Volume 2012, Issue 1 497620

Research Article

Open Access

Benzothiazine Dyes/2,4,6-Tris(trichloromethyl)-1,3,5-triazine as a New Visible Two-Component Photoinitiator System

Corresponding Author

Radosław Podsiadły

[email protected]

Institute of Polymer and Dye Technology, Lodz University of Technology, Stefanowskiego 12/16, 90-924 Lodz, Poland p.lodz.pl

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Radosław Michalski,

Radosław Michalski

Institute of Applied Radiation Chemistry, Lodz University of Technology, Zeromskiego 116, 90-924 Lodz, Poland p.lodz.pl

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Andrzej Marcinek,

Andrzej Marcinek

Institute of Applied Radiation Chemistry, Lodz University of Technology, Zeromskiego 116, 90-924 Lodz, Poland p.lodz.pl

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Jolanta Sokołowska,

Jolanta Sokołowska

Institute of Polymer and Dye Technology, Lodz University of Technology, Stefanowskiego 12/16, 90-924 Lodz, Poland p.lodz.pl

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Radosław Podsiadły,

Corresponding Author

Radosław Podsiadły

[email protected]

Institute of Polymer and Dye Technology, Lodz University of Technology, Stefanowskiego 12/16, 90-924 Lodz, Poland p.lodz.pl

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Radosław Michalski,

Radosław Michalski

Institute of Applied Radiation Chemistry, Lodz University of Technology, Zeromskiego 116, 90-924 Lodz, Poland p.lodz.pl

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Andrzej Marcinek,

Andrzej Marcinek

Institute of Applied Radiation Chemistry, Lodz University of Technology, Zeromskiego 116, 90-924 Lodz, Poland p.lodz.pl

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Jolanta Sokołowska,

Jolanta Sokołowska

Institute of Polymer and Dye Technology, Lodz University of Technology, Stefanowskiego 12/16, 90-924 Lodz, Poland p.lodz.pl

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First published: 24 December 2012

https://doi.org/10.1155/2012/497620

Citations: 2

Academic Editor: Xie Quan

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Abstract

Novel photoinitiator systems working under visible radiation were studied. The photoredox pair constructed with dye derivatives of 12H-quinoxalino-[2,3-b][1,4]-benzothiazine (1–3) and 2,4,6-tris(trichloromethyl)-1,3,5-triazine (Tz) were found to be effective initiators for free radical polymerization of trimethylolpropane triacrylate (TMPTA) using VIS light. Photosensitization occurred through electron transfer, which was confirmed by the observation of a radical cation of the studied dyes. The 1^•+ was also characterized in cryogenic matrices (mixture of CH₂Cl₂ and ionic liquid: 1-butyl-3-methylimidazolium hexafluorophosphate (BMIM⁺PF₆ ⁻)) and its reactivity was investigated by means of pulse radiolysis in solution at room temperature. In a halogenated solvent and in a mixture of CH₂Cl₂ and BMIM⁺PF₆ ⁻, the radical cation 1^•+ underwent deprotonation to form a neutral radical 1^•, which was stable in the second time scale. During photolysis of the 1/Tz photoredox pair in 1-methyl-2-pyrrolidone and monomer, the formation of a neutral radical 1^• was not observed.

1. Introduction

One of the most widely used and simplest methods of polymer formation is radical chain addition polymerization. Light-induced photopolymerization has several advantages over other methods; the process occurs at low temperatures, and it can be controlled by manipulating the intensity and wavelength of irradiation. Photo-initiated free radical polymerization of multifunctional monomers produces highly crosslinked polymers with high thermal stability, mechanical strength, and resistance to solvent. These polymers have many industrial applications, specifically in coatings for flooring and furniture, dental restorative materials, optical fiber coatings, hard and soft contact lenses, and photolithography [1–3].

Compounds with an efficient absorbance at long wavelengths were the most significant photoinitiators in the past decade. Absorbance at lower energies is significant for two reasons: first, the development of efficient long-wavelength, UV and visible emitting light sources, such as lasers and LEDs for imaging, printing, and medical applications, has created an increasing demand for an initiator system that is effective in the 400 to 500 nm spectral region; secondly, in exterior durable photopolymers, the key development was photoinitiators that absorb outside of the UV absorption curve of traditional UV absorbers used to protect organic coatings from the harmful rays of the sun.

