The effect of molecular structure of chlorin photosensitizers on photo-bleaching of 1,3-diphenylisobenzofuran—the possible evidence of iodine reactive species formation

Andrey Kustov; Philipp Morshnev; Natal’ya Kukushkina; Mikhail Krestyaninov; Nataliya Smirnova; Dmitry Berezin; Galina Kokurina; Dmitry Belykh

doi:10.5802/crchim.158

Communication préliminaire

The effect of molecular structure of chlorin photosensitizers on photo-bleaching of 1,3-diphenylisobenzofuran—the possible evidence of iodine reactive species formation

Andrey Kustov ^1,² ; Philipp Morshnev ^1,² ; Natal’ya Kukushkina ^1,² ; Mikhail Krestyaninov ¹ ; Nataliya Smirnova ¹ ; Dmitry Berezin ² ; Galina Kokurina ² ; Dmitry Belykh ³

¹ G.A. Krestov Institute of Solution Chemistry, Russian Academy of Sciences, Academicheskaya str., 1, Ivanovo, 153045, Russia
² Ivanovo State University of Chemistry and Technology, Research Institute of Macroheterocycles, Sheremetevsky av., 7, Ivanovo, 153000, Russia
³ Institute of Chemistry of Komi Science Centre of the Ural Branch of Russian Academy of Sciences, Pervomaiskaya str., 48, Syktyvkar, 167000, Russia

Comptes Rendus. Chimie, Volume 25 (2022), pp. 97-102.

Résumé

In this short communication, we focus on the ability of chlorin e $_{6}$ photosensitizers (PSs) with one, two or three cationic groups to generate singlet oxygen species ( $^{1}$ O $_{2}$ ) in an apolar model medium, viz. 1-octanol (OctOH). The quantum yield of $^{1}$ O $_{2}$ ( $Φ_{Δ}$ ) is determined indirectly by the chemical method for seven synthesized PSs using 1,3-diphenylisobenzofuran (DPBF) as a singlet oxygen trap. The $Φ_{Δ}$ values of four PSs with one or two cationic groups occupying opposite positions in the macrocycle are equal to 0.6, which is nearly identical to the values obtained by the time-resolved fluorescence spectroscopy method. In contrast, three PSs containing a 3(1),3(2)-bis-(N,N,N-trimethylaminomethylvinyl) iodide fragment with two adjacent cationic groups have an abnormally high quantum yield reaching 0.8. It is apparent that this phenomenon results from faster trap oxidation induced by radical reactions leading to molecular iodine formation.

Supplementary Materials:
Supplementary material for this article is supplied as a separate file:

crchim-158-suppl.pdf

Métadonnées

Reçu le : 2021-08-10
Révisé le : 2021-11-20
Accepté le : 2022-02-15
Publié le : 2022-03-16

DOI : 10.5802/crchim.158

Mots clés : Antimicrobial photodynamic therapy, Cationic chlorin photosensitizer, Singlet oxygen formation, 1,3-diphenylisobenzofuran, Reactive iodine species

Affiliations des auteurs :

Andrey Kustov ^{1, 2} ; Philipp Morshnev ^{1, 2} ; Natal’ya Kukushkina ^{1, 2} ; Mikhail Krestyaninov ¹ ; Nataliya Smirnova ¹ ; Dmitry Berezin ² ; Galina Kokurina ² ; Dmitry Belykh ³

Licence :

CC-BY 4.0

Droits d'auteur : Les auteurs conservent leurs droits

@article{CRCHIM_2022__25_G1_97_0,
     author = {Andrey Kustov and Philipp Morshnev and Natal{\textquoteright}ya Kukushkina and Mikhail Krestyaninov and Nataliya Smirnova and Dmitry Berezin and Galina Kokurina and Dmitry Belykh},
     title = {The effect of molecular structure of chlorin photosensitizers on photo-bleaching of 1,3-diphenylisobenzofuran{\textemdash}the possible evidence of iodine reactive species formation},
     journal = {Comptes Rendus. Chimie},
     pages = {97--102},
     publisher = {Acad\'emie des sciences, Paris},
     volume = {25},
     year = {2022},
     doi = {10.5802/crchim.158},
     language = {en},
}

