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Article

Photophysicochemical Properties and In Vitro Phototherapeutic Effects of Iodoquinoline- and Benzothiazole-Derived Unsymmetrical Squaraine Cyanine Dyes

1
Chemistry Centre of Vila Real (CQ-VR), University of Trás-os-Montes and Alto Douro, Quinta de Prados, 5001-801 Vila Real, Portugal
2
Centre for Research and Technology of Agro-Environmental and Biological Sciences (CITAB-UTAD), University of Trás-os-Montes and Alto Douro, Quinta de Prados, 5001-801 Vila Real, Portugal
3
Health Sciences Research Centre (CICS-UBI), University of Beira Interior, Av. Infante D. Henrique, 6201-001 Covilhã, Portugal
4
Centro de Química-Física Molecular (CQFM), Institute for Nanosciences and Nanotechnology (IN) and Institute of Bioengineering and Biosciences (iBB), Higher Technical Institute, University of Lisbon, Av. Rovisco Pais, 1049-001 Lisbon, Portugal
*
Authors to whom correspondence should be addressed.
Both authors can be considered first author since they contributed equally to this work.
Appl. Sci. 2019, 9(24), 5414; https://doi.org/10.3390/app9245414
Submission received: 25 November 2019 / Revised: 5 December 2019 / Accepted: 9 December 2019 / Published: 11 December 2019

Abstract

:

Featured Application

Potential application of unsymmetrical squaraine cyanine dyes as cancer photodynamic therapy photosensitizers.

Abstract

The search to replace conventional cancer treatment therapies, such as chemotherapy, radiotherapy and surgery has led over the last ten years, to a substantial effort in the development of several classes of photodynamic therapy photosensitizers with desired photophysicochemical and photobiological properties. Herein we report the synthesis of 6-iodoquinoline- and benzothiazole-based unsymmetrical squaraine cyanine dyes functionalized with amine groups located in the four-membered central ring. Their photodegradation and singlet oxygen production ability, as well as their in vitro photocytotoxicity against Caco-2 and HepG2 cell lines using a 630.8 ± 0.8 nm centered light-emitting diode system, were also investigated. All photosensitizer candidates displayed strong absorption within the tissue transparency spectral region (650–850 nm). The synthesized dyes were found to have moderate light stability. The potential of these compounds is evidenced by their cytotoxic activity against both tumor cell lines, highlighting the zwitterionic unsubstituted dye, which showed more intense photodynamic activity. Although the singlet oxygen quantum yields of these iodinated derivatives are considered low, it could be concluded that their introduction into the quinoline heterocycle was highly advantageous as it played a role in increasing selective cytotoxicity in the presence of light. Thus, the novel synthesized dyes present photophysicochemical and in vitro photobiological properties that make them excellent photosensitizer candidates for photodynamic therapy.

Graphical Abstract

1. Introduction

Since squaric acid (3,4-dihydroxy-1,2-dioxocyclobut-3-ene) was first reported in 1959 by Cohen et al. [1], and later by other studies, as a rigid structure [2] with high chemical reactivity [3], its condensation with electron-rich precursors has been extensively studied [4,5,6] aiming to find products with potential applicability in several technological and biomedical areas [7,8,9]. Among the squaric acid derivatives, it is essential to emphasize the squaraine cyanine dyes, a core of functional dyes, first reported by Treibs and Jacob [10], known for its good photochemical stability, conductivity, sharp and intense Vis/NIR absorption and high absorption coefficients [8,11,12]. These photochemical and photophysical properties encourage the study of the suitability of these core of dyes to their application as photoconductive and nonlinear optical materials [13,14], sensitizers for organic solar cells [15,16], fluorescent probes for detection of functional groups [17], toxic substances [18,19,20] or biomolecules [21,22,23], and as photodynamic therapy (PDT) photosensitizers [9,24,25].
Cancer has become one of the biggest health problems and leading causes of death worldwide as a result of a combination of several factors, such as genetic predisposition, exposure to environmental contaminants and incorrect diet [26,27]. Since conventional treatments reveal multiple side effects, such as being extremely debilitating and poorly effective in treating some types of tumors [28], substantial progress is being made in the areas of oncology, cellular and molecular biology and medicinal chemistry to improve chemotherapy and other treatments applied to cancer patients [29].
PDT is a minimally invasive therapeutic strategy with reduced side effects that involve the death of target tissue cells by the combined action of adequate light, a photoactive molecule and molecular oxygen, which results in the production of reactive oxygen species (ROS) that promote cell structural and functional failure [30,31]. This therapeutic modality has progressed over the last few years [32,33], not only to study its potential use for the treatment of cancer, but also for dermatological [34] and ophthalmic conditions [35], such as psoriasis [36,37] and age-related macular degeneration [38], respectively. Although some PDT photosensitizers are already commercially available, mostly derived from porphyrins, these light-sensitive molecules have the disadvantage of being slowly eliminated from the body, causing skin photosensitivity [8,39]. Thus, several research studies have recently reported the discovery of new compounds, such as cyanines [40], squaraines [24], chlorins [41] or phthalocyanines [42] which, by appropriate structural modifications, can ideally override the gaps of first-generation photosensitizers [43].
In this work, we report the synthesis and characterization of iodoquinoline- and benzothiazole-based unsymmetrical squaraine cyanine dyes with N-hexyl chains and the evaluation of their properties such as photostability and singlet oxygen production ability. The in vitro phototherapeutic effects of these squaraine-based photosensitizers has been evaluated on human hepatocellular carcinoma (HepG2) and human colorectal adenocarcinoma (Caco-2) cell lines by analyzing the variation of cell viability after exposure to various irradiation and incubation conditions with the synthesized dyes. This study also aimed to understand the role of the introduction of iodine atom on photophysicochemical and photobiological properties, by comparing the results obtained in this study with those recently described by us [25].

2. Materials and Methods

2.1. Chemistry

All reagents and solvents were purchased from commercial suppliers and used without further purification. Dichloromethane was dried as described in the literature [44] and used freshly distilled. 3-Hexyl-2-methylbenzothiazol-3-ium iodide (2) [45], 3,4-dibutoxy-3-cyclobuten-1,2-dione (4) [46], 3-butoxy-4-[(3-hexylbenzothiazol-2(3H)-ylidene)methyl]-cyclobut-3-en-1,2-dione (5) [47], 3-[(3-hexyl-benzothiazol-2(3H)-ylidene)methyl]-4-hydroxycyclobut-3-en-1,2-dione (6) [47], 6-iodo-1-hexyl-quinaldine (8) [48] and 6-iodo-1-hexylquinaldinium iodide (9) [49] was prepared according to the corresponding literature procedures. Reactions were monitored by thin-layer chromatography (TLC) on aluminium plates with 0.25 mm of silica gel (TLC Silicagel 60 F254, Merck, Darmstadt, Germany), which were, whenever necessary, visualized by UV detection. Purification by column chromatography was carried out on silica gel 60 (70–230 mesh) using a mixture of ethyl acetate and petroleum ether (1:1) or CH2Cl2 as eluent. Melting points (m.p.) were recorded on a hot plate binocular microscope apparatus (URA Technic, Porto, Portugal) and are uncorrected. Infrared (IR) spectra were obtained using KBr pellets with an IRAffinity-1S FTIR spectrophotometer (Shimadzu, Duisburg, Germany) using Shimadzu LabSolutions IR software; υmax in cm−1. The intensity of the band was described as s (strong), m (medium) and w (weak). Vis/NIR absorption spectra were measured on a Lambda 25 instrument (Perkin Elmer, Waltham, USA) using PerkinElmer UV WinLab Data processor and Viewer software; λmax in nm. These spectra were obtained from acetonitrile (ACN), acetone (ACT), dichloromethane (DCM), DMEM, dimethylformamide (DMF), dimethyl sulfoxide (DMSO), 1,4-dioxane (DXN), ethanol (EtOH), methanol (MeOH) and tetrahydrofuran (THF). 1H- and 13C-NMR spectra were recorded at 298.15 K, unless otherwise stated, on an Avance III 400 NMR spectrometer (Bruker, Bremen, Germany) operating at 9.4 T, observing 1H at 400.13 MHz and 13C at 100.63 MHz or on a Bruker Avance III 600 NMR spectrometer operating at 14.09 T, observing 1H at 600.13 and 13C at 150.91 MHz. Solutions were prepared in CDCl3 or DMSO-d6. Proton peak splittings are expressed as s (singlet), br s (broad singlet), d (doublet), t (triplet), br t (broad triplet), qt (quintet), br qt (broad quintet) or m (multiplet). The assignments of the carbons were made based on DEPT 90 and DEPT 135 spectra. The 1H-NMR and 13C-NMR spectra of all synthesized dyes are presented as supplementary material. High resolution electrospray ionization time-of-flight mass spectra (HRESI-TOFMS) were carried out on a microTOF (focus) spectrometer Bruker Daltonics (Bremen, Germany, located at University of Vigo).