Many attempts have been made to develop efficient photoinitiating polymerization systems that can be used with visible light. Previously, two components systems that operated via photoinduced electron transfer were developed [3–20]. In such systems, dyes play an important role. Dyes are chromophores that absorb visible light and after excitation, they react with coinitiators (electron donor D or electron acceptor A) via electron transfer. In both cases, the initiating radicals are formed through the cleavage of the oxidized or reduced form of the coinitiator (Scheme 1).

Description unavailable — **Scheme 1**
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In the photoreducible sensitization, the dye was photoreduced in the presence of a suitable reductant such as phenyltioacetic acid [8–10], N-phenylglycine [9, 10], amine [11–13], and alkyltriphenylborate salt [14, 15].

In the last decade, dye/coinitiators systems working under visible irradiation via photooxidizable sensitization have been developed [3–7, 16–20]. In such photoredox pairs, N-alkoxypyridinium salts were commonly used as coinitiators. Upon electron transfer, these compounds yielded alkoxy radicals (Scheme 2) which initiated polymerization. The second important coinitiator is the derivative of 2,4,6-tris(trichloromethyl)-1,3,5-triazine. The halogenmethyl radicals formed are responsible for initiation of free radical polymerization (Scheme 3) [16–20].

It is well known in the literature that not all dyes are able to initiate photopolymerization with the aid of 2,4,6-tris(trichloromethyl)-1,3,5-triazine (Tz) [16]. Therefore, the primary goal of the presented study is the application of dye derivatives of 12H-quinoxalino-[2,3-b][1,4]-benzothiazine (1–3) in combination with Tz as a photoinitiator for free radical polymerization of a multifunctional acrylate (TMPTA). The structure of studied dyes and Tz are presented in Scheme 4. Moreover, the photodarkening mechanism of dye 1 during photolysis was studied. The mechanism proposed is supported by spectroscopic characterization of its radical cation and neutral radical in low-temperature matrices (mixture of CH₂Cl₂ and ionic liquid: 1-butyl-3-methylimidazolium hexafluorophosphate). The rigid environment of these matrices at cryogenic conditions on recombination and fragmentation processes allows for the direct observation of the transient species. This effect also allows for convenient observation of the undergoing processes upon a controlled annealing and softening of the rigid matrix environment.

2. Experimental

2.1. Generals

The procedure for preparing the dyes has been described elsewhere [7]. 2,4,6-tris(trichloromethyl)-1,3,5-triazine (Tz) and 1-methyl-2-pyrrolidone (MP) were purchased from Wako-Chemicals and Sigma-Aldrich, respectively. Acetonitrile (MeCN), 2-propanol (2-PrOH), dichloromethane (CH₂Cl₂), and carbon tetrachloride (CCl₄) were purchased from POCH (Poland). The ionic liquid, 1-butyl-3-methylimidazolium hexafluorophosphate (BMIM⁺), was prepared by following the method of Huddleston et al. [21].

The absorption and steady state fluorescence spectra were recorded using a Jasco V-670 spectrophotometer and Jasco FP 6300 spectrofluorimeter (Jasco, Japan), respectively. All photochemical experiments were carried out in a Rayonet Reactor RPR 200 (The Southern New England Ultraviolet Co, USA) equipped with lamps emitting light at 419 nm. A specific spectral band was isolated by the use of band-pass filters at 419 ± 10 nm. Illumination intensity was measured using uranyl oxalate actinometry [22].

2.2. Free Radical Polymerization

Free radical photopolymerization reactions were conducted in the presence of air in solvents composed of 1 mL of MP and 4 mL of TMPTA. Dye concentration was maintained at 0.1 mM, and the concentration of Tz was 10 mM. The rate of polymerization (R_p) was calculated from the following:

()

In the above expression, Q_s is a heat flow per second during the reaction, m is the mass of the monomer in the sample, M is the molar mass of the monomer, n is the number of double bonds per monomer, and ΔH_p is the theoretical enthalpy for complete polymerization of acrylate double bonds (20.6 kcal/mol) [23]. The heat flow was measured with a PT 401 temperature sensor (Elmetron, Poland), immersed in the sample. A polymerizing mixture containing the dye without Tz was used as a reference sample.