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AU  - Dmitry Berezin
AU  - Galina Kokurina
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%0 Journal Article
%A Andrey Kustov
%A Philipp Morshnev
%A Natal’ya Kukushkina
%A Mikhail Krestyaninov
%A Nataliya Smirnova
%A Dmitry Berezin
%A Galina Kokurina
%A Dmitry Belykh
%T The effect of molecular structure of chlorin photosensitizers on photo-bleaching of 1,3-diphenylisobenzofuran—the possible evidence of iodine reactive species formation
%J Comptes Rendus. Chimie
%D 2022
%P 97-102
%V 25
%I Académie des sciences, Paris
%R 10.5802/crchim.158
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%F CRCHIM_2022__25_G1_97_0

Andrey Kustov; Philipp Morshnev; Natal’ya Kukushkina; Mikhail Krestyaninov; Nataliya Smirnova; Dmitry Berezin; Galina Kokurina; Dmitry Belykh. The effect of molecular structure of chlorin photosensitizers on photo-bleaching of 1,3-diphenylisobenzofuran—the possible evidence of iodine reactive species formation. Comptes Rendus. Chimie, Volume 25 (2022), pp. 97-102. doi : 10.5802/crchim.158. https://comptes-rendus.academie-sciences.fr/chimie/articles/10.5802/crchim.158/

Version originale du texte intégral (Proposez une traduction )

1. Introduction

Antimicrobial photodynamic therapy (APDT) with natural or synthetic photosensitizers seems to be a very promising alternative or an important supplement to classical antibiotic therapy of many localized infections [1, 2, 3, 4, 5]. This bright technique consists of three crucial components: a photosensitizer, molecular oxygen and visible light taken together and leads to the formation of reactive oxygen species (ROS) such as singlet oxygen ¹O₂ (Type II photochemical mechanism) or various radical forms (HO^∙, O $_{2}^{∙ -}$ ) and H₂O₂ (Type I photochemical mechanism) [6, 7, 8]. These ROS inflict a fatal damage towards bacterial cells and provide the excellent killing effect, if the PS molecule is able to penetrate a bacterial cell [1, 2, 3]. However, neutral and anionic PSs, which are currently in use for treating various tumors, have low affinity towards the outer lipopolysaccharide membrane of Gram-negative bacteria and can efficiently kill these pathogens under irradiation [2, 3]. In contrast, cationic PSs containing several charged groups or bound to an appropriate carrier provide efficient inactivation of Gram-negative pathogens [1, 2, 3, 9, 10]. Another important way to improve the ability of PSs to kill these microbes is to add non-toxic inorganic salts such as azides, iodides or thiocyanides to a PS formulation [4, 5]. In particular, the addition of various KI amounts to a 10 μM “Photofrin” (water-soluble hematoporphyrin) solution provides the concentration-dependent killing curve for five Gram-negative bacteria [4]. Similar results were reported for several cationic porphyrins but not for their neutral derivatives [5]. This “extra killing effect” is recognized to be dependent of the PS structure [4, 5] and results from several parallel processes initiated by the singlet oxygen reaction with an iodide ion in water and peroxyiodide formation [4, 5]. The latter is unstable and may suffer further decomposition via two different pathways that depend on the degree of PS binding to a microbial cell [5]. The first of them involves the formation of free iodine (I₂/I $_{3}^{-}$ ) and hydrogen peroxide. The second pathway leads to the formation of reactive iodine species (I $_{2}^{∙ -}$ ) with a short diffusion distance. In principle, both processes provide the efficient killing of Gram-negative bacteria but in a different way (see [4, 5] and references therein).

