Matches in SemOpenAlex for { <https://semopenalex.org/work/W2079438211> ?p ?o ?g. }
- W2079438211 endingPage "2640" @default.
- W2079438211 startingPage "2616" @default.
- W2079438211 abstract "Temperature‐dependent ESR spectra of O−2 adsorbed on Ti ions supported on porous Vycor glass were observed over the range 4.2 to 400 °K. These spectra were obtained under normal high vacuum conditions as well as under UHV conditions (P⩽10−9 Torr) and are very well resolved. It was observed that the line position of the g̃ tensor component that is perpendicular to the internuclear axis of O−2 remained constant with temperature, whereas the other two components of the g̃ tensor shift in position with temperature, and are accompanied by drastic line shape changes. This observation indicates that the molecular motion of O−2 on the surface is highly anisotropic, consisting essentially of planar rotation about the axis perpendicular to the internuclear axis of O−2 and parallel to the normal to the surface. Furthermore, the observation of nonequivalent 17O hfs of O−2 suggests that the internuclear axis of O−2 might be tilted slightly from the surface and/or one oxygen is closer to the Ti4+. The ESR line shapes were simulated for the different possible models: Brownian diffusion, jump diffusion (from weak jump to strong jump), approximate free diffusion, and discrete jump. It was found that the theoretical spectra calculated using the model of weak jump rotational diffusion best fit the observed spectra in the temperature range below 57.4 °K. However, in the temperature range above 57.4 °K, although the Brownian diffusion model seems the best among the models used, none of the present models used could successfully reproduce the observed line shapes. The rotational correlation time τR∥ was found to range between 10−5 sec (below 14.5 °K) and 10−9 sec (263 °K). The values of τR∥ depend strongly on the model used in the lower temperature range, but were essentially independent of model above 100 °K. The activation energy for rotational diffusion was estimated to be 0.5 kcal/mole above 100 °K. The line shape below 15 °K is independent of temperature, although the O−2 spectrum appears to exhibit residual motional effects. This observation suggests that coherent quantum mechanical motion is predominant below 15 °K. This matter is discussed in some detail, and the appropriate theory to investigate quantum effects on the motional dynamics is outlined including possible isotope effects on the motion. Spectral observation of possible interaction between C2H4 and O−2 on the surface is presented. Also discussed are the techniques for preparing samples with strong well‐resolved signals and for removing the other types of O−2 signals, which do not show significant temperature‐dependent spectral changes. The show." @default.
- W2079438211 created "2016-06-24" @default.
- W2079438211 creator A5016966558 @default.
- W2079438211 creator A5046753098 @default.
- W2079438211 creator A5075151360 @default.
- W2079438211 date "1981-02-15" @default.
- W2079438211 modified "2023-10-17" @default.
- W2079438211 title "ESR studies of 0<sup>−</sup><sub>2</sub>adsorbed on Ti supported surfaces: Analysis of motional dynamics" @default.
- W2079438211 cites W1749277125 @default.
- W2079438211 cites W190024905 @default.
- W2079438211 cites W1970933074 @default.
- W2079438211 cites W1973187065 @default.
- W2079438211 cites W1978575680 @default.
- W2079438211 cites W1978852781 @default.
- W2079438211 cites W1983509092 @default.
- W2079438211 cites W1983711109 @default.
- W2079438211 cites W1991456489 @default.
- W2079438211 cites W1991488874 @default.
- W2079438211 cites W2002151444 @default.
- W2079438211 cites W2008338581 @default.
- W2079438211 cites W2009742319 @default.
- W2079438211 cites W2011316251 @default.
- W2079438211 cites W2012416558 @default.
- W2079438211 cites W2018605607 @default.
- W2079438211 cites W2021203025 @default.
- W2079438211 cites W2024659946 @default.
- W2079438211 cites W2025248785 @default.
- W2079438211 cites W2026660278 @default.
- W2079438211 cites W2031173617 @default.
- W2079438211 cites W2031635772 @default.
- W2079438211 cites W2033392525 @default.
- W2079438211 cites W2034072354 @default.
- W2079438211 cites W2046108485 @default.
- W2079438211 cites W2058969938 @default.
- W2079438211 cites W2062470962 @default.
- W2079438211 cites W2064089445 @default.
- W2079438211 cites W2064274622 @default.
- W2079438211 cites W2069372826 @default.
- W2079438211 cites W2078348266 @default.
- W2079438211 cites W2085881056 @default.
- W2079438211 cites W2089689523 @default.
- W2079438211 cites W2089915823 @default.
- W2079438211 cites W2104536122 @default.
- W2079438211 cites W2112973214 @default.
- W2079438211 cites W2122076129 @default.
- W2079438211 cites W2152719559 @default.
- W2079438211 cites W2164000240 @default.
- W2079438211 cites W2164375779 @default.
- W2079438211 cites W2320753162 @default.
- W2079438211 cites W2335288621 @default.
- W2079438211 cites W2520226077 @default.
- W2079438211 cites W2736591807 @default.
- W2079438211 cites W4210970662 @default.
- W2079438211 cites W4233992656 @default.
- W2079438211 doi "https://doi.org/10.1063/1.441334" @default.
- W2079438211 hasPublicationYear "1981" @default.
- W2079438211 type Work @default.
- W2079438211 sameAs 2079438211 @default.
- W2079438211 citedByCount "60" @default.
- W2079438211 countsByYear W20794382112012 @default.
- W2079438211 countsByYear W20794382112013 @default.
- W2079438211 countsByYear W20794382112014 @default.
- W2079438211 countsByYear W20794382112017 @default.
- W2079438211 countsByYear W20794382112019 @default.
- W2079438211 countsByYear W20794382112021 @default.
- W2079438211 countsByYear W20794382112022 @default.
- W2079438211 crossrefType "journal-article" @default.
- W2079438211 hasAuthorship W2079438211A5016966558 @default.
- W2079438211 hasAuthorship W2079438211A5046753098 @default.
- W2079438211 hasAuthorship W2079438211A5075151360 @default.
- W2079438211 hasConcept C113196181 @default.
- W2079438211 hasConcept C120665830 @default.
- W2079438211 hasConcept C121332964 @default.
- W2079438211 hasConcept C1276947 @default.
- W2079438211 hasConcept C155281189 @default.
- W2079438211 hasConcept C184779094 @default.
- W2079438211 hasConcept C185592680 @default.
- W2079438211 hasConcept C198352243 @default.
- W2079438211 hasConcept C199631012 @default.
- W2079438211 hasConcept C2524010 @default.
- W2079438211 hasConcept C33923547 @default.
- W2079438211 hasConcept C39353612 @default.
- W2079438211 hasConcept C41999313 @default.
- W2079438211 hasConcept C43617362 @default.
- W2079438211 hasConcept C4839761 @default.
- W2079438211 hasConcept C69357855 @default.
- W2079438211 hasConcept C85725439 @default.
- W2079438211 hasConcept C97355855 @default.
- W2079438211 hasConceptScore W2079438211C113196181 @default.
- W2079438211 hasConceptScore W2079438211C120665830 @default.
- W2079438211 hasConceptScore W2079438211C121332964 @default.
- W2079438211 hasConceptScore W2079438211C1276947 @default.
- W2079438211 hasConceptScore W2079438211C155281189 @default.
- W2079438211 hasConceptScore W2079438211C184779094 @default.
- W2079438211 hasConceptScore W2079438211C185592680 @default.
- W2079438211 hasConceptScore W2079438211C198352243 @default.
- W2079438211 hasConceptScore W2079438211C199631012 @default.
- W2079438211 hasConceptScore W2079438211C2524010 @default.