ISSN 0006-2979, Biochemistry (Moscow), 2025, Vol. 90, No. 7, pp. 882-893 © Pleiades Publishing, Ltd., 2025.
Russian Text © The Author(s), 2025, published in Biokhimiya, 2025, Vol. 90, No. 7, pp. 961-973.
882
Cationic Antiseptics Disrupt the Functioning
of the Electron-Transport Chain at the Acceptor Side
in the Photosynthetic Reaction Centres
of the Purple Bacterium Cereibacter sphaeroides
Evgenii P. Lukashev
1
, Mahir D. Mamedov
2
, Liya A. Vitukhnovskaya
2
,
Aida M. Mamedova
2
, Peter P. Knox
1,a
*, and Vladimir Z. Paschenko
1
1
Department of Biophysics, Faculty of Biology, Lomonosov Moscow State University,
119234 Moscow, Russia
2
Belozersky Institute of Physico-Chemical Biology, Lomonosov Moscow State University,
119992 Moscow, Russia
a
e-mail: knox@biophys.msu.ru
Received March 11, 2025
Revised May 4, 2025
Accepted May 6, 2025
AbstractUsing electrometric technique, the cationic antiseptic octenidine was revealed to reduce generation
of transmembrane electrical potential difference in the chromatophores of photosynthetic bacterium Cerei-
bacter sphaeroides. This is also confirmed by measurements of electrochromic shifts of carotenoid absorption
bands in chromatophores. In reaction centers (RCs), isolated from chromatophores in the absence of external
electron donors and acceptors, the rate of recombination between photooxidized bacteriochlorophyll P
870
and
reduced secondary quinone acceptor Q
B
, as measured by absorption changes in the near infrared region, was
very weakly dependent on the presence of antiseptics, in contrast to the kinetics in the 400-600nm spectral
range, where absorption changes associated with the oxidation of P
870
and the formation of semiquinone
radicals Q
A
and Q
B
, as well as electrochromic shifts of the carotenoid and bacteriopheophytin RC absorption
bands, were observed. The addition of cationic antiseptics modified the flash-induced absorbance changes
in this region with the formation time of ~100-200 ms and a decay time of ~3 s. In the series: picloxydine
chlorhexidine– octenidine– miramistin, the last one was the most effective. The maximum amplitude of such
changes was observed in the absorption region of the semiquinone radical around 460 nm. When electron
transfer from Q
A
to Q
B
was blocked by o-phenanthroline, the effect disappeared. Cationic antiseptics are
suggested to stimulate protonation of Q
B
with the formation of a neutral Q
B
H
+
complex.
DOI: 10.1134/S0006297925600723
Keywords: cationic antiseptics, chromatophores, reaction centers, electrogenesis, electrometric method, flash
photolysis
* To whom correspondence should be addressed.
INTRODUCTION
Currently, the widespread and uncontrolled use
of antiseptics raises a reasonable question about their
possible negative impact on the biosphere. Under-
standing the behavior of these compounds in various
environments is important for their application. Pre-
viously, we have examined the effect of cationic anti-
septics with one or two charged groups (miramistin,
octenidine, chlorhexidine, and picloxydine) on energy
transfer in the membranes of chromatophores of pho-
tosynthetic purple bacteria [1, 2], as well as on isolat-
ed nuclear complexes of photosystem II from spinach
leaves [3]. Recently, the effect of these antiseptics on
fluorescence characteristics and electron transfer was
studied in another pigment-protein complex of pho-
tosystem I from the freshwater cyanobacterium Syn-
echocystis sp. 6803 [4]. For all the abovementioned
ANTISEPTICS BLOCK Δψ GENERATION 883
BIOCHEMISTRY (Moscow) Vol. 90 No. 7 2025
medications, the most noticeable effect was observed
in the presence of octenidine. In bacterial chromato-
phores from Cereibacter sphaeroides (previously called
Rhodobacter sphaeroides), which represent a minimal
possible photosynthetic unit which is structurally and
functionally intact, the addition of octenidine led to a
decrease in the efficiency of electron excitation energy
migration from the light-harvesting complex LH2 to
the core complex LH1–RC (RC– reaction center) by ap-
proximately three times[1]. Miramistin had the weak-
est effect on this energy migration in C. sphaeroides
chromatophores. It was suggested that the disruption
of effective energy transfer occurs due to the anti-
septic binding to the hydrophilic heads of negatively
charged cardiolipin molecules located in the rings of
light-harvesting pigments on the cytoplasmic surface
of the chromatophores.
The photosynthetic electron transport chain in
C. sphaeroides chromatophores catalyzes a light-driv-
en cyclic electron flow between the RC and the cy-
tochrome bc
1
complex involving a mobile membrane
pool of ubiquinones (UQ
10
) and soluble endogenous
cytochrome c
2
.