2.1.1. Synthesis of 2-[(1-hexyl-6-iodoquinolin-2(1H)-ylidene)methyl]-4-[(3-hexylbenzothiazol-3-ium-2-yl)methylene)- 3-oxocyclobut-1-en-1-olate (10)

A mixture of monosubstituted intermediate 6 (0.80 g, 2.43 mmol) and quaternary ammonium salt 9 (1.17 g, 2.43 mmol) was heated under reflux for 3h in n-butanol/pyridine (10%) (120 mL). After cooling at r.t. CH2Cl2 was added, and the mixture was washed with cold water. The organic layer was dried over anhydrous Na2SO4 and the solvent removed under reduced pressure. The resulting solid was recrystallized from Et2O/CH2Cl2/MeOH. Yield: 53%. Golden brown crystals. M.p. 143–144 °C. Vis λmax (DMSO): 726 nm, log ε = 5.26. Vis λmax (DMEM): 640 nm. Vis λmax (ACN): 714 nm, log ε = 5.25. Vis λmax (ACT): 720 nm, log ε = 5.12. Vis λmax (DCM): 723 nm, log ε = 5.16. Vis λmax (DMF): 725 nm, log ε = 5.14. Vis λmax (DXN): 729 nm, log ε = 5.15. Vis λmax (EtOH): 701 nm, log ε = 5.22. Vis λmax (MeOH): 695 nm, log ε = 4.45. Vis λmax (THF): 733 nm, log ε = 5.06. IR υmax (KBr): 3052, 2912, 2853, 1729, 1549, 1450, 1304, 1253, 1177, 1087, 975 cm−1; 1H-NMR (600 MHz, CDCl3) δ: 9.28 (1H, d, J = 7.8 Hz, ArH), 7.77 (1H, s, ArH), 7.72 (1H, d, J = 8.4 Hz, ArH), 7.54 (1H, d, J = 7.8 Hz, ArH), 7.37 (1H, t, J = 7.5 Hz, ArH), 7.28 (1H, br s, ArH), 7.20 (1H, t, J = 7.5 Hz, ArH), 7.13 (1H, d, J = 8.4 Hz, ArH), 7.02 (1H, d, J = 9.0 Hz, ArH), 5.89 (1H, s, C=CH), 5.73 (1H, s, C=CH), 4.10–4.06 (4H, m, NCH2(CH2)4CH3), 1.81 (4H, qt, NCH2CH2(CH2)3CH3), 1.53 (2H, qt, N(CH2)2CH2(CH2)2CH3), 1.45 (2H, qt, N(CH2)2CH2(CH2)2CH3), 1.42–1.32 (8H, m, N(CH2)3(CH2)2CH3), 0.94 (3H, t, J = 6.9 Hz, N(CH2)3CH3), 0.91 (3H, t, J = 6.9 Hz, N(CH2)3CH3) ppm; 13C-NMR (150.91 MHz, CDCl3) δ: 175.52, 159.20, 149.78, 141.02, 139.19 (ArCH), 139.05, 136.67 (ArCH), 131.01 (ArCH), 128.53, 127.73 (ArCH), 126.98, 126.95 (ArCH), 123.83 (ArCH), 122.04 (ArCH), 116.06 (ArCH), 111.26 (ArCH), 93.13 (C=CH), 86.86, 85.41 (C=CH), 47.98 (NCH2), 46.17 (NCH2), 31.36 (CH2), 27.22 (CH2), 26.48 (CH2), 26.40 (CH2), 26.37 (CH2), 22.55 (CH2), 22.44 (CH2), 13.92 (CH3) ppm; HRESI-TOFMS m/z: 664.16035 [M]+ (C34H37IN2O2S+, calc. 664.16149).

2.1.2. Synthesis of 3-hexyl-2-[(3-[(1-hexyl-6-iodoquinolin-2(1H)-ylidene)methyl]-2-methoxy-4-oxocyclobut-2-en-1-ylidene)methyl]benzothiazol-3-ium trifluoromethanesulfonate (11)

To a solution of squaraine cyanine dye 10 (0.800 g, 1.20 mmol) in anhydrous CH2Cl2, stirred under N2 atmosphere at r.t., was added an excess of CF3SO3CH3 (0.395 mL, 3.60 mmol). After 28 h, the mixture was quenched with cold 5% aqueous NaHCO3. The organic layer, after separation by decantation, was dried over anhydrous Na2SO4 and the solvent removed under reduced pressure. Yield: 73%. Bright green crystals. M.p. 215–218 °C. Vis λmax (DMSO): 677 nm, log ε = 5.25. Vis λmax (ACN): 665 nm, log ε = 5.28. Vis λmax (ACT): 668 nm, log ε = 5.24. Vis λmax (DCM): 672 nm, log ε = 5.33. Vis λmax (DMF): 675 nm, log ε = 5.23. Vis λmax (DXN): 680 nm, log ε = 5.11. Vis λmax (EtOH): 668 nm, log ε = 5.27. Vis λmax (MeOH): 665 nm, log ε = 4.60. Vis λmax (THF): 671 nm, log ε = 5.26. IR υmax (KBr): 2955, 2930, 1553, 1506, 1443, 1379, 1352, 1258, 1184, 1153, 1119, 1030 cm−1; 1H-NMR (600 MHz, CDCl3) δ: 8.65 (1H, br s, ArH), 7.92 (1H, s, ArH), 7.88 (1H, d, J = 9.0 Hz, ArH), 7.63 (2H, t, J = 7.5 Hz, ArH), 7.48 (1H, t, J = 7.2 Hz, ArH), 7.41 (1H, d, J = 9.0 Hz, ArH), 7.35–7.33 (2H, m, ArH), 6.08 (1H, s, C=CH), 5.55 (1H, s, C=CH), 4.61 (3H, s, OCH3), 4.39 (2H, t, J = 7.2 Hz, NCH2(CH2)4CH3), 4.32 (2H, br s, NCH2(CH2)4CH3), 1.81 (4H, qt, NCH2CH2(CH2)3CH3), 1.56 (2H, qt, N(CH2)2CH2(CH2)2CH3), 1.46–1.36 (6H, m, N(CH2)2(CH2)2CH2CH3), 1.31 (4H, br s, N(CH2)4CH2CH3), 0.92 (3H, t, J = 6.0 Hz, N(CH2)5CH3), 0.86 (3H, t, J = 6.3 Hz, N(CH2)5CH3) ppm; 13C-NMR (150.91 MHz, CDCl3) δ: 177.91, 162.08, 158,77, 157.49, 151.28, 141.05 (ArCH), 140.59, 138.40, 137.32 (ArCH), 134.84 (ArCH), 128.13 (ArCH), 128.00, 126.81, 125.54 (ArCH), 125.11 (ArCH), 122.27 (ArCH), 119.81, 117.75 (ArCH), 113.27 (ArCH), 91.83 (C=CH), 89.69, 86.50 (C=CH), 61.30 (OCH3), 48.95 (NCH2), 47.12 (NCH2), 31.43 (CH2), 31.34 (CH2), 27.84 (CH2), 27.12 (CH2), 26.30 (CH2), 26.16 (CH2), 22.46 (CH2), 22.39 (CH2), 13.94 (CH3), 13.91 (CH3) ppm; HRESI-TOFMS m/z: 679.18313 [M-CF3SO3]+ (C35H40IN2O2S+, calc. 679.18497).

