Journal of the American Chemical Society
Article
performance. Moreover, the data unequivocally establish that
catalyst structure and binding mode are far more relevant to
catalytic activity than acidity.
hypsochromic shift in Figure 1. An increased shift (lower λmax)
is predicted for binders of ostensibly greater strength (e.g.,
proton > benzoic acid > phenol).
The UV absorption behavior of the sensor with the
hydrogen-bonding agent can be represented as shown in
Figure 2a. The lowest energy electronic transition may be
ascribed to the n (HOMO) to π* (LUMO) transition, ΔE1,
corresponding to the measured λmax. As supported by the above
calculations, addition of a hydrogen-bonding agent stabilizes
the ground state (HOMO) to a greater extent than the excited
state (LUMO), i.e., ΔE3 > ΔE2. As a consequence, a
hypsochromic shift is observed upon interaction of the sensor
with the hydrogen-bond donors. For comparison, Figure 2b
illustrates the energy diagram for a typical reaction with a
hydrogen-bonding catalyst, in which catalysis is effected by
LUMO-lowering of the electrophile (ΔEa). We hypothesized
that ΔE3 − ΔE2 is proportional to ΔEa, i.e., the wavelength shift
of the bound sensor•catalyst is proportional to the rate
enhancement afforded in a reaction with the hydrogen-bonding
catalyst.
2. RESULTS AND DISCUSSION
2.1. Application of a Colorimetric Probe for Determin-
ing LUMO Activation. A key consideration in designing a
method for measuring hydrogen-bond strengths is the very
broad range of these noncovalent interactions (0.2−40 kcal/
mol).9 Observing the very weak range of these interactions is a
challenge with commonly employed spectroscopic techniques.
For example, despite successful application in measuring Lewis
Acid binding effects,10 preliminary NMR studies proved too
insensitive for detecting the interactions of weak hydrogen-
bonding catalysts with a carbonyl acceptor.11
We proposed an alternative approach using the sensitivity of
UV−vis absorption profiles, in which a change in electronic
excitation of an acceptor chromophore occurs upon binding to
a hydrogen-bond donor (Scheme 1). Specifically, imidazopyr-
azinone S displays solvatochromism with protic solvents as well
as color changes with a small number of Lewis Acids.12 We
postulated that upon treatment with various hydrogen-bond
donors, the carbonyl moiety of S would act as an acceptor
moiety. The resulting hydrogen-bonding interaction would
alter the electronic transition of the chromophore, detectable
by simple UV−vis spectroscopy.
2.2. Correlation of Binding with Sensor Wavelength
Shift. As shown in Figure 1, a continuous wavelength shift was
revealed upon saturation of the sensor with the catalyst. The
lack of two distinct peaks in intermediate measurements
containing both bound and unbound sensor indicates a rapid
equilibration. Thus, plots of absorbance vs [catalyst] (see
Figure 3 for an example with bisamidinium 12) were used to
determine the binding constants (Keq) for the sensor•catalyst
complex. A significant range of blue shifts was observed for the
different catalyst donors, ranging from ∼490 to 465 nm (Δλmax
In line with this reasoning, treatment of sensor S in
dichloromethane with various hydrogen-bond donors resulted
in visible hypsochromic (blue) shifts (Figure 1). Importantly,
∼10−30 nm). In general, catalysts with larger Δλ
values
max
possessed much stronger binding constants. Since ΔE1 is
proportional to 1/λmax, the energetics of the interaction of the
sensor with the catalysts (ΔE3 − ΔE2) is proportional to 1/
λmax(sensor•catalyst) − 1/λmax(sensor). Indeed, a good
correlation of this inverse wavelength shift with ln(Keq) was
found (Figure 4). Note that in this plot, both axes are linearly
proportional to energy terms: Δλ−1 to the ΔE of the sensor
electronic absorption, and ln(Keq) to ΔG of sensor•catalyst
formation. Importantly, this relationship establishes the
observed wavelength shift as a reliable gauge for binding
affinity of a catalyst to the sensor molecule.
Using the sensor•catalyst wavelength shift as predictors of
catalyst reactivity yields several noteworthy observations. Diol-
based 30 (TADDOL) and silanol catalysts 31 and 32 afforded
very weak shifts, despite application in numerous trans-
formations, including Rawal’s seminal report on the asymmetric
hetero Diels−Alder reaction.14 The greater λmax shift of 32
compared to the related monosilanol 31 mirrors the increased
reactivity of this silanediol scaffold, as elegantly reported by
Mattson15 and Franz.16,17 Benzoic acids and phenols spanned
the intermediate range of sensor shifts, with trends clearly based
on the electronic effects of aromatic substitution. Although
these structures are not as commonly incorporated as
hydrogen-bond catalysts, Schafmeister and co-workers have
recently demonstrated the spiroligozyme catalyst 24, containing
a carefully arranged carboxylic acid and phenol, as an effective
ketosteroid isomerase mimic for the aromatic Claisen
rearrangement.18 N,N′-Diaryl thioureas and ureas, particularly
those with multiple trifluoromethyl substituents such as
Schreiner’s catalyst 4,19 afforded some of the largest sensor
shifts, indicative of the immense utility of these structures in
various organocatalysts.20 The internally activated BF2-urea 9
Figure 1. Response in the UV−vis spectrum of S upon increasing
amounts of 12. [S] = 2.22 × 10−5 M in CH2Cl2, [12] = 0 to 1.78 ×
10−4 M.
compounds anticipated to be weaker donors, such as
diphenylthiourea (1), yielded significant changes in sensor
signal. Variation of binder concentration resulted in titration-
like behavior, with a measurable end point upon saturation of
sensor with catalyst. An array of catalysts (Chart 1), varying in
structure and anticipated strength, was examined with the
colorimetric sensor, and the Δλmax upon saturation was
determined.
DFT molecular orbital calculations were performed on
bound and unbound sensor for selected hydrogen-bonding
agents to gauge the orbital perturbation (Table 1). The
calculated lowest energy transition accurately predicts the
observed absorbance maximum for the free sensor. More
importantly, the HOMO−LUMO energy gap was larger for all
bound complexes, in accord with the empirically observed
B
dx.doi.org/10.1021/ja5086244 | J. Am. Chem. Soc. XXXX, XXX, XXX−XXX