With these results in mind, we studied photo-bleaching of the well-established ¹O₂ trap, viz. 1,3-diphenylisobenzofuran, using several chlorin PSs with one, two or three iodide ions in OctOH as an appropriate lipid-like environment model [11]. Then, the respective photo-bleaching rates were used to compute the 𝛷_𝛥 values and to compare them with the quantities obtained by direct spectroscopic measurements [9].

2. Experimental section

2.1. Reagents

1-Octanol (Panreac, >98%) was dried with 4 Å molecular sieves and distilled under reduced pressure at 353 K. Karl Fisher titration showed that the final water content in OctOH was less than 0.02 wt%. 1,3-diphenylisobenzofuran (DPBF) (Sigma-Aldich, >99%) and crystal iodine (Reachem, >99%) were used as supplied.

PSs shown in Figure 1 were synthesized, purified and identified in our laboratory with ¹H NMR, MS- and UV-Vis spectra. ¹H NMR spectra were registered with the Bruker Avance II spectrometer (300 MHz) or Bruker Avance III spectrometer (500 MHz). CDCl₃ or DMSO d₆ were used as appropriate solvents and TMS was applied as the internal standard for the ¹H NMR measurements. MS-spectra were obtained with the Thermo finnigan LCQ Flut (ESI) instrument and/or MALDI FAB MS-spectrometer Shimadzu AXIMA Confidence with α-cyano-4-hydroxycinnamic acid (CHCA) and 2,5-dihydroxybenzoic acid (DHB) as a matrix. UV-Vis spectra were obtained at 293 K with the Drawell D8 spectrophotometer in a highly diluted pigment solution ( ∼5–8 μmol).

A detailed description of the synthetic and identification procedures of compounds 1, 2, 5–8 was given earlier [9, 10, 12]. For newly synthesized compounds 3, 4 this information can be found in the Supplementary material file.

Figure 1.
Molecular structures of the PSs studied: (a) 13(1)-N-(2-N′N′N′-trimethylammonioethyl iodide)amide chlorin e₆ 15(2),17(3)-dimethyl ester 1, (b) 3(2)-(N,N,N-trimethylaminomethyl iodide) chlorin e₆ 13(1)-N-methylamide 15(2),17(3)-dimethyl ester 2; (c) chlorin e₆ 13(1)-(4′-N,N-dimethylpiperazinyl iodide)amide 15(2),17(3)-dimethyl ester 3; (d) 3(2)-(N,N,N-trimethylaminomethyl iodide) chlorin e₆ 13(1)-N′-(2-N′′,N′′,N′′-trimethylammonioethyl iodide)amide 15(2),17(3)-dimethyl ester 4; (e) 3(1),3(2)-bis-(N,N,N-trimethylaminomethyl iodide) chlorin e₆ 13(1)-N-methylamide 15(2),17(3)-dimethyl ester 5; (f) 3(1),3(2)-bis-(N,N,N-trimethylaminomethyl iodide) chlorin e₆ 13(1)-N-(2-myristoxyethyl)amide 15(2),17(3)-dimethyl ester 6; (g) 3(1),3(2)-bis-(N,N,N-trimethylaminomethyl iodide) chlorin e₆ 13(1)-N′-(2-N′′,N′′,N′′-trimethylammonioethyl iodide)amide 15(2),17(3)-dimethyl ester 7; (h) pheophorbide a 17(3)-methyl ester (methylpheophorbide a) 8.

PS
1	2	3	4	5	6	7	8
0.63 ± 0.05^a	0.63 ± 0.02	0.64 ± 0.04	0.60 ± 0.03	0.77 ± 0.02	0.79 ± 0.02	0.77 ± 0.05	0.49 ± 0.05
0.65 ± 0.07^b	-	-	-	0.60 ± 0.06^b		0.53 ± 0.05^b	0.47 ± 0.05^b

^aUncertainties represent a twice standard deviation. For the determination of the 𝛷_𝛥 value for compound 1 we have used compound 8 as the appropriate standard with the quantum yield equals 0.47 [9].

