420
M.P. Serrano et al. / Free Radical Biology and Medicine 96 (2016) 418–431
purity 499.998%), previously saturated in water. In the case of
oxygen-saturated solutions, the same procedure as that explained
for air was carried out to ensure a high enough concentration of
the gas.
counting equipment FL3 TCSPC-SP (Horiba Jobin Yvon), described
elsewhere [47].
For a given solution, the decay curve was recorded at multiple
emission wavelengths to construct the time-resolved emission
spectra (TRES), 3D data set of counts versus time and versus wa-
velength. The Global Analysis of TRES, a fit calculation (up to
5 exponentials) performed globally on up to 100 separate decay
curves, was carried out using the DAS6 Fluorescence Decay Ana-
lysis software.
2.3. Analysis of irradiated solutions
2.3.1. UV–vis spectrophotometry
Electronic absorption spectra were recorded on a Shimadzu
UV-1800 spectrophotometer, using quartz cells of 0.4 cm optical
path length. The absorption spectra of the solutions were recorded
at regular intervals of irradiation time.
2.6. Singlet oxygen (1O2) detection
The experiments were carried out at room temperature using
D2O as a solvent since the lifetime of 1O2
(
τΔ) is much longer in
2.3.2. High-performance liquid chromatography
D2O than in H2O [48,49]. The sample solution (0.8 mL) in a quartz
cell (1 cm ꢁ 0.4 cm) was irradiated with a pulsed LED source
(SpectraLED, maximum emission at 560 nm, light pulse duration
A high-performance liquid chromatography equipment Pro-
minence from Shimadzu (solvent delivery module LC-20AT, on-
line degasser DGU-20A5, communications bus module CBM-20,
auto sampler SIL-20A HT, column oven CTO-10AS VP, photodiode
array (PDA) detector SPD-M20A and fluorescence (FL) detector RF-
20A) was employed for monitoring the reaction. A Synergi Polar-
RP column (ether-linked phenyl phase with polar endcapping,
200
s). The 1O2 emission at 1270 nm was registered and analyzed
μ
using the equipment described elsewhere [40].
3. Results and discussion
150 ꢁ 4.6 mm, 4
μ
m, Phenomenex) was used for product separa-
tion. A solution of 25 mM formic acid (pH¼3.2) was used as mo-
3.1. Photosensitization of dTMP by pterin in air-equilibrated
solutions
bile phase.
2.3.3. Mass spectrometry analysis
The first aim of this work was to find out if upon UV-A irra-
diation pterin (Ptr) was able to photoinduce damage, not only in
the purine nucleotides as previously published [38–42], but also in
the pyrimidine nucleotides which are less susceptible to oxidation,
partly due to their higher redox potential. Therefore air-equili-
brated aqueous solutions containing Ptr and thymidine 5′-mono-
phosphate (dTMP) were exposed to UV-A radiation (350 nm) for
different periods of time. The pH range (5.5–6.0) was chosen so
that Ptr was present at more than 99% in its acid form (pKa 7.9).
The corresponding absorption spectra of Ptr and dTMP (Fig. 1)
show that only Ptr was excited under these experimental condi-
tions. The samples were analyzed by UV–vis spectrophotometry
and HPLC using the absorbance detector (HPLC-PDA, Section 2).
The concentration of dTMP decreased significantly as a function of
the irradiation time, whereas the decrease of the Ptr concentration
was very slow (Fig. 2, dTMP (●) and Ptr (▼)). Irradiation of Ptr
solutions in the absence of dTMP showed that the consumption of
Ptr was identical, within experimental error, to that registered in
The liquid chromatography equipment coupled to mass spec-
trometry (LC/MS) system consisted of an UPLC chromatograph
(ACQUITY UPLC from Waters) coupled to a quadrupole time-of-
flight mass spectrometer (Xevo G2-QTof-MS from Waters) (UPLC-
QTof-MS). UPLC analyses were performed using an Acquity UPLC
BEH C18 (1.7
μm; 2.1 ꢁ 50 mm) column (Waters), and isocratic
elution with 25 mM formic acid (pH¼3.2) at a flow rate of
0.2 mL minꢂ1. The mass spectrometer was operated in the nega-
tive ion mode. Therefore the samples were injected into the
chromatograph, the components were separated and then the
mass spectra were registered for each peak of the corresponding
chromatograms. In addition, mass chromatograms, i.e. re-
presentations of mass spectrometry data as chromatograms (the
x-axis representing time and the y-axis signal intensity), were
registered using different scan ranges.
2.4. Electron paramagnetic resonance-spin trapping experiments
the presence of the nucleotide (Fig. 2, Ptr ( )). Consequently, the
Δ
Electron paramagnetic resonance (EPR) experiments were
performed in order to detect the dTMP radical cation. EPR spectra
were collected on a Bruker ESP 500E spectrometer. Samples were
irradiated with Rayonet RPR3500 lamps. The following instru-
mental settings were employed for the measurements: microwave
power, 20 mW; field modulation amplitude, 0.1 mT; field mod-
ulation frequency,100 kHz; microwave frequency, 9.77 GHz.
Nitrones are common reagents for the detection and identifi-
cation of transient radicals due to their ability to form persistent
radical adducts that are detectable and fingerprintable by EPR
spectroscopy [44,45]. In our experiments, 5,5-dimethyl-1-pyrro-
line-N-oxide (DMPO) from Sigma was used as the spin trap [46].
consumption of the photosensitizer was due to its own photolysis.
Additional control experiments showed that no consumption of
the nucleotide was detected in dTMP solutions irradiated in the
absence of Ptr (Fig. 2, dTMP (○)), thus excluding the possibility of
product formation by spurious direct excitation of dTMP. More-
over, dTMP degradation was not observed in solutions containing
Ptr and dTMP that were kept in the dark. The products formed in
solutions containing Ptr and dTMP under irradiation were ana-
lyzed by HPLC and mass spectrometry (vide infra).
3.2. Photosensitization of dTMP by pterin in O2-free solutions
Samples (1 mL) contained 180 M Ptr, 1.3 mM dTMP, buffer Tris/
μ
In the experiments carried out in the absence of O2, under
otherwise the same experimental conditions, the dTMP concentration
also decreased as a function of irradiation time (Fig. 3). However, the
rate of consumption of dTMP was slower than that observed under
aerobic conditions (Fig. 2). In addition, a significant consumption of
Ptr was also observed (Fig. 3) and such consumption cannot be at-
tributed to the photochemistry of Ptr itself since, as previously re-
ported, this compound is photostable in O2-free solutions [32].
Moreover, a control experiment carried out in the absence of dTMP
HCl (pH 7.0), and DMPO (50 mM). The O2-free solutions were ir-
radiated at room temperature in sealable quartz cells of 0.4 cm
optical path length. EPR spectra were recorded every minute since
the beginning of the irradiation up to 15 min.
2.5. Fluorescence measurements
Steady-state and time-resolved fluorescence measurements
were performed at room temperature using a single-photon-