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1 ion in the solid and gas phases of argon and krypton.
2 e mid-1940s, of less than 5 dpm per liter of krypton.
3 ds is limited for xenon and even more so for krypton.
4 r to a mixture of chondritic and atmospheric krypton.
5 tion after inhalation of a mixture of stable krypton (80%) and oxygen (20%), with reconstruction of d
6 been used to count individual krypton-85 and krypton-81 atoms present in a natural krypton gas sample
8 d the release thereby of the fission product krypton-85 (half-life = 10.71 years, fission yield = 0.2
9 tral atoms has been used to count individual krypton-85 and krypton-81 atoms present in a natural kry
12 he binding of xenon and, to a lesser degree, krypton and argon, tend to expand the volume of the cavi
13 The level of enhancement after inhalation of krypton and its excellent clinical tolerance makes this
18 topic composition, heavy noble gases (argon, krypton and xenon) have an isotopic composition very sim
21 d to have higher affinity for xenon than for krypton, and have comparable affinity for Kr and N(2).
22 ass spectrometry technique to measure argon, krypton, and xenon isotopes in volcanic gas with ultrahi
23 purely hydrophobic solutes (methane, ethane, krypton, and xenon) to study hydrophobicity at the most
26 recently designed pressurization cell using krypton at high pressure, a new gas binding site has bee
27 sly binds to the noble gases (Ngs) xenon and krypton at room temperature in a reaction that is typica
28 udy the phase behavior of adsorbed argon and krypton atoms as well as their coupling to the substrate
29 Vacuum ultraviolet spectra emanating from krypton atoms, exposed to intense waveform-controlled op
31 alled CNTs filled with lead, barium and even krypton can be produced, and externally decorated with p
33 ion at far ultraviolet C (far-UVC) 222 nm by krypton chloride (KrCl*) excilamps can enhance microbial
35 inactivation level compared with that of the krypton chloride excilamp and low-pressure mercury lamp.
38 Far-UVC wavelengths (222 nm) from filtered krypton-chloride excimer lamps are effective at inactiva
39 4 nm) that are more hazardous to humans than krypton chlorine excimer lamps emitting 222 nm (UV(222))
40 water types using UV-C light emitted from a krypton-chlorine excimer lamp (UV light at 222 nm, UV(22
42 current induced vacuum ultraviolet (dc-VUV) krypton discharge lamp and an alternating current, radio
49 85 and krypton-81 atoms present in a natural krypton gas sample with isotopic abundances in the range
50 ays is tested in canine lung tissue by using krypton gas with natural abundance isotopic distribution
52 ction of 5 x 10(-9) Torr partial pressure of krypton in argon with a signal-to-noise ratio of approxi
54 Raman spectroscopy was performed using a krypton ion laser providing excitation at 406.7 nm (5 mW
55 is contribution, the only NMR active, stable krypton isotope (83)Kr (spin I = (9)/(2)) is explored as
56 tmosphere of Mars has different (solar-type) krypton isotope ratios, indicating that it is not a prod
63 vestigate diffusive transport of xenon (Xe), krypton (Kr), and sulfur hexafluoride (SF(6)) through in
66 ately dependent on small fluctuations in the krypton loading but differ strongly between some of the
67 f commensurate-incommensurate transitions in krypton monolayers adsorbed on graphite, in which there
69 surements revealed the mass transport of the krypton radioisotopes through the target-water processin
71 ctory elements occurred simultaneously, with krypton recording concomitant accretion of non-solar vol
72 placed in each quadrant of the fundus with a krypton red laser (614 nm, 50 microm, 0.05 second, 200 m
75 ion data ( u , u RMS', vRMS' ) recorded with Krypton Tagging Velocimetry (KTV) at 100 kHz in a hypers
76 of volatile radionuclides such as xenon and krypton that evolve into reprocessing facility off-gas i
78 In this study, dissolved gases (methane, krypton) were injected into a coastal plain stream in No
81 al practical potential for the separation of krypton, xenon and radon from air at concentrations of o