^bValues obtained from the direct measurements of ¹O₂ luminescence intensity at 1270 nm [9].

2.2. Determination of singlet oxygen quantum yield

The singlet oxygen quantum yield was determined by the indirect chemical method which was very similar to the technique described elsewhere [13, 14]. In brief, two quartz cuvettes with a 1 cm optical way contained 3 ml of a PS + DPBF or St + DPBF solution with the absorbance of 0.2–0.3 at the Q-band and 0.9–1.2 at 444 nm. The cuvettes were irradiated with a red light diode panel (BIC, Minsk) [9, 10]. This panel emitting between 590 and 720 nm with the maximum at 662 nm provided the light spot of 10 × 10 cm. The power density of red light was chosen to be equal to 3 mW⋅cm⁻². At this irradiance a fluence (light dose) of 0.18 J⋅cm⁻² was delivered every minute. The monocationic chlorin (see compound 1 in Figure 1) with the known 𝛷_𝛥 value equaling to 0.67 [9] was used as an appropriate standard.

DPBF degradation in both cuvettes was monitored spectrophotometrically each minute, and each irradiation session contained usually six-eight measurements. Then, the rate-of-degradation constants k_d were evaluated in terms of the first order exponential decay. All the photo-bleaching experiments were repeated from six to eight times. The 𝛷_𝛥 values were derived from the following equation:

𝛷_{𝛥 PS} = \frac{k_{d PS}}{k_{d St}} \frac{I P_{St}}{I P_{PS}} 𝛷_{𝛥 St},

(1)

where the PS and St symbols refer to the photosensitizer and the standard, respectively. The IP values were computed numerically by:

I P = \int_{𝜆_{1}}^{𝜆_{2}} I_{0} (𝜆) (1 - 1 0^{- A}) d 𝜆,

(2)

where 𝜆₁ and 𝜆₂ are the initial and the final wavelengths of the region, in which the panel and PS spectra overlap, I₀ (𝜆) is the LED panel intensity (between 590 and 720 nm) as a function of 𝜆 and A is the solution optical density. The photo-bleaching correction term was omitted because the PS concentration was constant over all the irradiation period.

3. Results and discussion

The PS molecules shown in Figure 1 in their ground state, i.e. singlet electronic state (S₀), contain two electrons with the opposite spins located in the most favorable molecular orbital [6]. Absorbance of red light at 660 nm leads to the transfer of the macrocycle to an excited singlet state (S₁). The excited PS molecule is capable of intersystem crossing and transition to the long-lived biradical triplet state (T₁) with an inverted spin of one electron [4, 6]. Then, the PS molecule in this triplet state may transfer its energy to molecular oxygen, ³O₂, which leads to the formation of a reactive singlet oxygen species, ¹O₂. This so-called Type II process is characteristic of apolar media, while in H-bonded solvents, especially water, some fraction of radical forms is detected [15].

We have recently shown [9] that in many chlorin-type PSs without metal ions in their coordination sphere, the 𝛷_𝛥 values range from 0.47 to 0.67 regardless of the macrocycle structure. Hence, the quantum yield of singlet oxygen of a chlorin photosensitizer is within 0.55 ± 0.1 in any weakly polar solvent. This finding is in agreement with chemical intuition and the available literature values [16, 17, 18, 19]. Table 1 shows that for compounds 1–4 and 8 the corresponding quantum yields agree with this estimation. It is interesting to note that the corresponding 𝛷_𝛥 values are larger for chlorin PSs (see compounds 1–4) compared to phorbin-type pigments (compound 8). Moreover, for compounds 1, 8 the indirectly obtained quantum yields are seen to be in very good agreement with the previously reported values [9].

