Matches in SemOpenAlex for { <https://semopenalex.org/work/W2289687887> ?p ?o ?g. }
- W2289687887 endingPage "703" @default.
- W2289687887 startingPage "693" @default.
- W2289687887 abstract "The photochemistry of pivaloyl, benzoyl, 4‐phenylbenzoyl, and 2‐anthroyl azides has been studied using femtosecond (fs) time‐resolved infrared (TRIR) and UV–vis spectroscopy and interpreted with the aid of computational chemistry. Density functional theory calculations revealed a significant difference in the nature of the lowest singlet excited state for these carbonyl azides. The lowest singlet excited states ( S 1 ) of p ‐phenylbenzoyl and 2‐anthroyl azides are (π,π*) in nature, while the pivaloyl and benzoyl azides S 1 states involve ( n ,π*) excitations. Nevertheless, for all acyl azides studied here, a similar, and intense, IR band at about 2100 cm −1 has been detected in the ultrafast TRIR experiments following 270 nm excitation. These bands were shifted to lower energy by about 100 cm −1 relative to the N 3 stretching mode for the ground states of these azides. These 2100 cm −1 vibrational bands were assigned to the S 1 states of acyl azides in agreement with density functional theory calculations. The decay of the acyl azide S 1 states was described by bi‐exponential functions. The fast component was attributed to the decay of the hot S 1 state and the longer component to the decay of the thermally relaxed S 1 state. A strong and broad transient absorption in the 350–650 nm spectral range was observed in the fs UV–vis experiments for p ‐phenylbenzoyl and 2‐anthroyl azides. The carrier of this absorption also decayed bi‐exponentially, and the time constants were in excellent agreement with those found in the fs TRIR experiments. The slow component of the S 1 state decay was found to be dependent on the solvent polarity. When the lifetime of the acyl azide S 1 state is substantially longer than the time constant for vibrational cooling of nascent (hot) isocyanate, the correlation between the S 1 decay and isocyanate formation was clear. The 270 nm excitation populates the S n ( n ≥ 2) states of these acyl azides. It was established that a hot nitrene is produced more efficiently from both the S n and hot S 1 states than from the relaxed S 1 state of these acyl azides. Thus, time‐resolved study provides direct experimental evidence that the S 1 state is the precursor of nitrene only when the S 1 state is pumped directly and when the S 1 state lifetime is longer than the time constant of vibrational cooling of the newborn nitrene. All of these results are consistent with the data obtained recently for 2‐napththoyl azide. Copyright © 2012 John Wiley & Sons, Ltd." @default.
- W2289687887 created "2016-06-24" @default.
- W2289687887 creator A5040137881 @default.
- W2289687887 creator A5048793815 @default.
- W2289687887 creator A5062225029 @default.
- W2289687887 creator A5071555595 @default.
- W2289687887 creator A5072466849 @default.
- W2289687887 creator A5075394278 @default.
- W2289687887 creator A5091350326 @default.
- W2289687887 date "2012-01-17" @default.
- W2289687887 modified "2023-09-26" @default.
- W2289687887 title "An ultrafast time-resolved infrared and UV-vis spectroscopic and computational study of the photochemistry of acyl azides" @default.
- W2289687887 cites W1482460480 @default.
- W2289687887 cites W1963683620 @default.
- W2289687887 cites W1972244709 @default.
- W2289687887 cites W1973689753 @default.
- W2289687887 cites W1977112925 @default.
- W2289687887 cites W1982590302 @default.
- W2289687887 cites W1985025658 @default.
- W2289687887 cites W1990185198 @default.
- W2289687887 cites W1991583740 @default.
- W2289687887 cites W1992838840 @default.
- W2289687887 cites W1993438424 @default.
- W2289687887 cites W2009648507 @default.
- W2289687887 cites W2011601505 @default.
- W2289687887 cites W2017650621 @default.
- W2289687887 cites W2023271753 @default.
