles Through Matter
Passage of Charged Particles Through Matter

Indiene 2D Monolayer: a New Nanoelectronic Material
Indiene 2D Monolayer: a New Nanoelectronic Material

... On the other hand, buckled form behaves like an indirect semiconductor, as small gaps appear as seen in Figure 4(d). If one looks in the direction from Γ to K point, there are two energy gaps illustrated using points A (valence band maximum), B and C (conduction band minimum). A gap between the poin ...
ELECTRON!DENSITY!IN!A!HELIUM!DISCHARGE! PLASMA!
ELECTRON!DENSITY!IN!A!HELIUM!DISCHARGE! PLASMA!

Landau-level mixing and spin degeneracy in the quantum Hall effect *
Landau-level mixing and spin degeneracy in the quantum Hall effect *

... The system of two coupled extended states was also studied in the context of a spin-split Landau band.13–17 In the absence of a Zeeman term it was found that two separate extended states appear, each with a localization exponent of '2.3. Allowing for a finite Zeeman term leads to level attraction at ...
Casimir Forces in a Piston Geometry at Zero and Finite Temperatures
Casimir Forces in a Piston Geometry at Zero and Finite Temperatures

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Double-ionization mechanisms of the argon dimer in intense laser

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Exercises in Statistical Mechanics

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This rigid form is made with sticks hinged together and forms a field

Comparison of Functionals for Metal Hexaboride Band Structure
Comparison of Functionals for Metal Hexaboride Band Structure

... d-like orbitals and the La d state have nearly equal energies in LaB6, and therefore, strong hybridization occurs. Similarly, Walch et al. [32] examine the predictions of the Hartree-Fock-Slater (HFS) model for the occupied levels and low-energy excitations of LaB6, adopting the simplest, one-electr ...
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Link to file - UH Department of Chemical and Biomolecular

Electron Explorer
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IOSR Journal of Applied Physics (IOSR-JAP)

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Physics Regents Review Sheet

... _____ what is the spring constant _____ how to calculate elastic potential energy _____ how a spring relates to energy and work Electrostatics _____ what three major particles atoms are made up of _____ how atoms become charged (positive or negative) _____ what an elementary charge is and where to f ...
AIAA-2004-5668 - CSU Radar Group
AIAA-2004-5668 - CSU Radar Group

... in order to attract the lowest-energy electrons in the distribution. For the sake of the MESA instrument, we needed to float the instrument sufficiently positive that ions that might pollute the electron signal were rejected before entering the analyzer, since in the configuration used here there wa ...
Multiphoton interactions in lepton photoproduction on nuclei at high
Multiphoton interactions in lepton photoproduction on nuclei at high

... plitude illZ through the dipole-proton one illp . This can be done if the nuclear protons can be considered as independent scattering centers. For large Z their distribution thus follows the Poisson law that leads to a particularly simple expression for the amplitude (10). To avoid possible confus ...
Acetate ligands determine the crystal structure of CdSe
Acetate ligands determine the crystal structure of CdSe

CHAPTER 11 The photoelectric effect
CHAPTER 11 The photoelectric effect

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Density of states



In solid-state and condensed matter physics, the density of states (DOS) of a system describes the number of states per interval of energy at each energy level that are available to be occupied. Unlike isolated systems, like atoms or molecules in gas phase, the density distributions are not discrete like a spectral density but continuous. A high DOS at a specific energy level means that there are many states available for occupation. A DOS of zero means that no states can be occupied at that energy level. In general a DOS is an average over the space and time domains occupied by the system. Localvariations, most often due to distortions of the original system, are often called local density of states (LDOS). If the DOS of an undisturbedsystem is zero, the LDOS can locally be non-zero due to the presence of a local potential.
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