2.1.3. Synthesis of 2-[(2-amino-3-[(1-hexyl-6-iodoquinolin-2(1H)-ylidene)methyl]-4-oxocyclobut-2-en-1-ylidene)methyl]-3-hexylbenzothiazol-3-ium trifluoromethanesulfonate (12)

To a solution of O-methylated squaraine cyanine dye 11 (0.20 g, 0.24 mmol) in anhydrous CH2Cl2, under N2 atmosphere at r.t., was added an excess of 2 M ammonia solution in MeOH (0.54 mL, 1.08 mmol). The reaction mixture was stirred at r.t. for 22 h and then washed with cold water. The organic layer was dried over anhydrous Na2SO4, and the solvent was removed under reduced pressure. The product was recrystallized from CH2Cl2/MeOH. Yield: 65%. Green crystals. M.p. 282–285 °C (dec.). Vis λmax (DMSO): 705 nm, log ε = 5.17. Vis λmax (DMEM): 619 nm. Vis λmax (ACN): 686 nm, log ε = 5.36. Vis λmax (ACT): 690 nm, log ε = 5.36. Vis λmax (DCM): 694 nm, log ε = 5.38. Vis λmax (DMF): 700 nm, log ε = 5.31. Vis λmax (DXN): 706 nm, log ε = 5.27. Vis λmax (EtOH): 693 nm, log ε = 5.38. Vis λmax (MeOH): 687 nm, log ε = 5.36. Vis λmax (THF): 702 nm, log ε = 5.26. IR υmax (KBr): 3319, 3205, 2954, 2929, 1643, 1553, 1524, 1449, 1384, 1354, 1273, 1249, 1170, 1158, 1080, 1032, 977 cm-1; 1H-NMR (600 MHz, DMSO) δ: 8.91 (1H, d, J = 9.6 Hz, ArH), 8.81 (1H, br s, NH, exchange with D2O), 8.69 (1H, br s, NH, exchange with D2O), 8.16 (1H, d, J = 1.8 Hz, ArH), 7.96–7.92 (2H, m, ArH), 7.83 (1H, d, J = 9.6 Hz, ArH), 7.65 (1H, d, J = 8.4 Hz, ArH), 7.55 (1H, d, J = 9.6 Hz, ArH), 7.52 (1H, t, J = 7.8 Hz, ArH), 7.35 (1H, t, J = 7.8 Hz, ArH), 6.10 (1H, s, C=CH), 5.86 (1H, s, C=CH), 4.23 (4H, t, J = 7.5 Hz, NCH2(CH2)4CH3), 1.76–1.67 (4H, m, NCH2CH2(CH2)3CH3), 1.51 (2H, qt, N(CH2)2CH2(CH2)2CH3), 1.42 (2H, qt, N(CH2)2CH2(CH2)2CH3), 1.36–1.27 (8H, m, N(CH2)3(CH2)2CH3), 0.90 (3H, t, J = 6.9 Hz, N(CH2)5CH3), 0.87 (3H, t, J = 6.9 Hz, N(CH2)5CH3) ppm; 13C-NMR (150.91 MHz, DMSO) δ: 174.24, 167.24, 160.27, 157.75, 155.79, 150.37, 140.64, 140.07 (ArCH), 138.27, 136.79 (ArCH), 133.67 (ArCH), 127.71 (ArCH), 127.46, 126.64, 125.25 (ArCH), 124.69 (ArCH), 122.68 (ArCH), 117.95 (Ar-CH), 113.11 (ArCH), 93.57 (C=CH), 89.60, 86.02 (C=CH), 47.84 (NCH2), 46.20 (NCH2), 31.07 (CH2), 30.95 (CH2), 27.12 (CH2), 26.63 (CH2), 25.77 (CH2), 25.61 (CH2), 22.19 (CH2), 22.06 (CH2), 13.91 (CH3), 13.85 (CH3) ppm; HRESI-TOFMS m/z: 664.18409 [M-CF3SO3]+ (C34H39IN3OS+, calc. 664.18530).

2.1.4. Synthesis of 3-hexyl-2-[(3-[(1-hexyl-6-iodoquinolin-2(1H)-ylidene)methyl]-2-methylamino-4-oxocyclobut-2-en-1-ylidene)methyl]benzothiazol-3-ium trifluoromethanesulfonate (13)

To a solution of O-methylated squaraine cyanine dye 11 (0.20 g, 0.24 mmol) in anhydrous CH2Cl2, under N2 atmosphere at r.t., was added an excess of 2 M methylamine solution in THF (0.54 mL, 1.08 mmol). The reaction mixture was stirred at r.t. for 2 h and then washed with cold water. The organic layer was dried over anhydrous Na2SO4, and the solvent was removed under reduced pressure. The resulting solid was recrystallized from CH2Cl2/MeOH. Yield: 50%. Brown crystals. M.p. 246–247 °C. Vis λmax (DMSO): 715 nm, log ε = 5.18. Vis λmax (DMEM): 637 nm. Vis λmax (ACN): 699 nm, log ε = 5.25. Vis λmax (ACT): 703 nm, log ε = 5.21. Vis λmax (DCM): 707 nm, log ε = 5.30. Vis λmax (DMF): 711 nm, log ε = 5.20. Vis λmax (DXN): 716 nm, log ε = 5.15. Vis λmax (EtOH): 702 nm, log ε = 5.28. Vis λmax (MeOH): 698 nm, log ε = 5.25. Vis λmax (THF): 714 nm, log ε = 5.17. IR υmax (KBr): 3240, 2953, 2930, 1623, 1551, 1445, 1380, 1347, 1286, 1242, 1180, 1157, 1112, 1078, 1029, 988 cm−1; 1H-NMR (400 MHz, DMSO) δ: 9.02 (2H, br s, NH, exchange with D2O), 9.00 (1H, d, J = 9.6 Hz, ArH), 8.88 (1H, d, J = 9.6 Hz, ArH), 8.21 (1H, s, ArH), 8.13 (1H, s, ArH), 8.00–7.96 (2H, m, ArH), 7.93–7.90 (3H, m, ArH), 7.78 (1H, d, J = 9.6 Hz, ArH), 7.71 (1H, d, J = 8.8 Hz, ArH), 7.64 (2H, t, J = 8.4 Hz, ArH), 7.59 (1H, d, J = 6.0 Hz, ArH), 7.55 (1H, d, J = 7.2 Hz, ArH), 7.52–7.48 (2H, m, ArH), 7.38 (1H, t, J = 8.8 Hz, ArH), 6.19 (1H, s, C=CH), 6.04 (1H, s, C=CH), 5.92 (1H, s, C=CH), 5.82 (1H, s, C=CH), 4.35 (4H, br t, J = 7.0 Hz, NCH2(CH2)4CH3), 4.26 (4H, br t, J = 7.0 Hz, NCH2(CH2)4CH3), 3.35 (3H, s, NCH3, only appears in DMSO + D2O spectrum), 3.32 (3H, s, NCH3, only appears in DMSO + D2O spectrum), 1.72 (8H, br qt, NCH2CH2(CH2)3CH3), 1.49 (4H, br qt, N(CH2)2CH2(CH2)2CH3), 1.40 (4H, br qt, N(CH2)2CH2(CH2)2CH3), 1.36–1.27 (16H, m, N(CH2)3(CH2)2CH3), 0.90–0.84 (12H, m, N(CH2)5CH3) ppm; 13C-NMR (100.63 MHz, DMSO) δ: 173.62, 173.54,165.36, 165.30, 160.88, 159.21, 157.22, 156.59, 155.70, 154.51, 150.55, 149.52, 140.59, 140.47, 140.21 (ArCH), 139.87 (ArCH), 138.46, 138.13, 136.88 (ArCH), 136.56 (ArCH), 134.16 (ArCH), 132.83 (ArCH), 127.84 (ArCH), 127.62 (ArCH), 126.78, 126.35, 125.25 (ArCH), 125.10 (ArCH), 124.99 (ArCH), 124.48 (ArCH), 122.76 (ArCH), 122.47 (ArCH), 121.74, 119.60, 118.09 (ArCH), 117.77 (ArCH), 113.35 (ArCH), 112.94 (ArCH), 94.03 (C=CH), 93.65 (C=CH), 90.11, 89.25, 86.61 (C=CH), 86.33 (C=CH), 48.18 (NCH2), 48.00 (NCH2), 46.41 (NCH2), 45.70 (NCH2), 31.10 (CH2), 30.98 (CH2), 30.93 (CH2), 30.81 (CH2), 30.30 (NHCH3), 30.06 (NHCH3), 27.24 (CH2), 26.87 (CH2), 26.79 (CH2), 26.30 (CH2), 25.76 (CH2), 25.69 (CH2), 25.63 (CH2), 22.23 (CH2), 22.17 (CH2), 22.11 (CH2), 22.04 (CH2), 13.93 (CH3), 13.88 (CH3), 13.85 (CH3), 13.83 (CH3) ppm; HRESI-TOFMS m/z: 678.19974 [M-CF3SO3]+ (C35H41IN3OS+, calc. 678.20095).