2.3. Pulse Radiolysis

Pulse radiolysis experiments were carried out with high energy (6 MeV) 17 ns electron pulses generated from an ELU-6 linear electron accelerator. All measurements were performed at room temperature. The dose absorbed per pulse was determined with N₂O saturated aqueous solution of KSCN (0.01 M), assuming mol/J and M⁻¹cm⁻¹ (G represents the radiation chemical yield and ε is a molar absorption coefficient at 475 nm). The dose delivered per pulse was within the range of 5 to 80 Gy. Details of the pulse radiolysis system are provided elsewhere [24, 25].

2.4. Cryogenic Measurements

Glassy samples were prepared by quench-freezing room temperature solutions in liquid nitrogen. The samples were 1.5 to 2 mm thick and were placed in a temperature-controlled liquid nitrogen-cooled cryostat (Oxford Instruments-OptiStat DN). The desired temperature (77 to 150 K) of the matrix was attained by automatically controlled heating. The samples mounted in a cryostat were irradiated with 4 μs electron pulses from the ELU-6 linear accelerator.

Radiolysis of the glassy sample of BMIM⁺

and CH₂Cl₂ led to the production of solvated electrons and oxidizing holes represented by radical dication BMIM^2+• and

(reaction (2)) or radical cation

(reaction (3)). The addition of methylene chloride to the matrix improved the solubility of many precursors but also resulted in more effective scavenging of electrons by dissociative electron attachment (reaction (4)) and led to a higher yield of radical cations generated by radiolysis. The positive charge was transferred to the solute molecule with a lower ionization potential (in this case the dye) to give the corresponding radical cation (reactions (5)–(7)):

()

Additionally, upon thermal annealing of the glassy samples chloromethyl radicals reacted with O₂, forming the oxidizing peroxyl radicals (reaction (8)), which subsequently oxidized the dye (reaction (9)):

()

3. Results and Discussion

3.1. Sensitized Free Radical Photopolymerization

The efficiency of benzothiazine dye derivatives of 12H-quinoxalino-[2,3-b][1,4]-benzothiazine (1–3) in combination with Tz as photoinitiating systems for the free radical polymerization of TMPTA was evaluated. It is well known, that the most efficient dyeing photoinitiators are the photoredox pair in which electron transfer occurs with the participation of the excited triplet states [4, 6, 7, 15]. Therefore, dyes 1–3 were selected as efficient oxidizable sensitizers with a high quantum yield of triplet state generation (~0.8 [7]). The spectroscopic and electrochemical properties of these dyes are presented in Table 1. The benzothiazine dyes absorbed light at higher wavelengths than Tz (304 nm); therefore the band-pass filters were used to irradiate the dye alone in photopolymerization experiments.

Table 1. Photophysical and electrochemical properties of studied dyes.

Dye	(nm)	(V)	E^00 c (kJ mol⁻¹)
1	425	0.97	260
2	424	0.79	259
3	442	0.90	253

^aIn 1-methyl-2-pyrrolidone from [7];
^bIn CH₃CN versus Fc⁺/Fc from [7]; Fc⁺/Fc = 0.38 versus SCE in CH₃CN;
^cIn CH₃CN.

The efficiency of the polymerization initiated by the dye/Tz systems was measured indirectly from the reaction’s heat flow during irradiation. The overall polymerization results are summarized in Table 2.

Table 2. Rate of photopolymerization, inhibition time, and thermodynamic parameters of studied photoredox pairs.

Dye	(μmol s⁻¹)	Inhibition time^a (s)	−ΔG_et (kJ mol⁻¹)
1	42.8	26	32.0
2	11.6	41	48.5
3	9.6	68	31.8

^a[Dye] = 0.1 mM, [Tz] = 10 mM.

The calculated polymerization rate of TMPTA (Table 2) indicated that the efficiency of polymerization strongly depended upon the structure of the dye employed. It was apparent that dye 1 significantly accelerated triacrylate photopolymerization in comparison with dyes 2 and 3. Free radical polymerization initiated by the tested photoredox pairs showed a significant inhibition time (Table 2). This effect should be related to the molecular oxygen dissolved in the composition. The oxygen both quenched the triplet state of the dye and reacted with the radical species generated by the dye/Tz systems. After consumption of the oxygen, the initiating radicals reacted with the monomer. As seen in Table 2, the most efficient photoredox pair, 1/Tz, had the shortest inhibition time.

