C O M M U N I C A T I O N S
with extended delocalization of the phenolate anion through the π
that Eu-1 will also be effective for ratiometric CEST imaging of
system to form the quinone-like structure. This would place a more
negative charge on the carbonyl oxygen atom coordinated to the Eu
pH at physiological temperatures as well (Figure S8).
3+
ion (Figure 1). The pK derived from these optical data (6.7 ( 0.1) is
a
nearly ideal for pH measurements in biological systems. One would
predict a priori that such a resonance structure would also alter the
water exchange rate and potentially the frequency of the exchanging
15
water molecule. The CEST spectra of Eu-1 recorded at five different
pH values (Figure 3) showed a surprisingly large change in exchange
frequency over this same pH range. The pK of Eu-1 derived from
a
the CEST data was 6.5 ( 0.1 (Figure S2), nearly identical to the value
determined optically.
Figure 4. Images of a phantom containing either water (w) or 10 mM
Eu-1 adjusted to the indicated pH (9.4 T, 298 K). (a) Proton density images,
(
b) ratio water intensities after activation at 54 versus 47 ppm, and (c)
calculated pH values as determined by ratiometric CEST imaging.
3
+
In summary, a novel Eu -based PARACEST agent is reported
that provides a concentration independent measure of pH by
ratiometric CEST imaging. A unique aspect of this agent is that
the ratiometric image data can be collected at CEST activation
frequencies widely separated from the bulk water frequency and
Figure 3. pH dependence of CEST spectra for Eu-1 recorded at 9.4 T and
2
98 K. Insert: expanded view of the water exchange peak as a function of
3+
pH. [Eu ] ) 10 mM, B ) 14.1 µT, and saturation time ) 2 s.
1
a
the pK of the sensor is nearly ideal for imaging pH over a range
This unusual CEST feature suggests it may be possible to image
pH directly using Eu-1 and ratiometric CEST imaging. For example,
the ratio of CEST intensities after activation of Eu-1 at 55 versus
of interest for detecting abnormal physiology. The basic platform
technology reported here will likely prove useful in the design of
other types of responsive imaging agents as well.
4
9 ppm was found to be nearly linear between pH 6.0 and 7.6 and,
Acknowledgment. Financial support from the National Institutes
of Health (CA115531, RR02584, and EB004582) and the Robert
A. Welch Foundation (AT-584) is gratefully acknowledged.
more importantly, independent of Eu-1 concentration (Figure S5).
Other combinations of activation frequencies gave similar results.
Thus, Eu-1 offers several advantages over previously reported
ratiometric pH indicators. First, the pH measurement can be made
using a single reagent rather than a cocktail of agents, and, second,
the exchange peak in Eu-1 is shifted well away from the frequency
Supporting Information Available: Complete synthetic details,
CEST results, and ratiometric plots are provided. This material is
available free of charge via the Internet at http://pubs.acs.org.
5
of solvent protons so it can be activated without concern about
6
,16,17
partial off-resonance saturation of bulk water protons.
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To demonstrate the simplicity of using this agent for imaging pH
by MRI, CEST images of a phantom prepared from five Eu-1 samples
adjusted to different pH values (plus a control sample lacking Eu-1)
were collected at two presaturation frequencies, 54 and 47 ppm. The
CEST intensity ratio in these two images is shown in Figure 4b as a
color map. The sample containing water alone showed nearly perfect
cancellation while the CEST ratio in samples of Eu-1 varied from 0.43
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1
8
equations using previously published methods. That fitting
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.0. This result is consistent with the expected increase in water
M
(
(
8
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(
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1
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JA106018N
J. AM. CHEM. SOC. 9 VOL. 132, NO. 40, 2010 14003