Matches in SemOpenAlex for { <https://semopenalex.org/work/W2294888750> ?p ?o ?g. }
- W2294888750 abstract "Ionic liquids (ILs), which have widely tunable structural motifs and intermolecular interactions with solutes, have been proposed as possible carbon capture media. To inform the choice of an optimal ionic liquid system, it can be useful to understand the details of dynamics and interactions on fundamental time scales (femtoseconds to picoseconds) of dissolved gases, particularly carbon dioxide (CO2), within the complex solvation structures present in these uniquely organized materials. The rotational and local structural fluctuation dynamics of CO2 in the room temperature ionic liquid 1-ethyl-3-methylimidazolium bis(trifluoromethylsulfonyl)imide (EmimNTf2) were investigated by using ultrafast infrared spectroscopy to interrogate the CO2 asymmetric stretch. Polarization-selective pump probe measurements yielded the orientational correlation function of the CO2 vibrational transition dipole. It was found that reorientation of the carbon dioxide occurs on 3 time scales: 0.91 ± 0.03, 8.3 ± 0.1, 54 ± 1 ps. The initial two are attributed to restricted wobbling motions originating from a gating of CO2 motions by the IL cations and anions. The final (slowest) decay corresponds to complete orientational randomization. Two-dimensional infrared vibrational echo (2D IR) spectroscopy provided information on structural rearrangements, which cause spectral diffusion, through the time dependence of the 2D line shape. Analysis of the time-dependent 2D IR spectra yields the frequency-frequency correlation function (FFCF). Polarization-selective 2D IR experiments conducted on the CO2 asymmetric stretch in the parallel- and perpendicular-pumped geometries yield significantly different FFCFs due to a phenomenon known as reorientation-induced spectral diffusion (RISD), revealing strong vector interactions with the liquid structures that evolve slowly on the (independently measured) rotation time scales. To separate the RISD contribution to the FFCF from the structural spectral diffusion contribution, the previously developed first order Stark effect RISD model is reformulated to describe the second order (quadratic) Stark effect—the first order Stark effect vanishes because CO2 does not have a permanent dipole moment. Through this analysis, we characterize the structural fluctuations of CO2 in the ionic liquid solvation environment, which separate into magnitude-only and combined magnitude and directional correlations of the liquid’s time dependent electric field. This new methodology will enable highly incisive comparisons between CO2 dynamics in a variety of ionic liquid systems." @default.
- W2294888750 created "2016-06-24" @default.
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- W2294888750 date "2016-03-11" @default.
- W2294888750 modified "2023-10-07" @default.
- W2294888750 title "Carbon dioxide in an ionic liquid: Structural and rotational dynamics" @default.
- W2294888750 cites W1637629097 @default.
- W2294888750 cites W1883779550 @default.
- W2294888750 cites W1912811808 @default.
- W2294888750 cites W1965324518 @default.
- W2294888750 cites W1966781307 @default.
- W2294888750 cites W1967177165 @default.
- W2294888750 cites W1970303261 @default.
- W2294888750 cites W1970809916 @default.
- W2294888750 cites W1974292841 @default.
- W2294888750 cites W1979132441 @default.
- W2294888750 cites W1982219464 @default.
- W2294888750 cites W1982479518 @default.
- W2294888750 cites W1983279743 @default.
- W2294888750 cites W1985515789 @default.
- W2294888750 cites W1987998850 @default.
- W2294888750 cites W1993313094 @default.
- W2294888750 cites W1993935900 @default.
- W2294888750 cites W1994316904 @default.
- W2294888750 cites W1998643104 @default.
- W2294888750 cites W2004620717 @default.
- W2294888750 cites W2005307077 @default.
- W2294888750 cites W2008760545 @default.
- W2294888750 cites W2011069586 @default.
- W2294888750 cites W2014464559 @default.
- W2294888750 cites W2017798184 @default.
- W2294888750 cites W2027186143 @default.
- W2294888750 cites W2029799575 @default.
- W2294888750 cites W2032764009 @default.
- W2294888750 cites W2036329457 @default.
- W2294888750 cites W2036801435 @default.
- W2294888750 cites W2043438870 @default.
- W2294888750 cites W2044585912 @default.
- W2294888750 cites W2050410865 @default.
- W2294888750 cites W2054748396 @default.
- W2294888750 cites W2056624015 @default.
- W2294888750 cites W2062396111 @default.
- W2294888750 cites W2063034973 @default.
- W2294888750 cites W2067051784 @default.
- W2294888750 cites W2070374323 @default.
- W2294888750 cites W2073421746 @default.
- W2294888750 cites W2075187353 @default.
- W2294888750 cites W2077894462 @default.
- W2294888750 cites W2081453625 @default.
- W2294888750 cites W2085470754 @default.
- W2294888750 cites W2087872396 @default.
- W2294888750 cites W2091230747 @default.
- W2294888750 cites W2101357626 @default.
- W2294888750 cites W2108595869 @default.
- W2294888750 cites W2109467211 @default.
- W2294888750 cites W2122250145 @default.
- W2294888750 cites W2122765546 @default.
- W2294888750 cites W2123453296 @default.
- W2294888750 cites W2125368238 @default.
- W2294888750 cites W2127577365 @default.
- W2294888750 cites W2128097747 @default.
- W2294888750 cites W2136939531 @default.
- W2294888750 cites W2156157987 @default.
- W2294888750 cites W2156454985 @default.
- W2294888750 cites W2160282773 @default.
- W2294888750 cites W2161787079 @default.
- W2294888750 cites W2165357882 @default.
- W2294888750 cites W2170317460 @default.
- W2294888750 cites W2228832545 @default.
- W2294888750 cites W2261642496 @default.
- W2294888750 cites W2301085974 @default.
- W2294888750 cites W2312242294 @default.
- W2294888750 cites W2313154154 @default.
- W2294888750 cites W2317517838 @default.
- W2294888750 cites W2320184831 @default.
- W2294888750 cites W2322182491 @default.
- W2294888750 cites W2327992839 @default.
- W2294888750 cites W2330884986 @default.
- W2294888750 cites W2332846646 @default.
- W2294888750 cites W2335324453 @default.
- W2294888750 cites W2470841300 @default.
- W2294888750 cites W331729359 @default.
- W2294888750 cites W4248104288 @default.
- W2294888750 cites W4250548700 @default.
- W2294888750 doi "https://doi.org/10.1063/1.4943390" @default.
- W2294888750 hasPubMedId "https://pubmed.ncbi.nlm.nih.gov/26979696" @default.
- W2294888750 hasPublicationYear "2016" @default.
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