It is well-known [26] that for polymerization initiated via intermolecular electron transfer process, the R_p can be described by the followings:

()

where A is a constant, which depends on the intensity of absorbed light (I_a), quantum yield of triplet state formation (Φ_T), the rate constants of polymerization (k_p) and chain termination steps (k_t), and the concentration of monomer and coinitiators. The examined dyes had the same value of singlet oxygen generation (~0.8 [7]) and one could conclude that their Φ_T values are also comparable. In the present study, the free energy change of electron transfer (ΔG_et) was calculated from the Rehm-Weller equation as follows [27]:

()

In this equation, E_ox (D/D^●+) and E⁰⁰(D) are the oxidation potential of the dye and the singlet excited state energy of the dye, respectively. Both parameters are given in Table 1. E_red (A^●−/A) is the reduction potential of Tz (−1.0 V [17]). The last term represents the Coulombic energy necessary to form an ion pair with charges Z₁ and Z₂ in a medium of dielectric constant ε for a distance r₁₂. This factor is often ignored, taking into account the overall value of ΔG_et. The calculated thermodynamic parameters listed in Table 2 indicate that all combinations of the benzothiazine dye/Tz systems possessed a strong driving force (−ΔG_et > 31 kJ mol⁻¹) upon exposure to light. The photoelectron transfer process occurred easily through the excited state. The detailed revision of the experimental data presented in Table 2 reveal that the photosystem 2/Tz with a high driving force for electron transfer (−ΔG_et) had moderate R_p and inhibition time in comparison with the other studied dyes. The same effects have been observed for photopolymerization initiated by the other photoredox systems [8, 20, 26].

3.2. Photodarkening Mechanism

During photopolymerization of the triacrylate monomer, the studied sensitizer does not really photobleach but photodarkens. An explanation of this phenomenon demands the identification of the products formed during photolysis. Therefore, the photooxidation mechanism of compound 1 was studied in detail. Because the proton of the nitrogen heteroatom in 1 can participate in the deprotonation reaction following the oxidation of benzothiazine, the pulse radiolysis of low temperature matrices was applied to the spectroscopic characterization of its radical cation and neutral radical. The electronic absorption spectrum of the radical cation 1^●+ obtained by low-temperature methodology is presented in Figure 1(A). The spectrum consisted of a strong absorption band at 514 nm and two smaller peaks at longer wavelengths of 620 nm and 675 nm. These bands decayed upon limited warming of the matrix (Figure 1(B)). The decrease of the absorption of 1^●+ was accompanied by an increase of the absorption band at 485 nm. This product was stable at room temperature.

Details are in the caption following the image — **Figure 1**
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Electronic absorption spectra obtained on oxidation of 1 (saturated solution, <0.01 M) embedded in a BMIM⁺ : CH₂Cl₂ (1 : 1) matrix. (A) spectra were collected after radiolysis at 77 K (a) and after annealing of the matrix at 140 K for 5 min (b) and for 15 min (c). (B) After annealing at 140 K for 25 min (a) and at 150 K for 10 min (b) and 20 min (c). The sample was 2 mm thick and received a radiation dose of 7.2 kGy.

Radical cations are more acidic than their neutral precursors and some of them are even superacids [28, 29]. Therefore they readily undergo deprotonation. Under matrix conditions the radical cation deprotonation can only start upon matrix softening. Therefore, one can conclude that radical cation 1^●+ undergoes deprotonation into the neutral radical 1^● (Scheme 5) on annealing of the matrix. The generation of the amine radical was more apparent in pulse radiolysis in CH₂Cl₂ at room temperature. Transient absorption spectra recorded under oxygen conditions are presented in Figure 2.