However, compounds 5–7 demonstrate significantly higher quantum yields than what could be expected from direct measurements (see Table 1). This difference results from the higher rate of DPBF oxidation that leads to larger k_d values (see (1)). Inspection of the solute structures shown in Figure 1 indicates that all three PS molecules (see compounds 5–7) contain two or even three iodine atoms which may be responsible for the higher oxidation rate of the trap. However, compound 4 also contains two iodine atoms but has a “normal” 𝛷_𝛥 value (see Table 1). Hence, the close location of ionic groups in compounds 5–7 is much more important for the higher oxidation rate of the trap than their relative number. In fact, two cationic groups occupy opposite positions in compound 4, while they are located in the 3(1),3(2)-bis-(N,N,N-trimethylaminomethylvinyl) iodide fragment in compounds 5–7. This close location seems to be responsible for the higher oxidation rate of DPBF. Another proof comes from our comparative analysis showing that the 𝛷_𝛥 values for compounds 5 and 7 are almost identical, although the latter solute contains an additional ionic group (see Figure 1). Thus, the structure of the 3(1),3(2)-bis-(N,N,N-trimethylaminomethylvinyl) iodide fragment with two adjacent ionic groups is responsible for the interaction between iodine and singlet oxygen [5]. The intermediate of this reaction can further decompose to free iodine (I₂/I $_{3}^{-}$ ) and peroxyalcohol radicals (ROO^∙) or short-lived reactive radicals I $_{2}^{∙ -}$ according to the Scheme S1 shown in the Supplementary material file [5].

In principal, both of these processes may lead to the abnormal 𝛷_𝛥 values due to faster oxidation of the trap. However, it should be kept in mind that the “extra killing effect” mentioned above takes place in an aqueous medium, where each singlet oxygen molecule interacts with well-hydrated iodide ions [5]. However, all the cationic PSs shown in Figure 1 are weakly dissociated in apolar OctOH, and ¹O₂ molecules interact with the iodide ion bound to the cationic group of PS.

To shed more light on the trap photobleaching mechanisms in a lipid-like medium, we studied the effect of ammonium iodide addition (∼0.2 mmol/kg) to compound 5 and found that irradiation lead to an increase in the solution absorbance at 365 nm (see Figure S12 in the Supplementary material file). According to the results mentioned above (see [4, 5] and references therein), this phenomenon can be attributed to the formation of molecular iodine in the liquid phase. To check this point, we dissolved an appropriate amount of iodine and NH₄I in OctOH and found that the solution spectrum was very similar to the spectrum of compound 5 + NH₄I shown in Figure S12. It is apparent that this proves that singlet oxygen interacts with ammonium iodide, which leads to the formation of molecular iodine. We assume that a similar phenomenon occurs in a solution of PSs with a 3(1),3(2)-bis-(N,N,N-trimethylaminomethylvinyl) iodide fragment. This induces faster oxidation of DPBF, which is responsible for the abnormal 𝛷_𝛥 values.

4. Conclusions

In summary, our experimental efforts aimed to study singlet oxygen generation by cationic chlorins indicate that PSs with one or two cationic groups occupying opposite positions in the macrocycle have normal 𝛷_𝛥 values of 0.6, which is in good agreement with the results of direct measurements. However, PSs with two adjacent cationic groups have a larger quantum yield that reaches 0.8. This phenomenon results from faster trap oxidation due to radical reactions that lead to the formation of molecular iodine.

CRediT authorship contribution statement

AVK: Conceptualization, Methodology, Investigation, Writing—original draft, Review and editing, Funding acquisition. PKM: Investigation, Formal analysis. NVK: Synthesis, Investigation. MAK: Methodology, Investigation. NLS: Methodology, Investigation. DBB: Conceptualization, Writing, Review and editing, Funding acquisition. GNK: Methodology, Formal analysis. DVB: Investigation, Synthesis, Writing—review and editing, Funding acquisition.

Conflicts of interest

Authors have no conflict of interest to declare.

Acknowledgment

This work was supported by the Russian Science Foundation (project N 21-13-00398).

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