RC is a transmembrane complex comprised of
three protein subunits (designated as L, M, and H)
with a total molecular weight of about 100 kDa.
Redox cofactors in the RC structure are organized
into two transmembrane branches, of which only
the L branch is functional. A special pair of bacte-
riochlorophylls (P
870
) is located near the periplasmic
surface of the photosynthetic membrane. The trans-
membrane protein L subunit contains monomeric
bacteriochlorophyll (BChl)a, bacteriopheophytin(BPh)
and the primary quinone acceptor Q
A
molecules,
forming the L branch, while the transmembrane sub-
unitM includes monomeric BChl, BPh, and the second-
ary quinone acceptor Q
B
, constituting the M branch.
A molecule of a specific carotenoid is also located in
the structure of the M subunit near BChl a. In par-
ticular, RCs of C. sphaeroides contain spheroidene
or spheroidenone as this carotenoid. The latter is
synthesized during bacterial growth in the presence
ofO
2
[5]. Upon light excitation of RCs, electron trans-
fer occurs from the primary electron donor P
870
to
BChl with a characteristic time of ~3 ps, then to BPh
in ~0.9 ps, to Q
A
(~200 ps) and to Q
B
(~100 μs) [6-8].
RCs from C. sphaeroides also contain three integral
lipid molecules: cardiolipin, phosphatidylcholine, and
glucosyl-galactosyl diacylglycerol[9]. This suggests the
possible existence of specific interactions between
phospholipids and electron transport components in
RCs. In particular, it was shown that the thermody-
namic and kinetic parameters of electron transfer in
the quinone acceptor unit of RCs from purple bacte-
ria depend on the presence of physiologically import-
ant lipids in their environment [9, 10]. It has been
suggested that electrostatic interactions of lipids with
quinone acceptors in RCs affect the stabilization time
of separated charges [11]. Other experiments have
shown that the packing of RCs in the lipid bilayer
of chromatophore membranes appears to increase
the pK
a
of the singly reduced secondary acceptor of
ubiquinone Q
10
, the semiquinone anion Q
B
, by al-
most three units [12] compared to its very low value
(about 4.5) in RC samples [13]. It is assumed that the
high pK
a
value of the secondary quinone promotes the
formation of neutral hydroquinone Q
B
H
+
and stimu-
lates the transfer of the second electron to it with the
formation of Q
B
2−
H
+
. This hypothesis of proton–elec-
tron events has been termed “proton-activated elec-
tron transfer” [13].
Since cationic antiseptics interact primarily with
amphiphilic molecules, it should be expected that not
only in membrane preparations but also in isolated RC
complexes containing lipid molecules and surrounded
by amphiphilic detergent molecules, electron trans-
port processes may depend on the presence of cationic
antiseptics. In this regard, the aim of this work was to
study the effect of a number of cationic antiseptics on
photosynthetic electron- and proton-transport activity
in C. sphaeroides chromatophore membranes and RC
preparations isolated from them by the electrometric
method and flash photolysis.
MATERIALS AND METHODS
Isolation and purification of chromatophores
and RC preparations from C.  sphaeroides. Chro-
matophores from the wild-type purple non-sulfur
C. sphaeroides bacteria were isolated and purified
according to the method described by Woronowicz
et al. [14], with minor modifications. In brief, cells
were collected and washed in 25 mM Hepes buf-
fer (pH 7.5) and disrupted using a French press at
12,000 psi. After centrifugation of the suspension
for 20 min at 4°C and 14,000g, the supernatant was
loaded onto a 5-35% (w/w) sucrose gradient prepared
in 25 mM Hepes buffer (pH 7.5) over a 60% sucrose
cushion and centrifuged in a VTi 50 vertical rotor for
2h at 140,000g. The bottom (third from the top) band
containing chromatophores was collected, dialyzed
twice against 25  mM  Hepes buffer (pH  7.5) for 2  h
and concentrated. The BChl concentration in the chro-
matophore suspension was determined as described
previously [15].
During RC isolation, the chromatophores were
incubated for 30 min at 4°C in 10 mM sodium phos-
phate buffer (pH 7.0) containing 0.5% lauryldimethyl-
amine oxide (LDAO) detergent. The membrane frag-
ments were then centrifuged for 90 min at 4°C and
144,000g. The RC fraction contained in the supernatant
LUKASHEV et al.884
BIOCHEMISTRY (Moscow) Vol. 90 No. 7 2025
was separated by chromatography on a hydroxyap-
atite column, as described by Zakharova et al. [16].
The applied method made it possible to obtain RC
preparations that had retained both quinone accep-
tors within their structure.
Electrometric method. Ag/AgCl electrodes im-
mersed in a Teflon cuvette were used to measure the
transmembrane electric potential difference (Δψ) on
chromatophores adsorbed on the surface of a collodion
film impregnated with a phospholipid (type IIS phos-
phatylcholine, Sigma-Aldrich, USA) in decane [17, 18].
