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low electron density of the aryl ring also makes electrophilic
addition to the aryl ring more challenging. It was also worthy to
note that this reaction could easily proceed in a high yield on a
gram scale (6q).
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After the above explorations, a series of control experiments
were carried out in order to gain more informations of this
designed dual-cycle reaction mechanism. First of all, Cu(OTf)
and some other Lewis acids were surveyed as the catalyst in this
reaction (entries 11-16, Table S1). The fact that no reaction
occurred in the presence of such catalysts clearly demonstrated
that only Cu(OTf)2 could catalyze this reaction. To examine
whether this reaction was catalyzed by the in situ generated
proton, reaction of 1a in the presence of 5 mol% of HOAc was
carried out. The results indicated that no reaction took place
under the catalysis of HOAc, which ruled out the above
possibility (see Scheme S1 in Electronic Supplymentary
Information). Omission of either Cu(OTf)2 (entry 17, Table S1) or
Eosin Y (entry 18, Table S1) from the standard reaction
conditions led to no conversion, indicating that both catalysts
were key factors in this transformation. The fact that no
reaction took place under dark conditions (entry 19, Table S1)
clearly illustrated that light was necessary. Notably, under the
irradiation of 254 nm UV light, dramatically increased reaction
rate and higher yield were obtained in the absence of Eosin Y
(entry 20, Table S1), but no reaction occurred in the absence of
Cu(OTf)2 under UV irradiation (entry 21, Table S1). In such a UV
reaction, we assumed that the reaction proceeded via Cu-
catalyzed photolytic π bond cleavage process which is distinct
from catalytic SET procedure. Considering that the household
lamp operates with a wide spectral window (around 400 to 760
nm) and the Eosin Y absorbs green light (characteristic peak at
539 nm,8 the green LED lamp (520 to 530 nm, 2 W) was used
instead of the household lamp. As a result, the reaction was
greatly accelerated (entry 22, Table S1). Moreover, the reaction
under the same irradiation conditions in the absence of Eosin Y
showed no conversion (entry 23, Table S1). These results
strongly suggested that the excited state of Eosin Y was a key
intermediate in this dual-catalysis mechanism.
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In conclusion, the strategy reported herein represents a
novel activation mode of carbon-carbon triple bond. In contrast
to the traditional reaction pathway, wherein the metal-
coordinated alkyne “passively” accepts the nucleophilic attack
resulting in concomitant cleavage of the
π bond and
10 M. Orbán, React. Kinet. Catal. Lett., 1990, 42, 343.
11 Note please: All the optimization reactions were carried
out in a thin glass tube (Table S1). All the scope
exploration reactions were carried out in a thick sealed
tube (Table 1). The transmittance of the thin glass tube
is more excellent than the thick sealed tube. Thus, the
corresponding reaction time of the same substrate
under the same reaction condition was not the same.
Reactions in a thick sealed tube took longer time.
construction of two new σ bonds at the same step, this new
strategy proceeds via electrophilic addition with the former
“nucleophile” to an initially formed positive species by SET-
induced cleavage of the π bond. In such a new reaction
procedure, the cleavage of the π bond and the constructions of
two new σ bonds proceed step by step. This new activation
mode will probably find wide applications in the design of
organic reactions.
We greatly acknowledge the financial support from National
Basic Research Program of China (973 Program, 2012CB720300)
and International Science & Technology Cooperation Program
of China (2014DFE40130).
Notes and references
4 | J. Name., 2012, 00, 1-3
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