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1 he adjacent phenyl group, and no evidence of Wolff rearrangement.
2 igh yields from amino acids in two steps via Wolff rearrangement.
3 onding EP beta-lactams via an intramolecular Wolff rearrangement.
4 e diazodicarbonyl moiety, results in a clean Wolff rearrangement.
5 processes: loss of nitrogen followed by the Wolff rearrangement and isomerization into diazo compoun
6 nusual wavelength selectivity indicates that Wolff rearrangement and isomerization originate from dif
10 rine 2 leads to the loss of nitrogen and the Wolff rearrangement, apparently via a carbene intermedia
11 f a key cyclobutane intermediate by a tandem Wolff rearrangement/asymmetric ketene addition, (2) a di
13 owing that azeteoporphyrin formation via the Wolff rearrangement is dependent upon the structural dis
14 Laser power dependence studies show that the Wolff rearrangement is induced by two-photon absorption
15 te that leads to elimination of nitrogen and Wolff rearrangement is one of the highest singlet excite
16 Taken together, the results suggest that the Wolff rearrangement is subject to the same kind of nonst
22 ntal and computational results indicate that Wolff rearrangement of the diacetylcarbene occurs with a
23 fies this intermediate as resulting from the Wolff rearrangement of the diazochlorins upon N(2) loss.
25 profile analyses reveal that the barrierless Wolff rearrangement proceeds via an out-of-plane carbene
26 becomes electron-rich, and the photoinduced Wolff rearrangement produces a highly emissive rhodol dy
27 ) acetate leads to a remarkably facile "thia-Wolff rearrangement", producing thio-substituted ketenes
28 s shown to be more effective in facilitating Wolff rearrangement than copper(I), although both are mo
30 egrees C results in decarbonylation of 1 and Wolff rearrangement to fulven-6-one (13) either concerte
31 n-poor core and, upon irradiation, undergoes Wolff rearrangement to give a ring-expanded xanthene cor
32 N,N-diethyl diazoamides) or almost exclusive Wolff rearrangement to ketenes (in the case of the cycli
35 H insertion product 6, while products of the Wolff rearrangement were not detected in both cases.
36 Thermal decomposition of 1 leads to clean Wolff rearrangement, while heating of 2 causes quantitat
37 nm it results in efficient (phi(254) = 0.34) Wolff rearrangement, while irradiation with 355 nm light
38 ions yields ketoester 3a, the product of the Wolff rearrangement, while products produced from the si
39 cy than the ketone analogue due to competing Wolff rearrangement (WR) in the excited state of the dia
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