In such experimental conditions, a product with absorption bands at 440 nm, 460 nm, and 490 nm were observed. The bands were assigned to neutral radical 1^●. In an oxygen-saturated solution, the ^●CH₂Cl radical reacted rapidly with O₂ to form the peroxyl radical, which oxidized dye 1 to the radical cation 1^●+ that undergoes deprotonation into the neutral radical 1^●. Similar deprotonation of the radical cation of phenothiazine in n-butyl chloride was observed [30]. Therefore, the direct oxidation of compound 1 by the trichloromethylperoxyl radical to its radical cation was observed in a 2-PrOH-water solution with 0.1 M of HClO₄ at room temperature. The pKa of compound 1 in the 2-PrOH-water solution was estimated to be approximately 0.4. The transient absorption spectrum recorded in the acidic condition consisted of a strong absorption band at 500 nm and two smaller peaks at longer wavelengths of 550 and 600 nm. A similar absorption was obtained in the cryogenic matrix (see Figure 1(a)). Thus, the formation of 1^●+ was followed at 500 nm. The observed rate of oxidation increased linearly with dye concentration (0.56 to 0.96 mM). The plot of k_obs versus concentration of the dye was used to determine the second order rate constant ²k = (2.18 ± 0.08) × 10⁷ M⁻¹s⁻¹.

After spectroscopic characterization of 1^●+ and 1^●, the photolysis of benzothiazine dye 1 in composition with Tz was examined in MP. The electronic spectra recorded in MP showed the characteristic broad absorption band at 625 nm (Figure 3), which was assigned to 1^●+.

The same effect was observed during irradiation of the 1/Tz photoredox pair in MP containing 0.37 M TMPTA. Extending the irradiation time to 30 s caused an increase of the new band at 560 nm but the absorption bands of radical 1^● were not detected. When the photolysis was carried out with higher irradiation intensity (6 × 10¹⁶ quant s⁻¹) the broad absorption band at 560 nm was observed (Figure 4(a)).

Moreover, extending the irradiation time to 50–120 s caused a decrease in the absorption bands at 560 nm. Decay of the absorption at 560 nm is accompanied by the growth of a band near 358 nm. A similar absorption spectrum was observed for the dication of 12H-benzo [b]phenothiazine (4) [31] which is converted into cation by the lost of the proton. Therefore, one can conclude that radical cation 1^●+ underwent a one-electron oxidation to the dication 1²⁺ (Scheme 5). Then, 1²⁺ underwent deprotonation to cation 1⁺. The isosbestic point at 398 nm (Figure 4(b)) confirms such direct conversion.

()

For comparison the photolysis of dye 1 in CH₂Cl₂ was carried out. In this steady state photolysis dichloromethane was used as an electron acceptor. Electronic absorption spectrum (Figure 5) recorded after 15 minutes of irradiation showed the characteristic absorption bands at 412 nm, 435 nm, 462 nm, and 494 nm similar to the spectrum obtained during radiolysis (see Figure 2).

Thus, the product formed during photolysis in CH₂Cl₂ is neutral radical 1^●. The elongation of irradiation time to 50 min caused the decrease the absorption of 1^●. While the 1^● disappears, the band at 353 nm increases. Therefore, we assigned this new band to 1⁺ cation (Scheme 5), which might be formed during oxidation of 1^● by CH₂Cl₂ or peroxyl radical .

Based on the presented above results, one can assume that in MP, 1^●+ underwent a one-electron oxidation to the dication 1²⁺ (Scheme 5). It is concluded that the photodarkening of the polymer was caused by the radical cation or dication of the studied dyes and not the neutral radical. Such behavior is normally unwanted, particularly in composites, because it diminishes the curing of deeper layers of resin. However, in some situations, such as stereolithography, photodarkening may be an advantage, since it reduces the penetration of radiation below the top photocuring layer and allows higher pattern resolution.

4. Conclusions

Novel photoinitiator systems constructed with dye derivatives of 12H-quinoxalino-[2,3-b][1,4]-benzothiazine (1–3) and 2,4,6-tris(trichloromethyl)-1,3,5-triazine (Tz) are found to be effective initiation systems for free radical polymerization of TMPTA using VIS light. Photosensitization occurs through electron transfer, which was confirmed by the observation of a radical cation of the dyes studied during photolysis. The radical cation formed after electron transfer between benzothiazine dye 1 and Tz in MP underwent one-electron oxidation to yield the dication 1²⁺. The formation of the neutral radical 1^● was observed during radiolysis and photolysis of benzothiazine dye 1 in CH₂Cl₂. The cation 1⁺ was formed as results of two reactions: deprotonation of dication 1²⁺ or oxidation of neutral radical 1^●. The photodarkening of the polymers was caused by the radical cation or dication from the sensitizers.