- W2289687887 cites W2024851262 @default.
- W2289687887 cites W2028022118 @default.
- W2289687887 cites W2036241264 @default.
- W2289687887 cites W2038184695 @default.
- W2289687887 cites W2040372970 @default.
- W2289687887 cites W2048103440 @default.
- W2289687887 cites W2053201390 @default.
- W2289687887 cites W2064828707 @default.
- W2289687887 cites W2070923891 @default.
- W2289687887 cites W2073629346 @default.
- W2289687887 cites W2078511509 @default.
- W2289687887 cites W2078596450 @default.
- W2289687887 cites W2082037815 @default.
- W2289687887 cites W2083032388 @default.
- W2289687887 cites W2093089582 @default.
- W2289687887 cites W2093884731 @default.
- W2289687887 cites W2095846432 @default.
- W2289687887 cites W2114308066 @default.
- W2289687887 cites W2143981217 @default.
- W2289687887 cites W2153174264 @default.
- W2289687887 cites W2162881471 @default.
- W2289687887 cites W2314826447 @default.
- W2289687887 cites W2328524028 @default.
- W2289687887 cites W4241925869 @default.
- W2289687887 cites W2018190889 @default.
- W2289687887 doi "https://doi.org/10.1002/poc.2903" @default.
- W2289687887 hasPublicationYear "2012" @default.
- W2289687887 type Work @default.
- W2289687887 sameAs 2289687887 @default.
- W2289687887 citedByCount "32" @default.
- W2289687887 countsByYear W22896878872012 @default.
- W2289687887 countsByYear W22896878872013 @default.
- W2289687887 countsByYear W22896878872014 @default.
- W2289687887 countsByYear W22896878872015 @default.
- W2289687887 countsByYear W22896878872016 @default.
- W2289687887 countsByYear W22896878872017 @default.
- W2289687887 countsByYear W22896878872018 @default.
- W2289687887 countsByYear W22896878872019 @default.
- W2289687887 countsByYear W22896878872020 @default.
- W2289687887 countsByYear W22896878872022 @default.
- W2289687887 crossrefType "journal-article" @default.
- W2289687887 hasAuthorship W2289687887A5040137881 @default.
- W2289687887 hasAuthorship W2289687887A5048793815 @default.
- W2289687887 hasAuthorship W2289687887A5062225029 @default.
- W2289687887 hasAuthorship W2289687887A5071555595 @default.
- W2289687887 hasAuthorship W2289687887A5072466849 @default.
- W2289687887 hasAuthorship W2289687887A5075394278 @default.
- W2289687887 hasAuthorship W2289687887A5091350326 @default.
- W2289687887 hasConcept C120665830 @default.
- W2289687887 hasConcept C121332964 @default.
- W2289687887 hasConcept C147597530 @default.
- W2289687887 hasConcept C152365726 @default.
- W2289687887 hasConcept C153642686 @default.
- W2289687887 hasConcept C158355884 @default.
- W2289687887 hasConcept C178790620 @default.
- W2289687887 hasConcept C180188523 @default.
- W2289687887 hasConcept C181500209 @default.
- W2289687887 hasConcept C184779094 @default.
- W2289687887 hasConcept C185544564 @default.
- W2289687887 hasConcept C185592680 @default.
- W2289687887 hasConcept C20853536 @default.
- W2289687887 hasConcept C32891209 @default.
- W2289687887 hasConcept C33062035 @default.
- W2289687887 hasConcept C62520636 @default.
- W2289687887 hasConcept C75473681 @default.
- W2289687887 hasConcept C95503338 @default.
- W2289687887 hasConceptScore W2289687887C120665830 @default.
- W2289687887 hasConceptScore W2289687887C121332964 @default.
- W2289687887 hasConceptScore W2289687887C147597530 @default.
- W2289687887 hasConceptScore W2289687887C152365726 @default.
- W2289687887 hasConceptScore W2289687887C153642686 @default.