4142
C. Boutin et al. / Bioorg. Med. Chem. 19 (2011) 4135–4143
4.5.2. Fluorescent labeling
columns can be directly compared. Due to the high xenon magne-
tization available in the gaseous phase, the values given in Table 1
correspond to the sum of two non-selective spectra for the first col-
umn, and six selective sub-spectra (two tube shakings) for the sec-
ond and third columns.
Cells were incubated with 200 nM of fluorescent probe for 1 h.
The cells were washed 3 times with PBS at 277 K to block the
membrane dynamics. The cells were then were fixed on the glass
substrate using 5% PFA for 30 min at 277 K. The observation was
made using an inverted microscope.
Acknowledgments
4.5.3. Preparation of the pronase sample
The cells were treated with a 2 mg/mL solution of pronase for
30 min at 310 K. The cells were then re-washed three times with
PBS and incubated with 5 lM of the biosensor for 1 h at 310 K. Fi-
Support from the French Ministry of Research (project ANR-06-
PCVI-0023 BULPOXI) is acknowledged.
nally, the cells were washed three times at 277 K to block plasma
membrane dynamics, and re-suspended in a final volume of
1.5 mL. Their viability was checked through the trypan blue exclu-
sion test.
Supplementary data
Supplementary data associated with this article can be found, in
4.6. 129Xe NMR experiments
References and notes
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The spectra were processed as follows: a line broadening of
20 Hz (no zero-filling) was applied before Fourier transformation.
As exactly the same conditions (same receiver gain, in particular)
were used for the non-selective spectra, the integration values
can be directly compared (first column of Table 1). Except for the
repetition time, the sub-spectra were also acquired in the same
experimental conditions, but obviously here the receiver gain
was different from that of the non-selective experiments. Within
each series the three sub-spectra were summed, and the peak inte-
gral values were divided by the integral value of the peak in the
corresponding non-selective experiment, in order to eliminate
the polarization fluctuations. So the values of the second and third
26. Despite
a xenon polarization level not fully reproducible, quantitative
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