Multichannel photoionization chamber.
Multichannel photoionization chamber to measure absorption, yield and light intensity of gases in vacuum UV
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Multichannel photoionization chamber to measure absorption, yield and light intensity of gases in vacuum UV
Use of photoionization in measuring velocity profile of free stream flow in expansion tube
Simultaneous photoexcitation and photoionization of He near threshold at 186 A, measuring probability
Major ions in chemi-ionization of hydrocarbon flames determined for heats of formation by photoionization mass spectrometer
Photoionization source with a vacuum UV monochromator is used in ion reaction kinetics. Monochromator passes only the photon energies near the threshold of the selected ionization process. Absence of electron impact alleviates creation of different type ions that result in ion fragmentation.
Trace gas analysis using photoionization mass spectrometer
Radial wave functions and photoionization cross sections for neutral atoms from central potential model based on Slater and Klein-Brueckner approximations
Analytical photoionization mass spectrometer with argon gas filter between light source and monochrometer
Shock tube data on far ultraviolet photoionizing radiation flux in precursor plasma of blunt reentry vehicles
Photoionization coefficients and photoelectron impact excitation efficiencies in daytime ionosphere, noting role in dayglow
Cross sections for fluorescence production in carbon dioxide photoionization by 58.4 nm radiation, deriving emission spectra
Atomic N and C photoionization cross sections by shock tube vacuum UV spectrometry
Photoionization mass spectrometry, considering application to appearance potentials determination, ion-neutral reactions and gas analysis
An analysis was conducted of a gas window photoionization device for studying cosmic X-rays in the region 20 eV to 1 keV. The detecting element is an argon proportional counter whose window is a two-dimensional supersonic gas jet. Spectroscopic features of the incoming radiation can be determined by the choice of gas forming the jet (as well by the fluid dynamic parameters of the flow). The choice of gas can be made from pure substances and/or compounds with Z between 1 and 10. The counter walls can be prepared for selective analysis of the extreme ultraviolet radiation.
The measurements have been conducted in the spectral range from 600 to 2000 A. Integrated oscillator strengths were determined for a number of strong Rydberg transitions above 1200 A. From the photoionization curve the first adiabatic ionization potential was found to be 10.87 plus or minus 0.01 eV. As an aid in interpreting the absorption spectrum, theoretical calculations were made using a single-configuration self-consistent field procedure for the Rydberg states and a model which included mixing between the Rydberg and valence states.
Detailed photoionization calculations are used to examine the information conveyed by relative emission-line intensities in QSO spectra. It is found that the elemental abundances cannot be estimated with any assurance; but if ?conventional' values are assumed, then certain restrictions may be placed on the ionizing spectra and gas densities. In particular, the ratio between radiation density and gas density is determined. Narrow filaments or sheets of ionized gas seem to be indicated; these may be compressed regions behind shock fronts.
Demonstration of the importance of core polarizability in a case where cancellation is only moderate, with suggestion of an improvement to the scaled Thomas-Fermi (STF) wave functions of Stewart and Rotenberg (1965). The inclusion of dipole polarizability of the core for argon is shown to substantially improve the agreement between the theoretical and experimental photoionization cross sections for the ground-state configuration.
Photoions produced in methanol and formaldehyde by radiation in the spectral region 450-1150 A were analyzed mass spectrometrically, and their relative yields were determined as a function of wavelength. First ionization potentials were determined, and the ion yield curves were interpreted in terms of ionization processes in conjunction with other data. Fragment ions were detected on mass numbers of 31, 30, 29, 15, and 14 for methanol, and 29, 2, and 1 for formaldehyde. The associated appearance potentials were determined and were used to calculate heats of formation of the ions CH2OH(+) and HCO(+), and the radicals CH3, CH2, and HCO.