The output voltage was connected through an op-
erational amplifier (3554BM, Burr Brown, USA) to a
GaGe CS8012 analog-to-digital converter and then to
a computer. The method allows direct measurements
of undistorted electrical signals with a time resolution
of ~200 ns. Each measurement was repeated at least
3 times. The error range of the signals was ~3%. All
measurements were performed at 22  ±  1°C. Second
harmonic laser flashes of a Nd:YAG laser (532 nm;
12 ns half-width; 20 mJ pulse energy; Quantel, Les
Ulis, France) were used for light activation.
To restore the function of the loosely bound sec-
ondary quinone acceptor Q
B
and the pool of membrane
ubiquinones in chromatophores, CoQ
10
(20 mg/ml) was
added to the lipid solution for impregnating the col-
lodion film.
Flash photolysis. Light-induced absorption chang-
es in the suspension of chromatophores and RCs were
recorded using the flash photolysis setup described
earlier [4]. In the chromatophores, photoelectric re-
sponses were recorded by measuring light-induced ab-
sorption changes (electrochromic shift of carotenoid
absorption bands) at 523 nm and the redox state of
P
870
at 790nm. An aliquot of concentrated chromato-
phores was diluted for experiments in 25 mM Hepes
buffer (pH 7.5) to a final volume of 1 ml and a final
concentration of BChl of ~30 μM. The measurement
medium contained 25 mM Hepes buffer (pH 7.5),
2 mM potassium ferrocyanide and 50 μM N,N,N′N′-
tetramethyl-p-phenylenediamine (TMPD).
In experiments with RCs in 10 mM Hepes buffer
(pH 7.5), the BChl concentration was ~1.5 μM. In this
case, exogenous cofactors were not added. Photoin-
duced absorption changes in the RC suspension
were recorded in the visible spectrum range, 400-
650  nm, with a step of 10  nm, and in the IR range at
wavelengths of 790 and 865  nm. A 1  cm
3
sample in a
10×10 mm glass cuvette was placed in a thermostat-
ted qpod-2e holder (Quantum Northwest, USA) with
a set temperature of 21°C. An Nd:YAG laser (532 nm;
7ns half-width, 10mJ pulse energy, Lotis-TII, Belarus-
Japan) was used for pulsed illumination. The kinetics
of absorption changes per flash were analyzed in the
time range from 1μs to 1 s. To improve the signal-to-
noise ratio, 50 to 100 single signals were accumulated
and averaged. The time interval between flashes was
chosen to ensure complete recovery of P
870
+
in the
darkness; it was 1.5  s for chromatophores and 5  s
for RCs. Kinetic data analysis was performed using
Origin 9.1 (OriginalLab Corp., USA) or Mathematica 8
(Wolfram Research Inc., USA) software. Absorption
spectra were recorded on a modified Hitachi-557 spec-
trophotometer (Hitachi Ltd., Japan).
Antiseptic preparations. The following ready-
made pharmaceutical preparations were used in the
studies: chlorhexidine bidigluconate 20%, picloxydine
dihydrochloride 0.05% (Vitabact), miramistin 0.01%.
The source of octenidine was the commercial prepa-
ration “Octenisept” (Schulke & Mayr, Germany), con-
taining 0.1% octenidine dihydrochloride and 2% phe-
noxyethanol. Preliminary experiments showed that
phenoxyethanol, a component of the Octenisept prepa-
ration, did not by itself affect the spectral properties
and the studied parameters of the analyzed samples
in equimolar concentrations.
RESULTS AND DISCUSSION
The cationic antiseptics used in the study had
similar effects on the spectral characteristics and the
studied functional characteristics of photosynthetic
membranes and RCs isolated from them. The mag-
nitude of these effects decreased in the series: mi-
ramistin – octenidine – chlorhexidine – picloxydine.
At the same time, chlorhexidine and picloxydine had
a significantly less pronounced effect compared to
miramistin and octenidine. Therefore, the discovered
effects are further illustrated using octenidine and
miramistin as an example.
Light-induced vector charge transfer (electron
and proton) in bacterial membrane vesicles (chro-
matophores) results in the formation of Δψ on the
chromatophore membrane [17-19]. The electrometric
method used in this study allows to reveal both the
kinetics and dielectrically weighted distances for vec-
tor (electrogenic) charge transfer reactions within RC
protein complexes [20, 21]. Using this method, elec-
trogenic reactions such as electron transfer from P
870
to Q
A
, re-reduction of P
870
+
from cytochrome c
2
, and
protonation of the doubly reduced quinone acceptor
Q
B
were previously shown in C. sphaeroides chro-
matophores [17, 18].
