2014
DOI: 10.1021/jp506243s
|View full text |Cite
|
Sign up to set email alerts
|

Photochemistry of Matrix Isolated (Trifluoromethyl)sulfonyl Azide, CF3SO2N3

Abstract: The photochemistry of matrix isolated (trifluoromethylsulfonyl) azide, CF3SO2N3, has been studied at low temperatures. Upon ArF laser irradiation (λ = 193 nm), the azide eliminates N2 and furnishes triplet [(trifluoromethyl)sulfonyl]nitrene, CF3SO2N, which has been characterized by IR and EPR spectroscopy. Upon subsequent UV light irradiation (λ = 260-400 nm) the nitrene converts to CF3N═SO2 and CF3S(O)NO through a Curtius-type rearrangement. Further two new species CF2N═SO2F and FSNO were identified together … Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
2

Citation Types

4
40
0

Year Published

2016
2016
2020
2020

Publication Types

Select...
8

Relationship

2
6

Authors

Journals

citations
Cited by 27 publications
(44 citation statements)
references
References 47 publications
4
40
0
Order By: Relevance
“…[14] Recently,w eh ave shown that reactive a-oxo-nitrenes can be generated efficiently through the irradiation of a-oxo-azides with an ArF laser in solidn obleg as matrices. [15] For instance, the ArF laser photolysis of the matrix-isolateda cyl azide FC(O)N 3 enabled the direct observation of the carbonyl nitrene FC(O)N, [15a] which was not observed in ap revious study of the photolysis in solid matricesb yu sing am ercuryl amp (l > 200 nm). [16] The use of the short-pulseArF laser has the distinct advantage of reducing secondary irradiation of the photolabile a-oxonitrenes by the unwanted UV or visible light from the mercury or xenon lamps.…”
Section: Introductionmentioning
confidence: 99%
“…[14] Recently,w eh ave shown that reactive a-oxo-nitrenes can be generated efficiently through the irradiation of a-oxo-azides with an ArF laser in solidn obleg as matrices. [15] For instance, the ArF laser photolysis of the matrix-isolateda cyl azide FC(O)N 3 enabled the direct observation of the carbonyl nitrene FC(O)N, [15a] which was not observed in ap revious study of the photolysis in solid matricesb yu sing am ercuryl amp (l > 200 nm). [16] The use of the short-pulseArF laser has the distinct advantage of reducing secondary irradiation of the photolabile a-oxonitrenes by the unwanted UV or visible light from the mercury or xenon lamps.…”
Section: Introductionmentioning
confidence: 99%
“…An experiment in which irradiation is interrupted for defined times showed no conversion during the dark periods (see the Supporting information). To distinguish a concerted C−H insertion of triplet N ‐nonaflyl nitrene from a radical process, THF ( 2 a ) and nonaflyl azide ( 1 a ) were mixed in the presence of half or two equivalents of 2,2,6,6‐tetramethylpiperidin‐1‐oxyl (TEMPO, 10 ) in rigorously deoxygenated solution and irradiated with UV light at 25 °C for 7.5 and 3.5 h, respectively, until complete consumption of 1 a . With half an equivalent of 10 , a 1:2:1 mixture of 5 a / 4 a / 11 was observed in the crude reaction mixture, whereas with two equivalents of TEMPO ( 10 ), a 1:2 mixture of 4 a / 11 was formed with 52 % mass balance .…”
Section: Methodsmentioning
confidence: 99%
“…The following mechanism is the most consistent with all observations (Scheme ). Triplet nitrene 12 is initially formed by photolysis. Both the reaction with TEMPO ( 10 ) and the KIE speak against a concerted C−H insertion reaction via transition state 13 , but rather point to facile hydrogen‐atom abstraction from ethers 2 by nitrene 12 to generate α‐alkoxy radicals 15 .…”
Section: Methodsmentioning
confidence: 99%
“…Both signals slowly disappear while keeping the matrix in the dark, but the rate is dramatically slower than the disappearance of CF 3 C(O)N in Ar matrix (IR spectroscopy), nitrenes can still be observed after 12 h. In the more rigid Ar matrix, one strong and persistent signal occurred at around 8690 G with ZFSP of | D / hc |=1.75 cm −1 and | E / hc |=0.01 cm −1 . It corresponds to the known triplet nitrene CF 3 N (| D / hc |=1.741 cm −1 and | E / hc |=0.0 cm −1 ), which is produced through the secondary photolysis of CF 3 NCO. Two much weaker signals with x 2 and y 2 splitting at around 6250 and 8510 G (| D / hc |=1.17 cm −1 and | E / hc |=0.045 cm −1 ) vanished completely in one hour in the dark at 4.2 K (Figure S37), coinciding with the kinetics for the tunneling disappearance of CF 3 C(O)N. The observed significant variation of D values for CF 3 C(O)N in different matrices suggest the existence of interaction with surrounding molecules.…”
Section: Methodsmentioning
confidence: 99%