2.2. Singlet Oxygen Formation Quantum Yields Measurement

Singlet oxygen formation quantum yields were determined using a nitrogen laser (OBB OL-401 from Horiba) exciting at 337.1 nm with 0.60 ns pulses and 1.1 mJ/pulse), in air equilibrated samples. The detector was an indium gallium arsenide CCD (model i-Dus from Andor Technology Limited, Belfast, UK) working at −60 °C coupled to a fixed spectrograph, model Shamrock 163i, also from Andor [50]. Phenazine was used as a standard at O.D. = 0.6 in chloroform. The quantum yield values were obtained by a simple comparison of the total areas of the emission spectra determined for the standard and samples, using the same O.D. at the excitation wavelength. For each determination, an average of 100 phosphorescence spectra were used.

2.3. Photostability Monitoring

Working solutions of each squaraine dye at a concentration of 20 µM were prepared by diluting dyes’ stock solutions in DMSO at 1 mM. To each well of a 96-well plate was added in quadruplicate 100 µL of each working solution. Squaraines were repetitively irradiated with suitable LED system equipment, which characterization is presented in the next section. Dyes absorbance was measured at the maximum absorption wavelength of each dye in DMSO for 60 min using Multiscan Go spectrophotometer microplate reader (Thermo Fisher Scientific, Vantaa, Finland).

2.4. In Vitro Photobiological Evaluation

The human colon adenocarcinoma and hepatocellular carcinoma cell lines, Caco-2 (Cell Lines Service, Eppelheim, Germany) and HepG2 (American Type Culture Collection, Rockville, USA) respectively, were grown as a monolayer culture in Dulbecco’s Modified Eagle Medium (DMEM) supplemented with 10% (v/v) heat-inactivated fetal bovine serum (FBS), 1 mM l-glutamine, 100 U/mL penicillin and 100 µg/mL streptomycin, at 37 °C in a humidified atmosphere of 5% CO2. The medium of these two cell lines was changed every two days, and cells were replated before reaching confluence. All reagents and consumables for cell culture were obtained from Gibco (Alfagene, Lisbon, Portugal). The general methods applied for handling these cell lines are already described in the literature [51,52].
At confluence, cells were trypsinized, counted, and resuspended in culture media at a density of 5 × 104 cells/mL, and then 100 µL/well of cell suspension was added to a 96-well culture plate for seeding and incubated at 37 °C under 5% CO2. After 24 h of cell growth, the medium was removed, and the cells incubated with serum-free culture medium solution of differing squaraine dyes’ concentrations (0.1, 1, 1.5 and 5 µM). The maximum DMSO concentration used in cell viability assays did not produce significant effects on cell proliferation (data not shown). A negative control was performed exposing the cells only to the cell culture medium.
After 24 h of squaraine dyes incubation, cells were exposed to three different irradiation conditions: (i) 0 min of irradiation (without irradiation; cells were protected from ambient light), (ii) 7 min of irradiation and (iii) 14 min of irradiation. The irradiation was performed with a self-designed and constructed apparatus consisting of an arrangement of LEDs of required wavelength. The device was built using aluminum gallium indium phosphide LEDs (B5B-445-TL, Roithner, Vienna, Austria) with a spectral emission peak at λ = 630.8 ± 0.8 nm with P = 4.3 ± 0.5 mW, operating at 20 mA. The apparatus was placed over the 96-well plates, with the LEDs fronting the cells, and each LED irradiated a single well at approximately 1.5 cm away from the wellbore, as previously described [25]. After light-treatment, cells were incubated for 1 h or 24 h with irradiated dyes. Later the media containing the dye solutions was removed, and the cells were washed with phosphate-buffered saline solution (PBS; 137.0 mM NaCl, 2.7 mM KCl, 1.75 mM KH2PO4, 10.0 mM Na2HPO4, pH 7.4).
Finally, in order to assess the photodynamic effects of squaraine dyes 10, 12 and 13, the culture medium containing the irradiated dyes was replaced by a 10% (v/v) Alamar Blue solution diluted in a serum-free culture medium. After about 4 to 5 h of Alamar Blue incubation, absorbance at 570 (reduced form) and 620 nm (oxidized form) was read in a Multiskan EX microplate reader (MTX Labsystems, Vantaa, Finland). The data were analyzed by calculating the percentage of Alamar Blue reduction and expressed as a percentage of control (untreated cells), as previously described [51].

Data Statistical Analysis

The photobiological assays were performed in quadruplicate, and its data are expressed as mean value ± standard deviation (mean ± SD). Statistical significance was determined using a Student’s t-test of the data of dye treatments and control, and differences were considered statistically significant for a p-value lower than 0.05. The IC50 values determination was done from the concentration-response curves by sigmoidal fitting analysis considering a 95% confidence interval and with the bottom of the curves constrained to greater than 0% of relative cell proliferation. All data shown are representative of at least three independent experiments.