A photoelectric signal consists of an unresolved
fast phase of Δψ generation (resolution time of the
measuring system is ~ 200 ns), which is caused by
charge separation between P
870
and Q
A
, followed by
Δψ dissipation. Since the primary and the secondary
quinone electron acceptors are located parallel to the
membrane plane, the stage of electron transfer from
Q
A
to Q
B
is not coupled with the formation of Δψ,
ANTISEPTICS BLOCK Δψ GENERATION 885
BIOCHEMISTRY (Moscow) Vol. 90 No. 7 2025
Fig. 1. Photoelectric responses induced by the first (curves1) and second (curves2) light flashes in the presence of 100μM
octenidine (lower curves) and 100 μM miramistin (upper curves), respectively. Arrows indicate the moment of the laser
flash. The incubation medium contains 25 mM Hepes buffer (pH 7.5), 2 mM potassium ferrocyanide, and 50 μM TMPD.
20 mg of ubiquinone Q
10
was added to 1 ml of the phospholipid solution in decane to impregnate the collodion film.
The inset shows the electrical responses of C. sphaeroides chromatophores adsorbed on the surface of a collodion film
impregnated with a phospholipid solution in the absence of antiseptics induced by the first (curve1) and second (curve 2)
laser flashes. The subtraction of curve 2 from curve 1 is marked as 2-1. The time interval between the first and second
flashes is 1 s here and below.
i.e., it is non-electrogenic. In early studies [17,  18],
it was shown that the association of chromatophores
with a collodion film impregnated with phospholipids
in decane leads to the extraction of loosely bound sec-
ondary quinone Q
B
and a pool of ubiquinones (UQ).
Indeed, in the absence of exogenous electron donors
and acceptors, the kinetics of Δψ decay caused by the
reverse electron transfer reaction between Q
A
and
P
870
+
is almost fully completed within 100 ms. In this
case, the Δψ signal decay is approximated fairly well
by a single exponential with τ ~  66  ms (not shown).
It should be noted that the redox conditions in the
medium in the presence of 50 μM TMPD and 2 mM
potassium ferrocyanide (the redox potential of the me-
dium is about +320 mV) allow the detection of slow
electrogenic stages caused by vector charge transfer
involving both RC and the cytochromebc
1
complex in
chromatophores [17,  18]. As can be seen on the inset
to Fig. 1, in response to the second light flash, an ad-
ditional electrogenic phase appears in the kinetics of
the photoelectric response with a rise time of ~190  μs
(~14% of the amplitude of the fast phase, see the dif-
ference between the 2nd and 1st flashes). This submil-
lisecond rise phase is inhibited by o-phenanthroline,
which displaces the loosely bound secondary quinone
acceptor Q
B
from the binding site in the RC protein
(not shown). The dissipation time of the photopoten-
tial in the darkness under these conditions is ~500-
600 ms and reflects passive membrane discharging.
The main part of Fig. 1 shows the kinetic curves
of photopotential generation in chromatophores in the
presence of 100 μM cationic antiseptics. At a concen-
tration of 50 μM, both antiseptics had a weak effect
on the additional submillisecond electrogenic phase
in response to the second flash of light (not shown),
but octenidine completely removed it already at a
concentration of 100μM, while miramistin was much
less effective. It should also be noted that while the
photoresponse decay time was greater than 0.5 s in
the control sample (insert to Fig. 1), in the presence
of antiseptics, especially octenidine, the decay kinet-
ics became faster (<12 ms) (Fig. 1). This is probably
due to the disordering effect of the antiseptic on both
the RC protein and the chromatophore membrane, re-
sulting in an increase in passive ionic conductivity of
the chromatophore membrane.
In parallel experiments, we investigated pho-
toinduced absorption changes in a chromatophore
suspension using flash photolysis, choosing a wave-
length of 523  nm to monitor the carotenoid shift and
a wavelength of 790  nm to monitor P
870
redox trans-
formations. It is important to note that in bacterial
photosynthetic chromatophores of C. sphaeroides,
measurements of the electrochromic shift at 523 nm
in response to single light flashes allow real-time de-
tection of generation and dissipation of the electri-
cal component of both the local and transmembrane
fields (Δψ and ΔμH
+
) [22-24]. Its formation is due to
LUKASHEV et al.886
BIOCHEMISTRY (Moscow) Vol. 90 No. 7 2025
Fig. 2. Kinetic curves of the absorption changes at 523 nm (curves 1 and 2) and 790 nm (curves 3 and 4) recorded by
flash photolysis in C. sphaeroides chromatophore preparations in the absence (control, 1 and 3) and in the presence of
100μM octenidine (2 and4). The curves were normalized to the maximum amplitude of absorption changes in the control.
The dots represent the experimental values; the solid line is an approximation as the sum of exponentials (details given in
the text). The medium was 25 mM Hepes buffer, pH 7.5, 50 μM TMPD, and 2mM potassium ferrocyanide.
the generation of Δψ as a result of the functioning
of both the RC and the cytochromebc
1
complex, and
the decline in the photoelectric response reflects ion
fluxes across the chromatophore membrane, includ-
ing the proton current through the F
O
-ATP synthase
channel [25] and the passive diffusion of ions across
the phospholipid bilayer[24].