Acknowledgments

This work was supported by the Polish Ministry of Science and Higher Education (Project no. N N205 1454 33).

References

1 Lowe C., Webster G., Kessel S., and McDonald I., Chemistry and Technology of UV and EB Formulation for Coatings, Inks and Paints, 1996, 4, Wiley, London, UK, Surface Coating Technology.
Google Scholar
2 Oldring P. K. T., Chemistry and Technology of UV and EB Formulation for Coatings, Inks and Paints, 1997, 5, Wiley, Sita Techn. Ltd., London, UK, Speciality Finishes.
Google Scholar
3 Podsiadły R., Photoreaction and photopolymerization studies on fluoflavin dye-pyridinium salt systems, Journal of Photochemistry and Photobiology A. (2008) 198, no. 1, 60–68, 2-s2.0-43849087017, https://doi.org/10.1016/j.jphotochem.2008.02.016.
10.1016/j.jphotochem.2008.02.016
CAS Web of Science® Google Scholar
4 Kolińska J., Podsiadły R., and Sokołowska J., Naphthoylenebenzimidazolone sensitisers for photo-oxidisable free radical polymerisation with the aid of pyridinium salts, Coloration Technology. (2008) 124, no. 6, 341–347, 2-s2.0-58149204222, https://doi.org/10.1111/j.1478-4408.2008.00161.x.
10.1111/j.1478-4408.2008.00161.x
CAS Web of Science® Google Scholar
5 Podsiadły R., Szymczak A. M., and Podemska K., The synthesis of novel, visible-wavelength, oxidizable polymerization sensitizers based on the 8-halogeno-5,12-dihydroquinoxalino[2,3-b]quinoxaline skeleton, Dyes and Pigments. (2009) 82, no. 3, 365–371, 2-s2.0-64849096817, https://doi.org/10.1016/j.dyepig.2009.02.008.
10.1016/j.dyepig.2009.02.008
CAS Web of Science® Google Scholar
6 Podsiadły R., The synthesis of novel, visible-wavelength oxidizable polymerization sensitizers based on the 5,12-dihydroquinoxalino[2,3-b]pyridopyrazine skeleton, Dyes and Pigments. (2009) 80, no. 1, 86–92, 2-s2.0-51249112205, https://doi.org/10.1016/j.dyepig.2008.05.005.
10.1016/j.dyepig.2008.05.005
CAS Web of Science® Google Scholar
7 Podsiadły R., Synthesis and photochemical reaction of novel, visible-wavelength oxidizable polymerization sensitizer based on the 12H-quinoxalino[2,3-b][1,4]benzothiazine skeleton, Journal of Photochemistry and Photobiology A. (2009) 202, no. 2-3, 115–121, 2-s2.0-59649125524, https://doi.org/10.1016/j.jphotochem.2008.11.017.
10.1016/j.jphotochem.2008.11.017
CAS Web of Science® Google Scholar
8 Podsiadły R., Sokołowska J., and Stoczkiewicz J., Styryl dyes as new photoinitiators for free radical polymerization, Dyes and Pigments. (2008) 77, no. 3, 510–514, 2-s2.0-36348975745, https://doi.org/10.1016/j.dyepig.2006.11.011.
10.1016/j.dyepig.2006.11.011
Web of Science® Google Scholar
9 Podsiadły R., Kolińska J., and Sokołowska J., Study of free radical polymerisation with dye photoinitiators containing a naphthoylenebenzimidazolone skeleton, Coloration Technology. (2008) 124, no. 2, 79–85, 2-s2.0-41149100510, https://doi.org/10.1111/j.1478-4408.2008.00125.x.
10.1111/j.1478-4408.2008.00125.x
CAS Web of Science® Google Scholar
10 Przyjazna B., Kucybała Z., and Pączkowski J., Development of new dyeing photoinitiators based on 6H-indolo[2,3-b] quinoxaline skeleton, Polymer. (2004) 45, no. 8, 2559–2566, 2-s2.0-1642388650, https://doi.org/10.1016/j.polymer.2004.02.025.
10.1016/j.polymer.2004.02.025
CAS Web of Science® Google Scholar