3. Results and Discussion

3.1. Synthesis and Characterization

The initial goal of this work was the synthesis of novel unsymmetrical squaraine cyanine dyes that exhibit properties inherent to those of an ideal photosensitizer molecule, aiming at the discovery of new photosensitizing potential molecules to be applied in cancer PDT.
The design of the molecules intended to be synthesized was based on the photophysical and photochemical studies already described in the literature, which reported that quinoline-based squaraines displayed higher wavelength absorption capacity than their benzothiazole- and benzoselenazole-based analogs, a photophysical property considered advantageous since, it allows greater therapeutic efficacy, as these molecules may be distributed to deeper tissue zones as they will be able to absorb and be stimulated by radiation of higher wavelength [5,53]. On the other hand, the introduction of heavy atoms into the dye structure, such as iodine, chlorine, or bromine, is widely described to improve its performance relative to its singlet oxygen production ability [54,55]. The choice of these unsymmetrical dyes also being derived from benzothiazole was due to the fact that this heterocycle correlates with notable phototherapeutic activity [56,57]. Given that increasing length of the pendant N-alkyl chains positively influences photophysical properties such as singlet oxygen production ability and maximum absorption wavelength, N-hexyl chains have been introduced in both heterocyclic dye moieties [8,58].
Thus, unsymmetrical squaraine cyanine dyes 1013 bearing 6-iodoquinoline and benzothiazole moieties were successfully prepared by a multistep procedure, as illustrated in Scheme 1. The dyes preparation was initiated by the quaternization of the commercially 2-methylbenzothiazole 1, through the alkylation of the nitrogen atom with iodohexane, resulting in the synthesis of the quaternary ammonium salt 2 [45]. Then, dibutyl squarate (4), obtained by the reaction between squaric acid (3) and n-butanol, reacted with the benzothiazole-based quaternary ammonium salt 2 to afford the monosubstituted intermediate 5 [46,47]. This latter intermediate was posteriorly hydrolyzed using a 40% sodium hydroxide aqueous solution, and the resulting sodium salt was protonated with a 2 M hydrochloric acid solution, yielding the key monosubstituted intermediate 6 [47].
The zwitterionic unsymmetrical squaraine dye 10 was prepared by a base-catalyzed condensation of intermediate 6 with the iodoquinoline-based quaternary ammonium salt 9, in a n-butanol/pyridine refluxing mixture. Ammonium salt 9 was prepared by the alkylation of 6-iodo-1-hexylquinaldine (8) with iodohexane [49], obtained by the described Doebner-Miller reaction between 4-iodoaniline (7) and crotonaldehyde in hydrochloric acid [48,59]. Methylation of the unsubstituted squaraine dye 10 with methyl trifluoromethanesulfonate produced the O-methyl ether intermediate 11 [4]. Finally, the aminosquaraine cyanine dyes 12 and 13 were obtained by nucleophilic substitution of the methoxy group of the O-methyl derivative 11 by ammonia and methylamine solutions, respectively [4,25]. As far as we know, all the synthesized squaraine cyanine dyes are not described in the literature, and their synthesis and spectroscopic characterization are herein presented for the first time.
The main features in the 1H-NMR spectra of dyes 1013 (Figures S1, S3 and S5) are the signals corresponding to the methine-protons. For 10, 11 and 12, the protons above referred appear at δ 5.89 and 5.73, 6.08 and 5.55, 6.10 and 5.86 ppm, respectively, as two singlets since these dyes have two different heterocycle rings. In the case of dye 13 (Figure S8), two additional singlets were observed in that region of the spectrum (6.19, 6.04, 5.92 and 5.82 ppm) as result of the hindrance of free rotation of the N-methylamine group, due to the partial character of the double bond between the nitrogen atom and the carbon atom of the four-membered ring, that should promote the non-equivalence of chemical environments. This phenomenon was previously observed in the NMR spectra of several symmetrical aminosquaraine cyanine dyes [24,60] and unsymmetrical aminosquaraine cyanine dyes [25]. It is also noted that in the spectrum of 13 the peaks of the NCH3 groups are under the water peak of the solvent but appear in the spectrum with D2O, at the chemical shifts of 3.35 and 3.32 ppm as two singlets of three protons each. Another important feature was observed in the 13C-NMR spectra of dye 13 (Figure S10) where the four signals that appeared at δ 94.03, 93.65, 86.61 and 86.33 ppm were assigned to the methine-carbons. In the spectra of the another dyes 1012, as expected, only two signals appear for each of the methine-carbons (Figures S2, S4 and S7).

3.2. Photophysical Properties

One of the most significant advances to be improved in PDT is the progression to the treatment of pathologies originating from deeper tissues, which can barely be treated with current porphyrin-based photosensitizers [61]. Thus, these light-sensitive compounds should possess photophysical properties such as high absorption capacity within the so-called “phototherapeutic window” (650–850 nm) and great singlet oxygen quantum yield. The photosensitizers that absorb in this electromagnetic spectrum region are the ones that can be the most easily excited in deeper tissues, since our body’s constituents, such as proteins and other biomolecules, do not absorb radiation at this spectral range [62,63]. Once the photodynamic activity of a photosensitizer may be due to two reaction types, type I or type II reactions [64], the singlet oxygen quantum yield measurement is relevant for this study since this value reflects the ability of new photosensitizing molecules to produce this highly cytotoxic ROS [55] and allows us to infer about the nature of the main reaction type to be produced in biological media [8].
All the prepared dyes exhibited sharp and intense absorption in the Vis/NIR region, matching the tissue transparency spectral region (Figure 1; Table 1). In DMSO, the four-membered central ring unsubstituted squaraine dye 10 displayed absorption at longer wavelengths than the aminosquaraine ones (12 and 13), in which the insertion of amine groups was found to produce a slight hypsochromic effect [4] (Figure 1. Compared to the non-iodinated analog dyes reported in our previous study [25], there is a bathochromic shift of at least 10 nm, so the introduction of this heavy atom influenced this photophysical property. When dissolved in Dulbecco’s Modified Eagle Medium (DMEM), the dyes exhibited broader absorption bands, behavior possibly explained by the formation of aggregates in this aqueous medium [65] (Figure 1). The acquisition of these spectra in this culture medium is due to the need to construct a light source that emits radiation close to the maximum absorption wavelength of the dyes in the solvent where cytotoxicity assays were carried out so that the squaraines perform the maximum activity. O-methyl ether dye 11 was not entered in this photodynamic study, and it was not shown the cell culture media spectra since it easily hydrolyzes in aqueous medium yielding its unsubstituted precursor 10.
To evaluate the photosensitizing ability of the synthesized dyes, the singlet oxygen formation quantum yields were measured in chloroform, and phenazine was used as a standard for its determination, as already described [55] (Table 1). In general, all iodinated dyes displayed quantum yields of less than 0.1, which is considered very low. Thus, compared to the non-iodinated dyes that we reported [25] and contrary to what is described in the literature [9], the heavy atom introduction into the heterocyclic quinoline moiety does not produced an increase in the singlet oxygen production ability of these dyes. Although reported as a crucial property in the phototherapeutic activity of a photosensitizer, as this ROS is highly relevant in biological systems [66], photosensitizing compounds with low singlet oxygen generation ability may exhibit consistent photodynamic effects resulting from the marked production of type I reactions [25,67].
In Figure 2, the normalized Vis/NIR absorption spectra of the squaraine dyes 1013 in acetonitrile, acetone, dichloromethane, dimethylformamide, dimethyl sulfoxide, 1,4-dioxane, ethanol, methanol and tetrahydrofuran are presented. The relevant spectra data are summarized in Table 2. Regardless of the solvent polarity, all compounds showed a narrow absorption band in the Vis/NIR region and high molar extinction coefficient values (4.0 < log ε (M−1·cm−1) < 5.5) in agreement with π-π* transitions. The introduction of the methoxy group and amines into the four-membered central ring had effects on the maximum absorption wavelength, proposing that the electronic levels involved in the π-π* transition have different energies. Additionally, the formation of a hypsochromic shoulder, a typical photophysical characteristic of this core of dyes, is also observable regardless of the solvent.