It should be noted that just as in the experiments
on recording the Δψ generation using the electromet-
ric method, 50  μM TMPD and 2  mM potassium ferro-
cyanide were also added to the medium for absorp-
tion measurements.
The parameters of the approximation of the ki-
netic curves of the carotenoid shift (Fig. 2, curves 1
and2) are given in Table1. The unresolved fast phase
(shorter than 0.1μs), reflecting the formation of a local
electric field during charge separation between P
870
and Q
A
in the control comprises ~60% of the total am-
plitude. The remaining 40% can be represented by two
phases with half-times of ~20 μs and ~2.4 ms, which,
in our opinion, are associated with the formation of
the transmembrane field. The decline in carotenoid
absorption changes occurs over tens to hundreds of
milliseconds with characteristic times of about 50 and
300 ms and an amplitude ratio of 3 :  7. When octeni-
dine is added at a concentration of 100 μM, the total
signal amplitude drops by about 2.5times, and signif-
icant changes occur in the kinetics of both its forma-
tion and decay. The fast phase of formation (<0.1 μs)
dominates, accounting for more than 80%, and the
microsecond phase (~20 μs) completely disappears.
A small-amplitude phase with the length of the order
of several milliseconds remains, the nature of which
is not entirely clear. And while the dark decay kinetics
at 523nm was much slower than the recovery of P
870
+
in the control sample, in the presence of octenidine
the dissipation of the carotenoid shift accelerated, and
these events occurred in the same time range.
Changes in P
870
absorption depend weakly on
the presence of octenidine in the medium. Both the
amplitude of P
870
photooxidation and the kinetics of
dark reduction of P
870
+
remain practically unchanged
(Fig. 2, curves 3 and 4). Since the primary photooxi-
dation of P
870
occurs on a subpicosecond time scale,
the instrumental capabilities allowed us to record only
the slower processes of dark reduction of P
870
+
on a
micro-millisecond time scale.
In Table 2 we present the results of fitting the
kinetics at 790 nm by a sum of 4exponentials.
The following assumptions can be made about
the nature of individual phases of P
870
+
reduction af-
ter the activating flash. Since the medium contains
reduced TMPD and some preserved amount of cyto-
chromec
2
, it is possible that phasesτ
1
and τ
2
, lasting
about 50-500  μs, reflect electron transfer from cyto-
chromec
2
, and the next two millisecond-range phases,
τ
2
and τ
3
, are associated with the reduction of P
870
+
by the redox mediator TMPD. It is important that the
amplitude of changes in P
870
absorption after the ad-
dition of octenidine remains constant and the kinetics
ANTISEPTICS BLOCK Δψ GENERATION 887
BIOCHEMISTRY (Moscow) Vol. 90 No. 7 2025
Table 1. The parameters (τ and A,%) of the multiexponential approximation of the kinetics of the photoinduced
shift of carotenoid absorption band at 523 nm
Parameters
Formation Dissipation
τ
1
(A
1
, %) τ
2
(A
2
, %) τ
3
(A
3
, %) τ
4
(A
4
, %) τ
5
(A
5
, %)
Control < 0.1 μs (~60) 20 μs (~16) 2.4 ms (~24) 52 ms (~30) 310 ms (~70)
+ 100 μM octenidine < 0.1 μs (~83) 3.1 ms (~17) 18 ms (~50) 117 ms (~50)
Table 2. The parameters (τ and A,%) of the multiexponential approximation of the kinetics of dark reduction
of P
870
+
at 790 nm
Parameters τ
1
(A
1
, %) τ
2
(A
2
, %) τ
3
(A
3
, %) τ
4
(A
4
, %)
Control 50 μs (~15) 0.5 ms (~15) 14 ms (~46) 79 ms (~24)
+ 100 μM octenidine 50 μs (~20) 0.5 ms (~17) 12 ms (~36) 74 ms (~27)
of dark reduction of P
870
+
changes insignificantly,
while the carotenoid shift decreases in amplitude, the
microsecond phase of its generation disappears from
the kinetics, and the dark decline accelerates.
Flash photolysis data obtained on chromato-
phores showed that octenidine does not affect the
primary charge separation between P
870
and quinone
acceptors, but disrupts transmembrane electric field
generation. Thus, these observations confirm the
conclusion drawn from the experiments with direct
measurements of electrogenesis in chromatophores.
However, the mechanism of this inhibitory effect in
the experiments on chromatophores could not be
established, so we studied the action of antiseptics
on preparations of RCs isolated from C. sphaeroides
chromatophores, which are a convenient object for
assessing the efficiency of the functioning of quinone
acceptors Q
A
and Q
B
. In the absence of an electron
donor in the medium, the kinetics of dark reduction
of P
870
+
after a flash reflects the degree of electron
occupancy of the primary and secondary acceptors.
