A. Reynoso et al.
Journal of Photochemistry & Photobiology, A: Chemistry 412 (2021) 113213
O2(1Δg) by TCS, kr (see process (11) presented in Scheme 1), was
determined by the method introduced by Foote and Ching [34]. The PN
synthetic sensitizer was used as O2(1Δg) generator. Assuming the reac-
tion of O2(1Δg) with the substrate is the only form of oxygen con-
sumption, the ratio of the slope of pseudo first-order plot for oxygen
consumption by TCS and by a reference compound (with a known krRef
value), under identical conditions, is equal to krTCS / krRef ratio. The
reference (Ref) used was FFA, with a reported krRef value in H2O-MeOH
of 6.2 × 107 Mꢀ 1 s-1 [28,29].
In all cases, conversions less than 10 % were used to avoid possible
interference from the photoproducts.
2.2.4. Time resolved phosphorescence detection of O2(1Δg) (TRPD)
The overall rate constant for deactivation of O2(1Δg) by TCS (kt = kq
+ kr, processes (12) and (11), in Scheme 1) was determined using a
previously described method [36]. Briefly, a Nd:YAG laser (Spectron
Laser System, SL400) was used as excitation source. The output at
355 nm was used to excite PN, and the O2(1Δg) emission at 1270 nm was
detected at right angles using an amplified Judson J16 / 8Sp germanium
detector, after passing through the appropriate filters. The detector
output was coupled to an Agilent Technologies DSO 6012A digital
oscilloscope and a personal computer for signal processing. In general,
6–8 shots were averaged, in order to achieve a good signal / noise ratio,
from which the decay curve was obtained [37]. D2O-MeOD, instead of
H2O-MeOH, was used as a solvent to extend the lifetime of O2(1Δg) [29].
From a first order fitting of the decay the lifetime of O2(1Δg) was eval-
Fig. 2. Changes in the UV–vis difference absorption spectra in air equilibrated
H2O-MeOH 1:1 v/v solution of 0.035 mM Rf plus 0.1 mM TCS upon irradiation
at 470 nm, taken vs. 0.035 mM Rf in the same solvent. Inset A: Changes in the
UV–vis difference absorption spectra of 0.035 mM Rf plus 0.1 mM TCS vs
0.035 mM Rf in Ar-saturated H2O-MeOH 1:1 v/v solutions. Irradiation times for
both figures: 0, 60, 120, 480, 2040s. Inset B: absorbance decrease of TCS at
280 nm in air equilibrated (-◼-) in Ar-saturated (-▸-).
was irradiated at λ> 450 nm in the same device used in the steady-state
photolysis experiments previously described in section 2.3. Aliquots to
different irradiation time were analyzed by UHPLC-MS / MS to photo-
products determination. The identification of the degradation products
formed was carried out from the mass-to-charge ratios, isotopic relation
of chlorine atoms, and spectra of the [Mꢀ H]ꢀ ions produced in the
negative electron spray ionization- (ESIꢀ ) mode. Also, the MS spectra
obtained were compared with reference spectra reported by other au-
thors [38,39]. This procedure allows us to guarantee the proposed
products structure with 99 % confidence.
uated in the presence (τ) and absence (τ0) of TCS, and the data were
plotted as a function of TCS concentration, according to a simple
Stern-Volmer treatment.
2.3. TCS degradation products
To obtain the photolysis products of TCS in the presence of Rf, a
home-made photoreactor was used, equipped with a merry-go-round
equipped with nine LEDs that emitting at 470 nm. In this region, the
absorption was due only to Rf. The irradiation was carried out for
300 min, taking aliquots every 30 min, which were kept in the dark until
further analysis.
MZmine 2.13.1 was used for data extraction and analysis of the
transformation product [40].
The degradation products of TCS were identified by an ultra-
performance liquid chromatography-tandem mass spectrometer
(UHPLC-MS/MS) analysis, using an ACQUITY UPLCTM system (Waters
Corp., Milford, MA, USA) coupled to a Quattro Premier TM XE tandem
quadrupole mass spectrometer (Waters, Manchester, UK). Mass Lynx 4.1
software equipped with Quan Lynx software (Waters) was used to con-
trol the instruments and to process the data. ACQUITY UPLC equipment
consisting of a binary pump, an auto-sampler, and a column heater was
used. Chromatographic separation was carried out on a UPLC BEH C18
3. Results and discussion
The results are interpreted and discussed by the mechanism shown in
Scheme 1, where Rf is the photosensitizer and TCS is the substrate that
can react with Rf electronic excited states (Rf*) or with the reactive
oxygen species (ROS) generated from Rf*. This scheme represents a
generic photosensitized process in which the absorption of visible light
promotes the sensitizer to electronically excited states singlet (1Rf*) and
triplet (3Rf*) (processes (1) and (3)). 3Rf* can transfer an electron to
oxygen in its ground state generating the superoxide radical anion
species (O●2 ꢀ ) (process (7)) or transfer energy to it generating the singlet
oxygen species (O2(1Δg)) (process (8)). The latter can decompose by
collision with solvent molecules (process (10)) or it can interact chem-
ically (process (11)) or physically (process (12)) with the photo-
oxidizable substrate.
(1.7 μm, 2.1 × 100 mm; Waters). Solvent A was water (0.1 mM NH4Ac/
0.01 % formic acid), and solvent B was methanol (0.1 mM NH4Ac/0.01
% formic acid). The flow rate was set at 0.3 mL minꢀ 1 and the column
temperature was 35 ◦C.The chromatography was performed as follows:
B was 10 % in 0ꢀ 0.5 min, linearly increased to 90 % in 0.5ꢀ 9 min; held
at 90 % for 9 ꢀ 12 min and returning to the initial condition in 1 min. An
auto-sampler was used to inject 20 μL of the samples. The Quattro Pre-
mier TM XE tandem quadrupole mass spectrometer was operated in a
negative mode with the electrospray-ionization (ESI) source. The oper-
ating parameters were optimized under the following conditions:
capillary voltage, 3 kV, ion source temperature 120 ◦C, desolvation
temperature 450 ◦C, cone gas flow 80 L hꢀ 1, desolvation gas flow 800 L
hꢀ 1(both gases were nitrogen) and collision gas flow 0.3 mL min-
ꢀ 1(argon gas). Liquid chromatography–mass spectrometry (LC–MS) full-
scan was used to select a list of molecular ions whose levels are signif-
icantly altered between case and control samples. These molecules are
then subjected to precursor-ion (PI) scans to acquire MS/MS data by
manually setting the m/z values of the PIs.
3.1. Photosensitized degradation
The experiments were performed at pH conditions where the neutral
form of TCS is the main species (Fig. 1). Spectral changes were observed
in a difference spectra of an irradiated (λ > 450 nm) solution of
0.035 mM Rf plus 0.1 mM TCS vs 0.035 mM Rf in H2O–MeOH (Fig. 2), a
region where TCS does not absorb (see figure S1 with the absorption
spectrum of Rf for comparative purposes). The time evolution of the
absorption spectrum was evaluated in air (Fig. 2, main) and inert at-
mosphere (Fig. 2, inset), to discern the oxygen participation in the
photosensitized process. The differences between the spectra shown in
A solution of 0.1 mM TCS plus 0.04 mM Rf in MeOH-H2O mixture
3