3.3. Photodegradation Evaluation

Since photosensitizers are ideally tools that produce ROS only in the presence of radiation, the stability evaluation of these compounds when exposed to this condition is of particular interest. Photodegradation of the potential photosensitizing candidate is considered a disadvantage since the destruction of the light-sensitive molecule in other products may complicate the interpretation of the experimental results as well as lead to decreased efficiency of ROS production [68,69]. Nevertheless, most commercial photosensitizing drugs used in tumor photodynamic treatment, such as porphyrins and chlorines, have poor photostability [70]. It is known that squaraine dyes are a class of compounds with fair photostability and that this photochemical property is mainly related to the nature of heterocyclic units [71].
For the photodegradation monitoring, solutions of each unsymmetrical squaraine dye in DMSO were irradiated by a light-emitting diode (LED) system centered at 630.8 ± 0.8 nm for periods of 1 min from 0 to 20 min, 2 min from 20 to 40 min and 5 min from 40 min to 60 min (Figure 3). All dyes showed moderate photostability, except for the precursor O-methylated dye 11, which degradation over the irradiation time was more pronounced. The remaining dyes showed very similar light stability over the studied time period. Unsubstituted dye 10 and aminosquaraines 12 and 13, after 14 min of irradiation, longer irradiation time performed in in vitro cytotoxicity assays, showed reduced degradation. Thus, we can consider that the in vitro photodynamic effects produced up to this irradiation period are of the dye in question, without significant interference of degradative compounds.

3.4. Photocytotoxicity Studies

An efficient PDT photosensitizer needs to possess relevant photocytotoxicity and low dark toxicity [30]. The evaluation of the toxicity level of novel compounds using cell lines as in vitro models is recurrent, as they have prolonged life expectancy, phenotypic stability and easy handling [72]. HepG2 is a human hepatoma nontumorigenic cell line with high growth and proliferation rates that allows the hepatotoxicity and drug metabolism research [72]. The photocytotoxicity study in the human colorectal carcinoma cell line Caco-2 is of particular interest as these cells have morphological and biochemical characteristics similar to those of the intestinal epithelium, as well as being an ideal in vitro model of the third most common malignant pathology and second cancer-related cause of death [73,74].
Thus, to determine the concentration range at which a in vitro phototherapeutic effect is produced, Caco-2 and HepG2 cells were exposed to increasing concentrations (0.1, 1.0, 5.0 and 10.0 µM) of squaraine cyanine dyes 10, 12 and 13. Irradiation was executed by a self-made LED system centered at 630.8 ± 0.8 nm with a power of 4.3 ± 0.5 mW for periods of 7 or 14 min, and a non-irradiated control was also performed. Cell viability was evaluated at 1 h or 24 h after irradiation by using Alamar Blue, a reliable and straightforward colorimetric method, which has several advantages compared to standard techniques such as 3-[4,5-dimethylthiazole-2-yl]-2,5-diphenyltetrazolium bromide (MTT) reduction assay, due to its high sensitivity, stability and minimal cell toxicity that allows continuous viability monitoring [75]. Dark and light cytotoxicity of culture medium containing the maximum DMSO concentration used were also assessed, and data confirmed that these did not influence the cell viability percentage (data not shown).
All the squaraine cyanine dyes induced a decrease of Caco-2 cell proliferation and dose-dependent cytotoxicity was observed. Interestingly, the unsubstituted squaraine dye 10 showed the most significant phototherapeutic potential in the Caco-2 cell line compared to aminosquaraine dyes, since that at 5.0 and 10.0 µM the presence of radiation was necessary to reduce cell viability in more than 30% (threshold level for cytotoxicity according to the Generally Recognised As Safe (GRAS) standards [76]) (Figure 4). The exposure times of Caco-2 cells to synthesized squaraine dyes showed to have an impact on dye cytotoxicity. Proof of this is the abrupt decrease in cell viability occurred at the concentration of 1.0 µM, 23 h after 1 h exposure reading with the irradiated dye, as well as at 10.0 µM without irradiation, regardless of the dye evaluated. The substitution of hydrogen atom by the methyl group did not potentiate the photodynamic activity of dye 13 since both aminosquaraines (12 and 13) showed very similar cytotoxicity results for the colorectal adenocarcinoma cells. The latter produced a good phototherapeutic effect at 5.0 µM when cells were exposed for 1 h to irradiated dye and at 1.0 and 5.0 µM when cells were analysed 24 h after exposure. Thus, the incubation of the cells over a more extended time period made it possible to increase the cytotoxic effect of these aminosquaraine dyes produced in vitro as photodynamic effect. Note that at the 1.0 µM concentration and an incubation time of 24 h, aminosquaraines can only abruptly reduce cell viability at 14 min of irradiation, so that the amount of energy absorbed may be strictly linked to the photosensitizer candidates’ biological action.
The dyes showed different degrees of cytotoxicity depending on the cell lines under study. These differences are due to the fact that each cell line is a system with its unique biological characteristics, nevertheless of whether they originate from the same tissue, species or histological tumor type, given the individual properties of the biological material from which the cell lines have been established and heterogeneity of the tumor cells [77,78]. Among the three dyes, the one that stood out most in the HepG2 cell line was the unsubstituted dye 10 (Figure 5). This dye produces, compared to the Caco-2 cell line, a more evident photodynamic effect at 5 and 10 µM concentrations, 1 h after irradiation. This effect is explained by the total absence of hepatocytotoxicity in the absence of radiation, which despite showing less than 30% decrease in cell viability, was statistically significant at the 10 µM concentration for the colorectal carcinoma cell line.
In contrast to the Caco-2 cell line, in which aminosquaraine 12 showed therapeutic properties, this dye evidenced weak photodynamic activity for HepG2 cells, since the conditions in which light produces reduced cell viability also decreased in the absence of irradiation. Finally, the compound bearing methylamino group 13 shows a slight photodynamic activity at a concentration of 1 µM under both irradiation conditions and times after irradiation. Similar effects of these dyes were produced in Caco-2 cells, but at a concentration of 5 µM, so the compound showed higher potency for the hepatocyte cell line.
Furthermore, the half-inhibitory concentration (IC50) of the evaluated squaraines was determined for each incubation and irradiation times of both studied cell lines by sigmoidal fitting analysis, and these values confirm the relevance and phototherapeutic ability of unsubstituted dye 10 (Table 3). Of the evaluated compounds, dye 10 has the highest IC50 values in the absence of light, regardless of cell line and incubation time, indicating low dark toxicity, and clearly lower IC50 values when irradiated, specifying good phototherapeutic response. The sensitivity of the hepatocyte cell line to aminosquaraine dyes 12 and 13 is evidenced by the significantly lower IC50 values under most conditions compared to the colorectal cell line (Table 3). Nevertheless, it is noteworthy that the aminosquaraine dyes produced considerably lower IC50 values when irradiated, so their in vitro photocytotoxic activity is not questioned. An inverse proportionality of photocytotoxicity to irradiation time and incubation time with irradiated dyes is also reflected in these values, since the longer the incubation and irradiation times, the lower the IC50 values.
In our last study [25], we concluded that unsymmetrical benzothiazole- and quinoline-based squaraine cyanine dyes has desirable photophysical and photobiological properties for their potential application as PDT photosensitizers, however, changes in their structure would be necessary to reduce dark cytotoxicity. Considering that it is already described in the literature that the introduction of heavy atoms in the structure of these core of dyes seems to improve their phototherapeutic performance by increasing their singlet oxygen production ability [79], we aimed to study this variant in dyes analogous to those of our previous study. In general, although we have shown that the introduction of the iodine atom into the quinoline heterocycle did not increase its formation ability of this ROS, we found that this structural modification very significantly improved their in vitro phototherapeutic activity. Given the poor singlet oxygen production capacity of these dyes, such as those of their non-iodinated analogues, it can be inferred that the biological activity of these compounds mainly involves type I reactions, the mechanism by which ROS that cause a lesser extent of oxidative damage, such as superoxide anions and hydroxyl radicals, are produced. The comparison of the photodynamic activity of the dyes involved in the present study could also be rigorously made taking into account the results of the photostability assays since, besides presenting similar stability levels, they displayed a slight degradation to the irradiation times to which the cells were exposed.