In RC preparations with two quinone acceptors, Q
A
and Q
B
, after an activating flash of light, a slow recov-
ery due to dark recombination of P
870
+
Q
B
is observed
Fig. 3. Kinetic curves of dark decay of absorption changes (normalized by amplitude and expressed as a positive value) in a
suspension of C. sphaeroides RCs, recorded in the IR (790 and 865nm) and visible (430, 550, and 600nm) spectral regions.
LUKASHEV et al.888
BIOCHEMISTRY (Moscow) Vol. 90 No. 7 2025
Fig. 4. Kinetic curves of dark decay of absorption changes for a C.sphaeroides RC suspension recorded at different wave-
lengths. a)790nm, curves 1 and2– control without and in the presence of 5mM o-phenanthroline, respectively, curves3
and4 – after adding 150 μM miramistin to these samples; b-d)430, 460, and 550nm, respectively; curves: 1) in the pres-
ence of 150 μM miramistin, 2) normalized kinetic curves at 790 nm in the presence of 150 μM miramistin, 3) differential
curves “2 minus 1”. An approximation of the differential curve by a sum of three exponentials is also shown in panel c
(description in the text). d) curves 4 and 5: the kinetics at 550 nm in the presence of 5 mM o-phenanthroline in the con-
trol (4) and after the addition of 150 μM miramistin(5).
with a characteristic half-time of about 1 s (the rate
of direct electron transfer from Q
A
to Q
B
is 3 orders
of magnitude higher than that of the electron return
to P
870
+
, therefore, all electrons that hit the primary
quinone will then go to the secondary). And in prepa-
rations where the direct transfer is blocked in some
RCs, the recovery of P
870
+
will occur from Q
A
with a
characteristic time of about 0.1s. Since the RC prepa-
rations used in this work contained both quinone ac-
ceptors and there was no exogenous electron donor,
after a flash of light we observed P
870
+
recovery from
the secondary acceptor Q
B
with a characteristic time
of ~1 s. The kinetics of the dark decay of absorption
changes in the visible spectrum (400-650  nm) and
near IR range (700-900nm) were almost identical. The
characteristic curves for a number of wavelengths are
shown in Fig. 3.
However, when antiseptics are added, the kinetic
curves begin to diverge. While in the IR region, only
a slight acceleration of the decay kinetics is observed
for absorption changes reflecting the transformations
of the P
870
dimer, in the visible region of the spectrum
the discrepancies are more significant (Fig. 4).
Fig. 4a demonstrates the kinetics of absorption
changes at 790 nm in the control (curve 1, τ  ≈  1.1  s)
and in the presence of 5mM o-phenatroline (curve2,
τ  ≈  85  ms). It also shows the kinetic curves for
these samples in the presence of 150  μM miramistin
(curves 3 and 4). It should be emphasized that even
at very high concentrations of miramistin or octeni-
dine (400μM), the reduction in recovery time was no
more than 10% of this value in the control. In other
words, the effect of antiseptics is fundamentally dif-
ferent from the action of o-phenanthroline, which is
well known to replace the secondary acceptor at the
site of its localization in moderate concentrations, and
even displace the primary quinone in high concentra-
tions[26]. It should also be noted that in the presence
of o-phenanthroline, the kinetics of photoinduced ab-
sorption changes in the visible and IR regions coin-
cided for all the studied concentrations of antiseptics.
In the RC preparations without o-phenanthroline,
negative changes appeared in the kinetics of photoin-
duced absorption changes in the 400-650  nm region
a few milliseconds after the activating flash, which
distorted the “normal” form of the kinetics, if we con-
sider that the kinetics of transformations at 790 nm
adequately reflects the charge separation in RCs be-
tween P
870
+
and Q
B
with the formation of a local elec-
tric field and the subsequent charge recombination
(Fig. 4, b-d). The strongest effect was observed in the
presence of miramistin (then, in the descending or-
der – octenidine, chlorhexidine, picloxydine), so we
studied the effect of this preparation in most detail.
ANTISEPTICS BLOCK Δψ GENERATION 889
BIOCHEMISTRY (Moscow) Vol. 90 No. 7 2025
Fig. 5. Single-flash-induced differential absorption “light minus dark” spectra in a suspension of C.sphaeroides RCs. a)Bythe
amplitude of absorption changes 1 ms after the flash (1) and by the amplitude of negative absorption changes appearing
with a delay(2), shown, in particular, in Fig. 4, b-d by curves 3; b) the same (2) dependence on an enlarged scale.
Let us recall that the recorded absorption changes in
the visible spectrum region reflect a number of pro-
cesses: oxidation of the BChl dimer, formation of the
semiquinone radical, as well as electrochromic shifts
of the absorption bands of carotenoids and BPh.