11 Encinas M. V., Rufs A. M., Bertolotti S. G., and Previtali C. M., Xanthene dyes/amine as photoinitiators of radical polymerization: a comparative and photochemical study in aqueous medium, Polymer. (2009) 50, no. 13, 2762–2767, 2-s2.0-66049142574, https://doi.org/10.1016/j.polymer.2009.04.024.
10.1016/j.polymer.2009.04.024
CAS Web of Science® Google Scholar
12 Wan X., Zhao Y., Xue J., Wu F., and Fang X., Water-soluble benzylidene cyclopentanone dye for two-photon photopolymerization, Journal of Photochemistry and Photobiology A. (2009) 202, no. 1, 74–79, 2-s2.0-58249100309, https://doi.org/10.1016/j.jphotochem.2008.10.029.
10.1016/j.jphotochem.2008.10.029
CAS Web of Science® Google Scholar
13 Fitilis I., Fakis M., Polyzos I., Giannetas V., and Persephonis P., Two-photon polymerization of a diacrylate using fluorene photoinitiators-sensitizers, Journal of Photochemistry and Photobiology A. (2010) 215, no. 1, 25–30, 2-s2.0-77956612275, https://doi.org/10.1016/j.jphotochem.2010.07.016.
10.1016/j.jphotochem.2010.07.016
CAS Web of Science® Google Scholar
14 Kabatc J., Multicationic monomethine dyes as sensitizers in two- and three-component photoinitiating systems for multiacrylate monomers, Journal of Photochemistry and Photobiology A. (2010) 214, no. 1, 74–85, 2-s2.0-77955560167, https://doi.org/10.1016/j.jphotochem.2010.06.011.
10.1016/j.jphotochem.2010.06.011
CAS Web of Science® Google Scholar
15 Kabatc J. and Paczkowski J., Monomeric asymmetric two- and three-cationic monomethine cyanine dyes as novel photoinitiators for free-radical polymerization, Dyes and Pigments. (2010) 86, no. 2, 133–142, 2-s2.0-76449102595, https://doi.org/10.1016/j.dyepig.2009.12.007.
10.1016/j.dyepig.2009.12.007
CAS Web of Science® Google Scholar
16 Tarzi O. I., Allonas X., Ley C., and Fouassier J. P., Pyrromethene derivatives in three-component photoinitiating systems for free radical photopolymerization, Journal of Polymer Science A. (2010) 48, no. 12, 2594–2603, 2-s2.0-77952969205, https://doi.org/10.1002/pola.24039.
10.1002/pola.24039
CAS Google Scholar
17 Grotzinger C., Burget D., Jacques P., and Fouassier J. P., Photopolymerization reactions initiated by a visible light photoinitiating system: dye/amine/ bis(trichloromethyl)-substituted-1,3,5-triazine, Macromolecular Chemistry and Physics. (2001) 202, no. 18, 3513–3522, 2-s2.0-0035960995.
10.1002/1521-3935(20011201)202:18<3513::AID-MACP3513>3.0.CO;2-Z
CAS Web of Science® Google Scholar
18 Karatsu T., Yanai M., Yagai S., Mizukami J., Urano T., and Kitamura A., Evaluation of sensitizing ability of barbiturate-functionalized non-ionic cyanine dyes; application for photoinduced radical generation system initiated by near IR light, Journal of Photochemistry and Photobiology A. (2005) 170, no. 2, 123–129, 2-s2.0-13944252107, https://doi.org/10.1016/j.jphotochem.2004.08.010.
10.1016/j.jphotochem.2004.08.010
CAS Web of Science® Google Scholar
19 Urano T., Nagao T., Takada A., and Itoh H., Photosensitization mechanisms in photopolymer coating film containing photoinitiators sensitized by aminochalcone-type dye for computer-to-photopolymer plate, Polymers for Advanced Technologies. (1999) 10, no. 4, 244–250, 2-s2.0-0032672142.
10.1002/(SICI)1099-1581(199904)10:4<244::AID-PAT871>3.0.CO;2-D
CAS Web of Science® Google Scholar
