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Cross-sectional atomic force imaging of semiconductor heterostructures
Materials Science and Engineering: B, 1996Abstract We performed imaging of semiconductor heterostructures, in particular GaAs-AlGaAs quantum wells and quantum wires, by atomic force microscopy (AFM) of the cleaved edge of the samples. We used two methods to transform the alloy composition into height differences, measurable by AFM: natural oxidation and selective etching.
B Dwir, F Reinhardt, G Biasiol, E Kapon
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On atomic photoionization cross section calculation
Physics Letters A, 1969Abstract Essential peculiarities of the Hartree-Fock photoionization cross section are discussed: 1) the choice of the operator of interaction with the electromagnetic field, 2) sum rules and 3) the influence of various modifications of the self-consistent field.
M.Ya. Amusia +3 more
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Cross sections for electron scattering by atomic potassium
Physical Review A, 1992Electron elastic and collisional excitation cross sections from the ground state of potassium are calculated using the noniterative integral-equation method of Henry, Rountree, and Smith [Comput. Phys. Commun. 23, 233 (1981)] in the electron energy range 4\ensuremath{\le}E\ensuremath{\le}200 eV. Configuration-interaction target wave functions that take
, Msezane, , Awuah, , Hiamang, , Allotey
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Cross sections for the alkali atom-Br2 reactions
The Journal of Chemical Physics, 1973The reaction cross sections of alkali metal atoms with bromine molecules have been obtained by direct measurements of alkali atom decay rates. The alkali atoms were produced in the presence of a known amount of bromine molecules by photodissociating the bromide of the particular alkali atom with a short pulse of uv light.
J. Maya, P. Davidovits
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Electron Ionization Cross Sections for Atomic Subshells
Microscopy and Microanalysis, 2003Ionization of atoms is the first step in many analytical procedures. The cross section for ionizing a particular atomic shell is essential for calculating the magnitude of analytical signals. Calculations using atomic wave functions for various shells of all elements relevant for X-ray microanalysis over a range of electron energies up to 400 keV ...
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, 2021
To protect the human from the γ–radiation hazard, the novel shielding materials are ever-demanding in the field of nuclear medicine. In this research, we assessed the mass attenuation coefficient (μ/ρ), mean atomic number ( ), effective atomic cross ...
Mohammed J. R. Aldhuhaibat +3 more
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To protect the human from the γ–radiation hazard, the novel shielding materials are ever-demanding in the field of nuclear medicine. In this research, we assessed the mass attenuation coefficient (μ/ρ), mean atomic number ( ), effective atomic cross ...
Mohammed J. R. Aldhuhaibat +3 more
semanticscholar +1 more source
Photoionisation cross section of atomic oxygen
Journal of Physics B: Atomic and Molecular Physics, 1978The photoionisation cross section for the ground state 2s22p4 3P of O I is calculated in the close-coupling approximation employing the frozen-cores model. Results include detailed resonance analysis using accurate interpolation and extrapolation procedures.
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Ion-Rydberg atom collision cross sections
Journal of Physics B: Atomic and Molecular Physics, 1980Classical-trajectory Monte Carlo calculations have been performed for collisions of ions in charge states q=+1, +2, +5 and +10 with hydrogenic atoms in principal quantum levels n=1, 2, 5, 10 and 20. The collision velocity range investigated was 1 or=2.
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Electron-impact cross sections for Cu atoms
Journal of Physics B: Atomic and Molecular Physics, 1977Relative differential electron-impact cross sections have been measured for elastic scattering for excitation of the 3d104p 2 P1/2,3/2, 3d94s2 2D5/2 and 3d94s2 2D3/2 states of Cu at 6, 10, 20, 60 and 100 eV in the 0 degrees to 140 degrees angular range.
S Trajmar, W Williams, S K Srivastava
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Measurement of Differential Atomic Collision Cross Sections
Review of Scientific Instruments, 1971An apparatus for the study of differential angular scattering of atomic projectiles by gas targets is described. The design facilitates system alignment and provides for accurate reproducible location of components. The performance of the instrument is studied for scattering of H+ at 5–25 keV energies by helium and argon targets.
R. L. Fitzwilson, E. W. Thomas
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