For illustration, Fig. 4, b-d shows photoinduced
absorption changes for wavelengths of 430, 460, and
440 nm (curves 1) and absorption changes at 790  nm
normalized by amplitude, which we considered “un-
distorted” (curves 2), as well as differential kinetic
curves (curves 3). Fig. 4c shows the fitting of such
kinetics by two growth exponents with characteristic
times τ
1
≈  25.6 ms (~30%) and τ
2
≈  191.2 ms (~70%)
and one decay exponent characterized by a time
τ
3
≈  3s. The kinetic parameters differed little, but the
amplitude of the resulting curves depends significantly
on the wavelength.
Fig. 5a shows the differential absorption spec-
trum “light minus dark” in the visible part of the
spectrum (1), constructed from the signal amplitude
1 ms after the light flash until the moment of neg-
ative changes appearing, as well as the dependence
of the amplitude of the discussed negative absorption
changes on the wavelength (2). Fig. 5b presents this
dependence on an enlarged scale. We recall that in
the 400-600 nm spectral region, multiple absorption
changes are observed associated with redox transfor-
mations and electrochromic shifts of various RC com-
ponents: RC BChl (about 430 and 600 nm), BPh (about
540  nm), RC carotenoid (500-600 nm), and semiqui-
none forms of Q
A
and Q
B
acceptors (in the 450-460  nm
region) [27].
It has been previously shown that the formation of
the semiquinone anion Q
B
in the RC of Rb. sphaeroi-
des is accompanied by the appearance of a broad ab-
sorption band with a maximum at 450nm[28]. Asfol-
lows from Fig. 5b, the amplitude of the absorption
changes occurring ~200 ms after the flash reaches a
maximum of about 460 nm, which indicates a possi-
ble connection with a change in the absorption of the
semiquinone anion.
Despite long-term studies, the mechanisms of Q
B
reduction, proton binding and its migration in various
redox states are not yet fully understood [29]. It was
previously suggested that electrostatics plays a deci-
sive role in the interaction of various redox states
LUKASHEV et al.890
BIOCHEMISTRY (Moscow) Vol. 90 No. 7 2025
of Q
B
with the surrounding amino acid residues [30].
Indeed, all models of stabilization of the anionic form
of Q
B
suggest that this requires a significant rear-
rangement of charges and dipoles at the Q
B
site [31].
At the same time, it is known that in RCs from wild-
type Rb. sphaeroides bacteria, in which ubiquinone
Q
10
is located at the site of the secondary acceptor
Q
B
, the formation of its semiquinone anion form is
not accompanied by direct protonation, which is ex-
plained by the low value of its pK
a
~ 4.5 [13]. Since
the environment of Q
B
is rich in protons and polar
groups, the appearance of a negative charge on Q
B
affects the equilibrium of protons in the system of
hydrogen bonds involved in stabilizing the electron
on the acceptor. In particular, the pK of the amino
acid Glu L212 changes [32]. This amino acid, linked
through a network of hydrogen bonds with other
protonated amino acids and water molecules in the
RC structure, plays a key role in donating the first
proton in the process of forming hydroquinone Q
B
H
2
during two-electron reduction of the secondary accep-
tor[28]. It is proposed that in response to the electron
transfer to Q
B
, changes occur in the hydrogen bond
network formed by the surrounding water molecules
and the polar groups of the amino acids. Calculations
show that even small changes in the orientation of
these molecular groups can induce shifts in their pK,
ensuring the directional proton transfer[33].
The protonation of Q
B
in RC preparations was
successfully recorded in an experiment when ubiqui-
noneQ
10
was replaced with rhodoquinone, for which
the pK
a
value was much higher (about 7.3) [13].
At acidic pH values, a decrease in the amplitude of
the photoinduced absorption band of the semiquinone
anion Q
B
was observed. As noted in the Introduction,
in contrast to purified RC preparations, in chromato-
phores, this stage of protonation of the secondary
acceptor after its one-electron reduction was experi-
mentally observed [12]. This result was attributed to
an increase in the pK
a
of the secondary quinone Q
10
by more than 3units due to RC immersion in the lipid
bilayer of the chromatophore membranes.
RC protein relaxation during electron transfer
to quinone acceptors is sensitive to protein-bound
lipids. It has been shown that electrostatic changes
on the protein surface or in the hydrogen bond net-
work surrounding Q
B
can lead to changes in pK
a
of
amino acids near Q
B
and the pK of the semiquinone
Q
B
itself [34]. It can be assumed that the absorption
changes we detected reflect the partial disappearance
of the absorption band of the semiquinone anion Q
B
and the appearance of the absorption band of the
electroneutral form Q
B
H due to the displacement of
protons in the immediate environment or upon direct
binding with a proton in the medium[12,13]. The ob-
served effect of amphiphilic cationic antiseptics in RC
preparations could be associated with their influence
on the pK
a
value of the secondary quinone, as it oc-
curs in the membrane lipid matrix of chromatophores.
