Journal of the American Chemical Society
Communication
hydroxycarbenes display QMT to the corresponding aldehyde.
The tunneling half-life depends on the substituent R, which in
the case of R = OH, OMe, and NH2 inhibits QMT.
band vanishes almost completely along with bands at 3545.0
(theor. 3563.1), 3306.9 (3333.6), 2036.2 (2069.9), 1327.1
(1335.2), 797.7 (806.3), and 539.0 (533.2) cm−1 all of which
can be assigned to 1t. Concomitantly, bands that can be
assigned to 2 in accordance with literature data5,17 at 2868.0
(theor. 2833.4), 2107.5 (2160.5), 1688.5 (1720.0), and 940.1
(940.9) cm−1 increase in intensity.
Shorter irradiation times at 436 nm led to an increase of
three bands that cannot be assigned to propynal (2). These
bands at 2029.1, 1263.0, and 792.1 cm−1 are barely visible after
pyrolysis, reach a maximum after 10 min of irradiation at
436 nm, and decrease before they finally vanish completely
after prolonged irradiation times (40 min). We assign these
bands to cis-ethynylhydroxycarbene (1c) based on computed
bands at 2064.3, 1265.9, and 796.8 cm−1 (Figure 1B). This
result is in analogy to previous studies on trans-trifluoro-
In general, ethynylcarbenes are relevant in astrochemical
processes23,24 and can even be used synthetically.25−29 The
electronic structure of parent ground-state triplet propynyli-
dene (HCCCH) has been explored in numerous experimental
and computational studies with the result that both terminal
carbons are equivalent in terms of their reactivity.30−32 The
photoreaction of propynylidene with triplet dioxygen provides
another entrance channel to the C3H2O PES as shown in a
study by Wierlacher et al., who observed 2 besides the
corresponding dioxirane and carbonyl oxide.33 Other triplet
ground-state derivatives of propynylidene have been inves-
tigated spectroscopically and they display similarly delocalized
electronic structures.34−36 In contrast, singlet ethynylcarbenes
(such as 1) can best be represented by a localized carbene
center in α-position to a localized CC bond.37
̈
methylhydroxycarbene (F3C−C−OH, 12) and trans-cyano-
̈
hydroxycarbene (NC−C−OH, 13), which undergo photo-
induced rotamerizations to their corresponding cis-conform-
ers.43,44 Both cis-hydroxycarbenes also vanish after prolonged
irradiation.
Herein we answer the following questions: (1) Can 1 be
generated via pyrolysis of ethynylglyoxylic acid ethyl ester (10,
Scheme 2) and (2) if so, does 1 undergo [1,2]H-tunneling to
2? We support our experiments with computations at the
CCSD(T)/cc-pVTZ and B3LYP/def2-QZVPP levels of theory
and discuss our findings in the context of previous studies.
In order to complement our photochemical experiments we
checked for QMT reactivity by keeping the as-deposited matrix
in the dark and measuring IR spectra in intervals of 1 h. We
performed three such experiments: (1) at 3 K, (2) at 20 K, and
(3) at 3 K and a 4.5 μm cutoff filter installed between the
spectrometer’s light source and the matrix window. In all three
experiments we observed a slow decay of the bands of 1t and a
simultaneous increase of those of 2 (Figure 1C). Additionally,
another such set of bands is apparent, which we assign to trans-
ethynylglyoxylic acid (9t) and its more stable cis-conformer
(9c; Figure 1D), both of which are present due to incomplete
pyrolysis of 10. Both 9c and 9t can be assigned in a spectrum
measured directly after pyrolysis as minor components (see the
We evaluated the kinetics of both QMT reactions by
integrating over the strongest IR bands of all four species (1t,
2, 9t, and 9c) and following their increase (decrease) over
time. The obtained curves were fitted to monoexponential
functions (first-order rate law) from which tunneling half-lives
details, error estimates, and the data for 9t → 9c. The kinetic
profile of the reaction 1t → 2 is not temperature dependent,
and the spectrometer beam does not seem to have a significant
impact on the associated tunneling half-life of ca. 70 h taking
the estimated relative error of ca. 12% into account. This result
clearly points toward a QMT reaction from 1t to 2, which is
further supported by CVT/SCT computations (vide infra).
We computed the potential energy surface around 1 at the
CCSD(T)/cc-pVTZ level of theory (Figure 3). Similar to
other hydroxycarbenes the 1t → 2 reaction is associated with a
substantial barrier of 31.8 kcal mol−1 and, hence, cannot be
initiated solely by excitation from the IR spectrometer in a
single photon process. IR spectra were recorded up to
7000 cm−1 corresponding to a maximum energy output of
only 20.0 kcal mol−1.
Scheme 2. High-Vacuum Flash Pyrolysis (HVFP) of 10
a
Yields 1 via 9
a
1t undergoes QMT to 2. There is a second tunneling reaction from
9t to 9c, both of which are present after pyrolysis. Irradiation of the
matrix at 436 nm leads to an increase of the concentrations of 1c and
2 while 1t vanishes nearly completely over the course of 40 min.
Carbene 1c is not photostable and vanishes after prolonged
irradiation to form 2.
We synthesized ethynylglyoxylic acid ethyl ester (10) via
oxidation of 2-hydroxybut-3-ynoic acid ethyl ester (11) with
details). Precursor 10 was obtained as a yellow to brown liquid,
which was stable for several weeks in a Schlenk tube connected
to the matrix apparatus under reduced pressure (ca. 3 ×
10−6 mbar). Gaseous 10 was pyrolyzed at 900 °C, and all
pyrolysis products were co-condensed with an excess of argon
onto the cold matrix window for IR measurements.
Mid-IR measurements of the resulting matrix revealed the
formation of CO2 and ethylene38 during the pyrolysis.
Additionally, we detected 2, acetylene,39 CO, and unreacted
10. Bands from hitherto unreported species are discussed
below. Conceivable species that are literature known (Scheme
1) like 3,40,41 4,15 and C3O42 were not observed based on
comparison with published data.
Tunneling computations using canonical variational theory
in conjunction with small curvature tunneling (CVT/SCT) at
the B3LYP/def2-QZVPP level of theory yield a QMT half-life
of 62.1 h for 1t → 2 in excellent agreement with our
experiment. The QMT half-life of 1t nicely fits in the series of
hydroxycarbenes (Figure 4). Ethynyl (sp hybridized) as a
moderate σ acceptor (−I)45,46 is expected to captodatively
After pyrolysis, a strong band at 1249.4 cm−1 coincides well
with the strongest band of 1t computed at 1238.4 cm−1
(determined anharmonically at B3LYP/def2-QZVPP). When
irradiating the matrix at 436 nm for 40 min (Figure 1A) this
3742
J. Am. Chem. Soc. 2021, 143, 3741−3746