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1 ds is limited for xenon and even more so for krypton.
2 e mid-1940s, of less than 5 dpm per liter of krypton.
3 ion in the solid and gas phases of argon and krypton.
4 tion after inhalation of a mixture of stable krypton (80%) and oxygen (20%), with reconstruction of d
5 been used to count individual krypton-85 and krypton-81 atoms present in a natural krypton gas sample
7 d the release thereby of the fission product krypton-85 (half-life = 10.71 years, fission yield = 0.2
8 tral atoms has been used to count individual krypton-85 and krypton-81 atoms present in a natural kry
11 he binding of xenon and, to a lesser degree, krypton and argon, tend to expand the volume of the cavi
12 The level of enhancement after inhalation of krypton and its excellent clinical tolerance makes this
16 topic composition, heavy noble gases (argon, krypton and xenon) have an isotopic composition very sim
18 purely hydrophobic solutes (methane, ethane, krypton, and xenon) to study hydrophobicity at the most
21 recently designed pressurization cell using krypton at high pressure, a new gas binding site has bee
22 sly binds to the noble gases (Ngs) xenon and krypton at room temperature in a reaction that is typica
23 udy the phase behavior of adsorbed argon and krypton atoms as well as their coupling to the substrate
24 Vacuum ultraviolet spectra emanating from krypton atoms, exposed to intense waveform-controlled op
26 alled CNTs filled with lead, barium and even krypton can be produced, and externally decorated with p
28 current induced vacuum ultraviolet (dc-VUV) krypton discharge lamp and an alternating current, radio
33 85 and krypton-81 atoms present in a natural krypton gas sample with isotopic abundances in the range
34 ays is tested in canine lung tissue by using krypton gas with natural abundance isotopic distribution
36 ction of 5 x 10(-9) Torr partial pressure of krypton in argon with a signal-to-noise ratio of approxi
37 Raman spectroscopy was performed using a krypton ion laser providing excitation at 406.7 nm (5 mW
38 is contribution, the only NMR active, stable krypton isotope (83)Kr (spin I = (9)/(2)) is explored as
42 ately dependent on small fluctuations in the krypton loading but differ strongly between some of the
43 f commensurate-incommensurate transitions in krypton monolayers adsorbed on graphite, in which there
44 placed in each quadrant of the fundus with a krypton red laser (614 nm, 50 microm, 0.05 second, 200 m
46 of volatile radionuclides such as xenon and krypton that evolve into reprocessing facility off-gas i
48 In this study, dissolved gases (methane, krypton) were injected into a coastal plain stream in No
51 al practical potential for the separation of krypton, xenon and radon from air at concentrations of o
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