The rate of proton binding in our experiments was
quite low; this process takes 100-200ms. At the same
time, the calculations performed for Q
B
protonation
with rhodoquinone give a value of several microsec-
onds[13], since this process must precede the transfer
of the second electron from Q
A
, which occurs on a
microsecond time scale. Apparently, the increase in
pK
a
in our case is not very large, and therefore, when
the measurements were performed with a medium pH
of 7.5, the rate constant of the direct protonation re-
action is close to the deprotonation constant. Never-
theless, the results obtained indicate that cationic an-
tiseptics (mainly miramistin and octenidine) promote
the direct protonation of Q
B
with the formation of a
neutral complex Q
B
H. It should be noted that in the
structure of the resulting “negative” absorption chang-
es, a certain constant value is present for the entire
spectral range of 400-650 nm, which clearly does not
belong to the semiquinone anion spectrum (Fig. 5b).
Apparently, neutralization of the charge on the sec-
ondary quinone partially reduces the local electric
field, which reduces the magnitude of the electrochro-
mic shifts of carotenoids and BPh, making a signifi-
cant contribution to the absorption changes in this
wavelength range. Indeed, it has been shown that an
increase in the yield of the neutral form of semiqui-
none Q
B
H correlates with a decrease in the amplitude
of the electrochromic shift of the BPh absorption band
at 760 nm [12].
It should be noted that the analyzed cationic
antiseptics, according to various data, exhibit a de-
tergent-like effect in high concentrations [35, 36].
Moreover, in a number of studies, the ability of these
compounds to disrupt the integrity, i.e. barrier prop-
erties of membranes is considered the basis of their
antimicrobial action[37, 38]. Considering the acceler-
ation of the decline in the photoelectric response of
chromatophores to single light flashes in the presence
of 100 μM octenidine which indicates a marked in-
crease in the passive ionic conductivity of the mem-
brane (Fig. 1), as well as a sharp drop in the ampli-
tude of the carotenoid shift under similar conditions
(Fig.3), the possibility of a significant contribution of
the detergent-like effect to the observed effects of cat-
ionic antiseptics cannot be excluded.
CONCLUSION
The new experimental data presented in this
study complement the general picture of the effects
of cationic antiseptics on biomembranes. The present-
ed results indicate that these agents can affect the
ANTISEPTICS BLOCK Δψ GENERATION 891
BIOCHEMISTRY (Moscow) Vol. 90 No. 7 2025
cyclic electron transfer in bacterial chromatophores,
reducing the generation of the transmembrane pro-
ton gradient on the photosynthetic membrane. Ex-
periments on RC preparations showed the effect of
cationic antiseptics on local proton equilibria respon-
sible for stabilization of electrons on the secondary
quinone acceptor in protein-pigment complexes. The
discovered differences in the action of octenidine and
miramistin on membrane preparations and prepara-
tions of isolated RCs are apparently due to the specific
physico-chemical properties of these antiseptics– their
amphiphilicity, charge characteristics, and general mo-
lecular structure. As a result, octenidine has a great-
er effect on membrane preparations, influencing their
functional activity. Miramistin modifies protein–pig-
ment complexes isolated from membranes more ef-
fectively, interacting with the surface of the complex
and, possibly, partially penetrating the surface struc-
ture of the protein.
The main conclusion from the obtained results
is that cationic antiseptics, which are increasingly
entering the environment, disrupt the functioning of
the quinone acceptor side of the electron transport
chain, reducing the energization of the coupling pho-
tosynthetic membrane necessary for ATP synthesis.
Thus, they can have a negative impact on the global
processes of photosynthetic utilization of light energy.
Abbreviations. Δψ, transmembrane electrical
potential difference; BPh, bacteriopheophytin; BChl,
bacteriochlorophyll; P
870
, special pair of bacteriochlo-
rophyll, the primary donor of RC; Q
A
and Q
B
, the
primary and the secondary quinone acceptors, re-
spectively; RC, photosynthetic reaction center; TMPD,
N,N,N′N′-tetramethyl-p-phenylenediamine.
Contributions. E. P. Lukashev, M. D. Mamedov,
P. P. Knox, V. Z. Paschenko– setting the objectives, dis-
cussion of the results of the study, writing the text of
the paper; E. P. Lukashev, M. D. Mamedov, L. A. Vitukh-
novskaya, A. M. Mamedova– conducting experiments,
processing results; L. A. Vitukhnovskaya, A. M. Mame-
dova– preparing the samples for the study.
Funding. The study was carried out within the
framework of the scientific project of the State Assign-
ment of Moscow State University No.121032500058-7.
Ethics approval and consent to participate.
This work does not contain any studies involving hu-
man and animal subjects.
Conflict of interest. The authors of this work de-
clare that they have no conflicts of interest.
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