4. Conclusions

In the presented work, a successful synthesis of unsymmetrical iodoquinoline- and benzothiazole-based squaraine dyes bearing amino and methylamino groups is described. All the synthesized dyes displayed narrow and intense absorption bands in the Vis/NIR region regardless of the polarity of the solvent used. Contrary to expectations, the singlet oxygen production quantum yields were similar to those obtained in non-iodinated dyes. Concerning to their photodegradation, the synthesized dyes, except for O-methylated precursor, showed moderate radiation stability. Interesting results were observed in the Alamar Blue cell proliferation assay in Caco-2 and HepG2 cells. The unsubstituted squaraine dye presented relevant in vitro phototherapeutic effects in both cell lines, as it exhibited low antiproliferative effects in the absence of irradiation (IC50 values higher than or near the maximum tested concentration) and significantly lower half inhibitory concentrations when irradiated. Besides, the introduction of amine groups into the four-membered central ring increased the dark cytotoxicity of the dyes. However, it is noteworthy that the potentiality of these latter dyes is not invalidated since, compared to the dark, the half inhibitory concentration values in the light-presence are distinctly lower. In conclusion, compared to the non-iodinated dyes of our previous study, the inclusion of iodine atoms substantially improved the photobiological performance of these core of unsymmetrical dyes, so these latter bearing this heavy atom have so far intrinsic properties of a PDT photosensitizer candidate.

Supplementary Materials

The following are available online at https://www.mdpi.com/2076-3417/9/24/5414/s1, Figure S1: 1H-NMR spectrum of dye 10 (600 MHz, CDCl3), Figure S2: 13C-NMR spectrum of dye 10 (150.9 MHz, CDCl3), Figure S3: 1H-NMR spectrum of dye 11 (600 MHz, CDCl3), Figure S4: 13C-NMR spectrum of dye 11 (150.9 MHz, CDCl3), Figure S5: 1H-NMR spectrum of dye 12 (600 MHz, DMSO-d6), Figure S6: 1H-NMR spectrum of dye 12 (600 MHz, DMSO-d6+D2O), Figure S7: 13C-NMR spectrum of dye 12 (150.9 MHz, DMSO-d6), Figure S8: 1H-NMR spectrum of dye 13 (400 MHz, DMSO-d6), Figure S9: 1H-NMR spectrum of dye 13 (400 MHz, DMSO-d6+D2O), Figure S10: 13C-NMR spectrum of dye 13 (150.9 MHz, DMSO-d6).

Author Contributions

Conceptualization, L.V.R. and A.M.S.; Investigation, S.F., E.L., R.E.B., D.F., J.R.F. and L.F.V.F.; Supervision, L.V.R. and A.M.S.; Writing–original draft, E.L.; Writing–review & editing, R.E.B., L.F.V.F., A.M.S. and L.V.R.

Funding

This research was funded by the European Investment Funds by FEDER/COMPETE/POCI under projects POCI-01-0145-FEDER-006958 (CITAB) and POCI-01-0145-FEDER-007491 (CICS-UBI) and Funds by FCT – Portuguese Foundation for Science and technology, under the projects UID/AGR/04033/2019 (CITAB) and UID/QUI/UI0616/2019 (CQ-VR). This work was also supported by funds from the Health Sciences Research Center (CICS-UBI) through National Funds by FCT—Foundation for Science and Technology (UID/Multi/00709/2019). The research at CQFM was supported by Project UID/NAN/50024/2019 and M-ERA-NET/0002/2015 from FCT.

Conflicts of Interest

The authors declare no conflict of interest.

