M.L. Dántola et al.
JournalofPhotochemistry&Photobiology,B:Biology181(2018)157–163
a,V
0,V
What is the mechanism of the initial step, that is, before the photo-
sensitized process dominates the degradation of PteGlu? Unconjugated
pterins are present as impurities in the commercial presentation of fo-
lates? If so, does the photosensitization by these compounds contribute
to the photodegradation of PteGlu? When the photophysical properties,
such as the fluorescence, of PteGlu are studied, do the unconjugated
pterins, present as impurities or generated photochemically, con-
tribute?
Motivated by the importance of the photochemistry of folates in
vivo, this work was aimed to answer the questions raised in the previous
paragraph. For this purpose, aqueous solutions of PteGlu were prepared
using different commercially available solids and were analyzed by
high-performance liquid chromatography (HPLC) and mass spectro-
metry to investigate pterinic impurities. PteGlu was purified by HPLC
and the photochemical and spectroscopic properties of solutions of
purified and unpurified PteGlu were compared.
q
= q (1 − 10−A
)
n,p
n,p
(1)
where A is the absorbance of the reactant at the excitation wavelength.
2.3. High-performance Liquid Chromatography (HPLC)
A Prominence equipment 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, pho-
todiode array (PDA) detector SPD-M20A and fluorescence (FL) detector
RF-20A was employed for monitoring the photochemical processes and
to purified the PteGlu commercial sample. A Synergi Polar-RP column
(ether-linked phenyl phase with polar endcapping, 150 × 4.6 mm,
4 μm, Phenomenex) was used for isolation of PteGlu from HPLC runs
(preparative HPLC).·The column temperature was set at 25 °C and the
flow rate at 0.6 mL/min. Solution containing 100% NH4Ac (1 mM,
pH = 6.7
0.1) was used as mobile phase. The same column and runs
conditions were used to analyze the purity of the isolated PteGlu sample
and the progress of the photochemical processes.
2. Materials and Methods
2.1. General
2.4. Fluorescence Spectroscopy
2.1.1. Chemicals
Folic acid (PteGlu) was provided by Sigma Aldrich (solid I,
purity ≥ 97%) and Schircks Laboratories (solid II, purity > 98.5%).
Other pterins derivatives were purchased from Schircks Laboratories.
Ammonium acetate (NH4Ac) and formic acid (HCOOH) were purchased
from Sigma Chemical Co. Acetonitrile (ACN) was purchased from J. T.
Baker. Aqueous solutions were prepared using ultrapure water from
Milli-Q® purification system (Millipore Corporation, USA).
Steady-state and time-resolved fluorescence measurements were
performed on air-equilibrated aqueous solutions using a Single-Photon-
Counting equipment FL3 TCSPC-SP (Horiba Jobin Yvon). The equip-
ment has been previously described in detail [32].
In steady-state measurements the sample solution in a quartz cell
was irradiated with a 450 W Xenon source through an excitation
monochromator (FL-1004). The fluorescence, after passing through an
emission monochromator (iHR320), was registered at 90° with respect
to the incident beam using a room-temperature R928P detector. The
emission measurements were performed at 25 °C. Corrected fluores-
cence spectra obtained by excitation at 340 nm were recorded in the
range 375–580 nm. The total fluorescence intensities (IF) were calcu-
lated by integration of the fluorescence band centered at ca. 440 nm.
The fluorescence quantum yields (ΦF) were determined from the
corrected fluorescence spectra using the following equation:
2.1.2. Measurements of pH
A pH-meter sensION+pH31 GLP combined with a pH electrode
5010T (Hach) or microelectrode XC161 (Radiometer Analytical) were
used. The pH of the aqueous solutions was adjusted by adding drops of
0.1–0.2 M aqueous NaOH or HCl solutions with a micropipette. The
concentration of the acid and the base used for this purpose ranged
from 0.1 M to 2 M.
R IAR
ΦF = ΦF
IRA
(2)
2.1.3. UV/vis Spectrophotometric Analysis
Electronic absorption spectra were recorded at room temperature
on a Shimadzu UV-1800. Measurements were made using quartz cells of
0.4 and 1.0 cm optical path length.
where I is the integrated intensity, A is the absorbance at the excitation
wavelength and the superscript R refers to the reference fluorophore. In
our experiments, pterin in acid medium (pH = 6.0) was used as a re-
ference (ΦF = 0.32) [33]. The sample and reference were excited at the
same wavelength. To avoid inner filter effects, the absorbance of the
solutions at the excitation wavelength was kept below 0.10.
In time-resolved experiments a NanoLED source (maximum at
341 nm) was used for excitation and the emitted photons, after passing
through a monochromator, were detected by a TBX-04 detector and
counted by a FluoroHub-B module.
2.2. Steady-state Irradiation
2.2.1. Irradiation Setup
Air equilibrated aqueous solutions containing PteGlu were irra-
diated in quartz cells (1.0 cm optical path length) at room temperature
using a Rayonet RPR lamp (Southern N. E. Ultraviolet Co.) with emis-
sion centered at 350 nm (bandwidth ~ 20 nm).
2.5. Mass Spectrometry Analysis
2.2.2. Actinometry
Aberchrome 540 (Aberchromics Ltd.) was used as an actinometer
The liquid chromatography mass spectrometry system was equipped
with 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 the
Acquity UPLC BEH Phenyl (1.7 μm, 2.1 × 50 mm) column (Waters). An
isocratic elution with 90% of aqueous HCOOH (0.1% v/v) and 10% of
ACN was used as mobile phase with a flow rate of 0.2 mL/min. Mass
chromatograms, i.e. representations of mass spectrometry data as
chromatograms (the x-axis representing time and the y-axis signal in-
tensity), were registered using different scan ranges. The mass spec-
trometer was operated in both positive (ESI+) and negative (ESI−) ion
modes.
0,V
for the measurement of the incident photon flux density (q ) at the
n,p
excitation wavelength, which is the amount of incident photons per
time interval (qn0,p) and divided by the volume (V) of the sample [30].
Aberchrome 540 is the anhydride form of the (E)‑α‑(2,5‑di-
methyl‑3‑furylethylidene)(isopropylidene)succinic acid which, under
irradiation in the spectral range 316–366 nm leads to a cyclized form.
0,V
The method for the determination of q
has been described in detail
n,p
The value of q
was 3.7 ( 0.4) × 10−6 Einstein L−1 s−1. The
0,V
n,p
a,V
value of the absorbed photon flux density (
q
) was calculated from
n,p
0,V
q
according to the Lambert-Beer law:
n,p
159