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Behavior of Negative Ions in Inductive RF Negative Ion Sources

open access: yesBehavior of Negative Ions in Inductive RF Negative Ion Sources
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Negative Ion Extraction from a Large RF Negative Ion Source

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Negative ions

Philosophical Transactions of the Royal Society of London. Series A, Mathematical and Physical Sciences, 1979
During the last few years, improvements in ionization techniques have revived interest in negative ion mass spectrometry and its applications. Ion sources that operate at pressures of up to 1 Torr (133 Pa) produce high concentrations of low energy electrons which may react directly with suitable sample molecules to form negative molecular ...
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Ion–Molecule Reactions of Negative Ions. I. Negative Ions of Sulfur

The Journal of Chemical Physics, 1968
Negative ions from carbonyl sulfide and carbon disulfide have been studied in a time-of-flight mass spectrometer. The principal ions formed by dissociative resonance electron capture in carbonyl sulfide are S− and O−. Those from carbon disulfide are S− and CS−.
John G. Dillard, J. L. Franklin
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Autodetachment of negative ions

Physical Review A, 1991
The autodetachment of 1s2s2p 4p0 in He- and nsnp 2 4P(e) in Be- (n = 2), Mg- (n = 3), and Ca- (n = 4) is calculated using an extension to continum processes of the multiconfiguration Hartree-Fock method. The main interest is to investigate the processes giving rise to long-lived, metastable states in negative ions. In He- and Be- our results agree with
, Brage, , Fischer
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Negative Ion Spectroscopy

Annual Review of Physical Chemistry, 1979
This article surveys experimental methods for studying the interactions of small, free atomic and molecular negative ions with radiation, and the structural information that can be obtained from such studies. The subject is an old one, having its origins some 40 years ago when Wildt (1) recognized that Hwas a major source of opacity in the solar ...
R R Corderman, W C Lineberger
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Negative ion lasers

Applied Physics Letters, 1974
The principle of detailed balance is used to show that at a maximum in an electron excitation cross section, due to a very-short-lived negative ion resonance (10−14–10−16 sec), the electron deexcitation cross section can be significantly smaller than the electron excitation cross section. Using experimental estimates of the various necessary parameters,
David E. Golden, Stephan Ormonde
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Atomic Negative Ions

Physical Review, 1964
Results of Hartree-Fock calculations on the ions of ${\mathrm{Li}}^{\ensuremath{-}}$, ${\mathrm{B}}^{\ensuremath{-}}$, ${\mathrm{C}}^{\ensuremath{-}}$, ${\mathrm{N}}^{\ensuremath{-}}$, ${\mathrm{O}}^{\ensuremath{-}}$, ${\mathrm{F}}^{\ensuremath{-}}$, ${\mathrm{N}}^{\ensuremath{-}\ensuremath{-}}$, ${\mathrm{O}}^{\ensuremath{-}\ensuremath{-}}$ in states ...
Enrico Clementi, A. D. McLean
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Negative ion plasmas

The Physics of Fluids, 1975
In a plasma composed of negative (SF−6) ions, positive (Ar+) ions, and electrons (with ne/n+ reducible to less than 10−3) a fast ion mode (vph≈9Cs), due to the out-of-phase motion between positive and negative ions, is observed with reduced spatial attenuation. This fast ion mode exhibits spatial growth in the presence of a fast ion beam.
A. Y. Wong, D. L. Mamas, D. Arnush
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