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Scheme 1. Synthesis of iodoquinoline- and benzothiazole-derived squaraine cyanine dyes. Experimental conditions: (i) iodohexane, acetonitrile, reflux; (ii) n-butanol, reflux; (iii) triethylamine, ethanol, reflux; (iv) 1: sodium hydroxide aqueous solution (40%), 90 °C; 2: hydrochloric acid aqueous solution (2M); (v) 1: crotonaldehyde, hydrochloric acid (6M), toluene, reflux; 2: sodium hydroxide aqueous solution (6M); vi) n-butanol/pyridine (10%), reflux; (vii) methyl trifluoromethanesulfonate, dry dichloromethane, nitrogen atmosphere, room temperature (r.t.); (viii) ammonia or methylamine solution (2M), dry dichloromethane, nitrogen atmosphere, r.t.
Scheme 1. Synthesis of iodoquinoline- and benzothiazole-derived squaraine cyanine dyes. Experimental conditions: (i) iodohexane, acetonitrile, reflux; (ii) n-butanol, reflux; (iii) triethylamine, ethanol, reflux; (iv) 1: sodium hydroxide aqueous solution (40%), 90 °C; 2: hydrochloric acid aqueous solution (2M); (v) 1: crotonaldehyde, hydrochloric acid (6M), toluene, reflux; 2: sodium hydroxide aqueous solution (6M); vi) n-butanol/pyridine (10%), reflux; (vii) methyl trifluoromethanesulfonate, dry dichloromethane, nitrogen atmosphere, room temperature (r.t.); (viii) ammonia or methylamine solution (2M), dry dichloromethane, nitrogen atmosphere, r.t.
Applsci 09 05414 sch001
Figure 1. Vis/NIR absorption spectra obtained in dimethyl sulfoxide (DMSO) and in Dulbecco’s Modified Eagle Medium (DMEM) dye solutions. Absorbance was normalized and is presented as arbitrary units (a.u.).
Figure 1. Vis/NIR absorption spectra obtained in dimethyl sulfoxide (DMSO) and in Dulbecco’s Modified Eagle Medium (DMEM) dye solutions. Absorbance was normalized and is presented as arbitrary units (a.u.).
Applsci 09 05414 g001
Figure 2. Vis/NIR absorption spectra of squaraine cyanine dyes 1013 obtained in acetonitrile (ACN), acetone (ACT), dichloromethane (DCM), dimethylformamide (DMF), dimethyl sulfoxide (DMSO), 1,4-dioxane (DXN), ethanol (EtOH), methanol (MeOH) and tetrahydrofuran (THF). Absorbance was normalized and is presented as arbitrary units (a.u.).
Figure 2. Vis/NIR absorption spectra of squaraine cyanine dyes 1013 obtained in acetonitrile (ACN), acetone (ACT), dichloromethane (DCM), dimethylformamide (DMF), dimethyl sulfoxide (DMSO), 1,4-dioxane (DXN), ethanol (EtOH), methanol (MeOH) and tetrahydrofuran (THF). Absorbance was normalized and is presented as arbitrary units (a.u.).
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Figure 3. Photodegradation evaluated of squaraine cyanine dyes 1013. DMSO squaraine dye solutions were irradiated with a LED system centered at 630.8 ± 0.8 nm with the power of 4.3 ± 0.5 mW and their absorbance read over 60 min (Abst (dye): absorbance of squaraine dye when irradiated at time t; Abs0 (dye): absorbance of squaraine dye without irradiation).
Figure 3. Photodegradation evaluated of squaraine cyanine dyes 1013. DMSO squaraine dye solutions were irradiated with a LED system centered at 630.8 ± 0.8 nm with the power of 4.3 ± 0.5 mW and their absorbance read over 60 min (Abst (dye): absorbance of squaraine dye when irradiated at time t; Abs0 (dye): absorbance of squaraine dye without irradiation).
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Figure 4. In vitro phototherapeutic effects of squaraine cyanine dyes 10, 12 and 13 on Caco-2 cells. Cells were incubated for 24 h with the dyes at several concentrations (0.1, 1.0, 5.0 and 10.0 µM) and then exposed to the radiation of a LED system centered at 630.8 ± 0.8 nm and with the power of 4.3 ± 0.5 mW for 0, 7 and 14 min. Irradiated dyes were in contact with the cells for 1 h or for 24 h. Data are expressed as a percentage of control (untreated cells) and presented as mean ± standard deviation of three independent assays performed in quadruplicate. Data points without error bars showed no differences between the independent tests performed. Experiments with t-Student’s statistical significance compared to the negative control are signed by an asterisk (*) of the color relative to the irradiation time.
Figure 4. In vitro phototherapeutic effects of squaraine cyanine dyes 10, 12 and 13 on Caco-2 cells. Cells were incubated for 24 h with the dyes at several concentrations (0.1, 1.0, 5.0 and 10.0 µM) and then exposed to the radiation of a LED system centered at 630.8 ± 0.8 nm and with the power of 4.3 ± 0.5 mW for 0, 7 and 14 min. Irradiated dyes were in contact with the cells for 1 h or for 24 h. Data are expressed as a percentage of control (untreated cells) and presented as mean ± standard deviation of three independent assays performed in quadruplicate. Data points without error bars showed no differences between the independent tests performed. Experiments with t-Student’s statistical significance compared to the negative control are signed by an asterisk (*) of the color relative to the irradiation time.
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Figure 5. In vitro phototherapeutic effects of squaraine cyanine dyes 10, 12 and 13 on HepG2 cells. Cells were incubated for 24 h with the dyes at several concentrations (0.1, 1.0, 5.0 and 10.0 µM) and then exposed to the radiation of a LED system centered at 630.8 ± 0.8 nm and with the power of 4.3 ± 0.5 mW for 0, 7 and 14 min. Irradiated dyes were in contact with the cells for 1 h or for 24 h. Data are expressed as a percentage of control (untreated cells) and presented as mean ± standard deviation of three independent assays performed in quadruplicate. Data points without error bars showed no differences between the independent tests performed. Experiments with t-Student’s statistical significance compared to the negative control are signed by an asterisk (*) of the color relative to the irradiation time.
Figure 5. In vitro phototherapeutic effects of squaraine cyanine dyes 10, 12 and 13 on HepG2 cells. Cells were incubated for 24 h with the dyes at several concentrations (0.1, 1.0, 5.0 and 10.0 µM) and then exposed to the radiation of a LED system centered at 630.8 ± 0.8 nm and with the power of 4.3 ± 0.5 mW for 0, 7 and 14 min. Irradiated dyes were in contact with the cells for 1 h or for 24 h. Data are expressed as a percentage of control (untreated cells) and presented as mean ± standard deviation of three independent assays performed in quadruplicate. Data points without error bars showed no differences between the independent tests performed. Experiments with t-Student’s statistical significance compared to the negative control are signed by an asterisk (*) of the color relative to the irradiation time.
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Table 1. Relevant Vis/NIR spectral data and singlet oxygen quantum yields (ΦΔ) of squaraine cyanine dyes 1013.
Table 1. Relevant Vis/NIR spectral data and singlet oxygen quantum yields (ΦΔ) of squaraine cyanine dyes 1013.
DyeDMSODMEMΦΔ
λmax (nm)log ε (M−1·cm−1)λmax (nm)
107265.266400.03
116775.25
127055.176190.03
137155.186370.05
Table 2. Vis/NIR absorption data of the squaraine cyanine dyes 1013 in acetonitrile (ACN), acetone (ACT), dichloromethane (DCM), dimethylformamide (DMF), 1,4-dioxane (DXN), ethanol (EtOH), methanol (MeOH) and tetrahydrofuran (THF) (λmax in nm and log ε in M−1·cm−1.
Table 2. Vis/NIR absorption data of the squaraine cyanine dyes 1013 in acetonitrile (ACN), acetone (ACT), dichloromethane (DCM), dimethylformamide (DMF), 1,4-dioxane (DXN), ethanol (EtOH), methanol (MeOH) and tetrahydrofuran (THF) (λmax in nm and log ε in M−1·cm−1.
SolventDye 10Dye 11Dye 12Dye 13
λmaxlog ελmaxlog ελmaxlog ελmaxlog ε
ACN7145.256655.286865.366995.25
ACT7205.126685.246905.367035.21
DCM7235.166725.336945.387075.30
DMF7255.146755.237005.317115.20
DXN7295.156805.117065.277165.15
EtOH7015.226685.276935.387025.28
MeOH6954.456654.606875.366985.25
THF7335.066715.267025.267145.17
Table 3. Calculated IC50 values (µM) for squaraine cyanine dyes 10, 12 and 13 in Caco-2 and HepG2 cells (95% confidence level) for the different irradiation treatments (0, 7 and 14 min) and irradiated dyes’ incubation times (1 and 24 h).
Table 3. Calculated IC50 values (µM) for squaraine cyanine dyes 10, 12 and 13 in Caco-2 and HepG2 cells (95% confidence level) for the different irradiation treatments (0, 7 and 14 min) and irradiated dyes’ incubation times (1 and 24 h).
DyeIrradiation TimeCaco-2HepG2
1 h24 h1 h24 h
100′>108.811>10>10
7′2.2772.3209.6065.068
14′1.6550.4563.2912.306
120′>104.3834.4912.116
7′1.4971.0691.4781.182
14′1.3220.9891.1450.903
130′9.6323.4112.3161.645
7′1.9731.2561.4140.800
14′1.5670.7511.4410.732

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Friães, S.; Lima, E.; Boto, R.E.; Ferreira, D.; Fernandes, J.R.; Ferreira, L.F.V.; Silva, A.M.; Reis, L.V. Photophysicochemical Properties and In Vitro Phototherapeutic Effects of Iodoquinoline- and Benzothiazole-Derived Unsymmetrical Squaraine Cyanine Dyes. Appl. Sci. 2019, 9, 5414. https://doi.org/10.3390/app9245414

AMA Style

Friães S, Lima E, Boto RE, Ferreira D, Fernandes JR, Ferreira LFV, Silva AM, Reis LV. Photophysicochemical Properties and In Vitro Phototherapeutic Effects of Iodoquinoline- and Benzothiazole-Derived Unsymmetrical Squaraine Cyanine Dyes. Applied Sciences. 2019; 9(24):5414. https://doi.org/10.3390/app9245414

Chicago/Turabian Style

Friães, Sofia, Eurico Lima, Renato E. Boto, Diana Ferreira, José R. Fernandes, Luis F. V. Ferreira, Amélia M. Silva, and Lucinda V. Reis. 2019. "Photophysicochemical Properties and In Vitro Phototherapeutic Effects of Iodoquinoline- and Benzothiazole-Derived Unsymmetrical Squaraine Cyanine Dyes" Applied Sciences 9, no. 24: 5414. https://doi.org/10.3390/app9245414

APA Style

Friães, S., Lima, E., Boto, R. E., Ferreira, D., Fernandes, J. R., Ferreira, L. F. V., Silva, A. M., & Reis, L. V. (2019). Photophysicochemical Properties and In Vitro Phototherapeutic Effects of Iodoquinoline- and Benzothiazole-Derived Unsymmetrical Squaraine Cyanine Dyes. Applied Sciences, 9(24), 5414. https://doi.org/10.3390/app9245414

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