Emission cross sections of N2 in the vacuum ultraviolet by electron impact
Emission cross sections of nitrogen in vacuum UV by electron impact
Ajello, J. M.↗
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Use of a tungsten filament lamp as a calibration standard in the vacuum ultraviolet
Sapphire windowed argon filled tungsten ribbon filament lamp in vacuum UV for application in photomultiplier quantum efficiency calibration
Buckley, J. L.↗
Vacuum ultraviolet wavelength standards and improved energy levels in the first spectrum of silicon.
Vacuum UV wavelength standards and energy levels in first silicon spectrum from low pressure source
VACUUM SPECTROSCOPY↗
The fourth positive system of carbon monoxide observed in absorption at high resolution in the vacuum ultraviolet region.
Fourth positive carbon monoxide system observed in absorption in vacuum UV region, discussing rotational and vibrational band structure
Bass, A. M.↗
Formaldehyde absorption coefficients in the vacuum ultraviolet /650 to 1850 angstroms/
Formaldehyde absorption coefficients measured photoelectrically in vacuum UV range
Gentieu, E. P.↗
Polarized vacuum ultraviolet and X-radiation
The most intense source of polarized vacuum UV and X radiation is synchrotron radiation, which exhibits a degree of partially polarized light between about 80-100%. However, the radiation transmitted by vacuum UV monochromators can also be highly polarized. The Seya-Namioka type of monochromator can produce partially polarized radiation between 50-80%. For certain experiments it is necessary to know the degree of polarization of the radiation being used. Also, when synchrotron radiation and a monochromator are combined the polarization characteristic of both should be known in order to make full use of these polarization properties. The polarizing effect of monochromators (i.e., diffraction gratings) have been measured at the Seya angle and at grazing angles for various spectral orders. Experimental evidence is presented which shows that the reciprocity law holds for polarization by reflection where the angle of incidence and diffraction are unequal. These results are reviewed along with the techniques for measuring the degree of polarization.
Samson, J. A. R.↗
A polarizer for the vacuum ultraviolet.
Magnesium fluoride double Rochon prism used as polarizer or analyzer in vacuum UV wavelengths
MAGNESIUM FLUORIDE↗
Vacuum-ultraviolet photon production in low- energy collisions between two neutral argon atoms
Vacuum UV photons production during ground state neutral argon atomic collisions, measuring relative cross sections energy dependence
Amme, R. C.↗
Time-controllable continuum photon emission from a pulsed vacuum spark and application to absorption spectroscopy in the vacuum ultraviolet
Time controllable continuous photon emission from plasma produced by pulsed laser vacuum spark applied to absorption spectroscopy in vacuum UV
Mehlman-Balloffet, G.↗
Vacuum-ultraviolet series of Mg I and Mg II
Mg I and II vacuum UV emission series, presenting quantum defect plot
Goorvitch, D.↗
Measurement of atomic nitrogen and carbon photoionization cross sections using shock tube vacuum ultraviolet spectrometry
Atomic N and C photoionization cross sections by shock tube vacuum UV spectrometry
Marrone, P. V.↗
Optical constants of evaporated barium in the vacuum ultraviolet.
Optical properties of evaporated barium films investigated at various wavelengths, using ultrahigh vacuum reflectometer
REFRACTIVE INDEX↗
Dissociative excitation of vacuum ultraviolet emission features by electron impact on molecular gases. I - H2 and O2
Vacuum UV emission features dissociative excitation by electron impact on molecular hydrogen and oxygen, measuring excitation cross sections from threshold to 350 eV
Mumma, M. J.↗
Optical properties of evaporated rhodium films deposited at various substrate temperatures in the vacuum ultraviolet from 150 to 2000 A
Evaporated Rh films preparation at various substrate temperatures in vacuum UV, determining reflectance and optical constants
Cox, J. T.↗
Techniques for suppressing anomalous response to vacuum ultraviolet radiation in the charged- particle lunar environment experiment.
Procedures to suppress anomalous response to vacuum UV radiation in lunar environment experiment
Ferguson, L. D.↗
Oscillator strengths of CH2 and CH3 in the vacuum ultraviolet
Flash photolysis produced methyl and methylene radical transitions maximum extinction coefficients and oscillator strength in vacuum UV
Bass, A. M.↗
Lifetime measurements and absolute oscillator strengths for some vacuum-ultraviolet transitions in O I and O II
O I and II resonance transitions radiative lifetimes in vacuum UV, using beam foil method
Berry, H. G.↗
Vacuum ultraviolet radiation/atomic oxygen synergism in materials reactivity
Experimental results are presented which indicate that low fluxes of vacuum UV (VUV) radiation exert a pronounced influence on the atomic oxygen reactivity of such fluorocarbon and fluorocarbon spacecraft materials as the FEP Teflon and PCTFE that are under consideration for the Space Station Freedom. With simultaneous exposure to VUV fluxes comparable to those experienced in LEO, the reactivity of these materials becomes comparable to that of Kapton; VUV radiation has also been shown to increase the reactivity of Kapton with thermal-energy oxygen atoms.
Koontz, Steven↗