20 Podsiadły R. and Sokołowska J., Synthesis of novel oxidizable polymerization sensitizers based on the dithiinoquinoxaline skeleton, Dyes and Pigments. (2012) 92, no. 3, 1300–1307.
10.1016/j.dyepig.2011.09.006
CAS Web of Science® Google Scholar
21 Huddleston J. G., Willauer H. D., Swatloski R. P., Visser A. E., and Rogers R. D., Room temperature ionic liquids as novel media for “clean” liquid-liquid extraction, Chemical Communications. (1998) no. 16, 1765–1766, 2-s2.0-21844432372.
10.1039/A803999B
Web of Science® Google Scholar
22 Leighton W. B. and Forbes G. S., Precision actinometry with uranyl oxalate, Journal of the American Chemical Society. (1930) 52, no. 8, 3139–3152, 2-s2.0-0011397329.
10.1021/ja01371a015
Web of Science® Google Scholar
23 Avci D., Nobles J., and Mathias L. J., Synthesis and photopolymerization kinetics of new flexible diacrylate and dimethacrylate crosslinkers based on C18 diacid, Polymer. (2003) 44, no. 4, 963–968, 2-s2.0-0037449618, https://doi.org/10.1016/S0032-3861(02)00899-6.
10.1016/S0032-3861(02)00899-6
CAS Web of Science® Google Scholar
24 Karolczak S., Hodyr K., Łubis R., and Kroh J., Pulse radiolysis system based on ELU-6E LINAC, Journal of Radioanalytical and Nuclear Chemistry Articles. (1986) 101, no. 2, 177–188, 2-s2.0-34250131432, https://doi.org/10.1007/BF02042418.
10.1007/BF02042418
CAS Web of Science® Google Scholar
25 Karolczak S., Hodyr K., and Polowinski M., Pulse radiolysis system based on ELU-6E LINAC - II. Development and upgrading the system, Radiation Physics and Chemistry. (1992) 39, no. 1, 1–5, 2-s2.0-0026797203.
CAS Web of Science® Google Scholar
26 Pączkowski J. and Kucybała Z., Generalization of the kinetic scheme for a dye-photosensitized free-radical polymerization initiating system via an intermolecular electron-transfer process. Application of marcus theory, Macromolecules. (1995) 28, no. 1, 269–273, 2-s2.0-0029632164.
10.1021/ma00105a036
CAS Web of Science® Google Scholar
27 Rehm D. and Weller A., Kinetics of fluorescence quenching by electron and H-atom transfer, Israel Journal of Chemistry. (1970) 8, no. 2, 259–271.
10.1002/ijch.197000029
CAS Web of Science® Google Scholar
28 Bally T., A. Lund and M. Shiotani, Properties in condensed phases, Radical Ionic Systems, 1991, Kluwer Academic, Dordrecht, The Netherlands, 3–54.
10.1007/978-94-011-3750-8_1
Google Scholar
29 Gębicki J. and Marcinek A., Z. B. Alfassi, Radical Ions: generation, characterization and reactions, General Aspects of the Chemistry of Radicals, 1999, Wiley, Chichester, UK, 175–208.
Google Scholar
30 Brede O., Maroz A., Hermann R., and Naumov S., Ionization of cyclic aromatic amines by free electron transfer: products are governed by molecule flexibility, Journal of Physical Chemistry A. (2005) 109, no. 36, 8081–8087, 2-s2.0-25444441554, https://doi.org/10.1021/jp053172x.
10.1021/jp053172x
CAS PubMed Web of Science® Google Scholar
31 Urasaki N., Yoshida S., Ogawa T., Kozawa K., and Uchida T., Oxidation potential and absorption spectra of phenothiazine derivatives I. Benzophenothiazine and triphenodithiazine, Bulletin of the Chemical Society of Japan. (1994) 67, no. 8, 2024–2030.
10.1246/bcsj.67.2024
CAS Web of Science® Google Scholar

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Benzothiazine Dyes/2,4,6-Tris(trichloromethyl)-1,3,5-triazine as a New Visible Two-Component Photoinitiator System

Abstract

1. Introduction