Abstract
We demonstrated microwave-assisted photooxidation of sulfoxides to the corresponding sulfones using ethynylbenzene as a photosensitizer. Efficiency of the photooxidation was higher under microwave irradiation than under conventional thermal heating conditions. Under the conditions, ethynylbenzene promoted the oxidation more efficiently than conventional photosensitizers benzophenone, anthracene, and rose bengal. Ethynylbenzene, whose T1 state is extremely resistant to intersystem crossing to the ground state, was suitable to this reaction because spectroscopic and related reported studies suggested that this non-thermal effect was caused by elongating lifetime of the T1 state by microwave. This is the first study in which ethynylbenzene is used as a photosensitizer in a microwave-assisted photoreaction.
Subject terms: Chemistry, Catalysis, Organic chemistry
Introduction
Microwave (MW)-assisted reactions have recently been established as a successful synthetic method because of their enhanced reaction rates, increased yields, and suppressed side reactions and because they do not require solvents, unlike the thermally assisted reactions1–18. Non-thermal effects of MWs have been observed in some cases where the reaction proceeds much faster under MW irradiation than under conventional heating conditions. Interestingly, existence of the non-thermal effects of MWs is still a debatable topic4,5. The non-thermal effects of MWs are usually thought to originate due to three factors: dipolar polarization, ionic conduction, and non-thermal effects of highly polarizing radiation. Lately, the non-thermal effects of MWs were investigated at the liquid–solid interface, and nonequilibrium heating and accelerated electron transfer were determined to be the main factors responsible this effect19,20. This effect was also observed during decarboxylation using a silicon nanowire-array stabilized-Rh nanoparticle catalyst, and the reaction proceeded only under MW irradiation8. However, the precise mechanism by which these non-thermal effects are manifested is still elusive, and in particular, MW-assisted photoreactions are unexplored21,22. Considering this, we chose to investigate the photooxidation of sulfoxides in this study because the sulfones produced in this reaction have broad applications in the industrial, healthcare, and pharmaceutical sectors in the form of polyphenylsulfones, dimethyl sulfone23, and some coxibs24, respectively. Sulfones are synthesized either via the oxidation of sulfides or sulfoxides with peroxides25,26 or hypervalent iodine27, or by coupling sulfonates with haloarenes28, or via photooxidation29. However, these methods require the use of heavy metals or a high-pressure mercury lamp, and this should be strictly avoided. Thus, development of an unprecedented MW-assisted photooxidation reaction of sulfones using an organic photosensitizer is desirable both in the industry and academia. Herein, we report the ethynylbenzene-catalyzed photooxidation of sulfoxides and the mechanism by which the non-thermal effects of MWs are manifested in this reaction, where microwave is used to promote the photooxidation effectively.
Results and discussion
The photooxidation of dimethylsulfoxide (1a) to dimethylsulfone (2a) was investigated using various photosensitizers under white light (Xe lamp) or MW irradiation (8 W, 2.45 GHz) at 50 °C for 20 h (Table 1). The temperature in the MW-irradiated conditions was monitored with an IR thermometer from outside, and was confirmed to be comparable to that measured with an optical fiber thermometer. The temperature of the reaction mixture was maintained at 50 °C during the reaction time. Ethynylbenzene (3) acted as a photosensitizer and promoted the oxidation to give 2a in 31% yield (Entry 1; for detail, see Supplementary Figs. S1–S3 online). To the best of our knowledge, this is the first example of an oxidation reaction using ethynylbenzene as a photocatalyst. Notably, thermal heating alone, in the absence of MW irradiation, lowered the yield to 15% (Entry 2), suggesting that the oxidation was accelerated under MW irradiation. However, benzoic acid, presumably derived from 3, was detected in 4% and 18% yields (Entries 1 and 2) in the presence and absence, respectively, of MW irradiation. The reaction did not proceed at all in the dark (Entry 3) and afforded the product in 5% yield in the absence of a photosensitizer (Entry 4). The yield of 2a decreased when common photosensitizers, such as, benzophenone, anthracene, and rose bengal were used (Entries 5–7). Para-iodo substituted ethynylbenzene rather decreased the yield (Entry 9) comparing with non-substituted one (Entry 1). In the absence of MW, the yields afforded by rose bengal and p-iodoethynylbenzene showed no significant difference from those under irradiation of MW respectively (Entries 8 and 10). Thus, 3 was the best photosensitizer for this MW-assisted photooxidation. The role of the functional group on 3 was investigated next. Diphenylacetylene and biphenyl gave 2a in 11% and 10% yields, respectively (Entries 11 and 12), suggesting that the terminal alkynyl group was the crucial moiety in the photosensitizer. Benzoic acid, which is presumably a decomposed product of 3, did not have any specific role, either individually or in combination with 3, in this reaction (Entries 13 and 14). No peracids were detected under any of the reaction conditions, suggesting that the oxidation did not proceed via peracid intermediates. Lowering the light intensity (15 mW/cm2 at 450 nm) decreased the yield of 2a to 19% (Entry 13). When the reaction was conducted in toluene under the conditions corresponding to Entry 1, 2a was obtained in 25% yield, suggesting that toluene is applicable to this reaction (Entry 16). Increasing the reaction time to 48 h linearly increased the yield to 77% (Entry 17). In the absence of either MW or light irradiation, 2a was obtained in 21% and 0% yields, respectively, after 48 h (Entries 18 and 19). This observation suggested the synergistic effect of MW and light in this reaction. Only 2% yield of 2a was detected in the presence of a selective singlet oxygen quencher Co(acac)3 (Entry 20).
Table 1.
Screening of photosensitizer in the MW-assisted photooxidation of dimethyl sulfoxide (1a).
| ||||
|---|---|---|---|---|
| Entry | PSa | MW | Yield of 2a (%)b | Recovery of 1a (%)b |
| 1 | PhC≡CH 3 | + | 31 | 69 |
| 2 | 3 | − | 15 | 81 |
| 3d | 3 | + | 0 | 100 |
| 4 | None | + | 5 | 91 |
| 5 | Benzophenone | + | 12 | 87 |
| 6 | Anthracene | + | 24 | 74 |
| 7 | Rose bengal | + | 3 | 94 |
| 8 | Rose bengal | − | 4 | 93 |
| 9 | p-I-C6H4-C≡CH | + | 3 | 94 |
| 10 | p-I-C6H4-C≡CH | - | 7 | 89 |
| 11 | PhC≡CPh | + | 11 | 86 |
| 12 | Ph–Ph | + | 10 | 90 |
| 13 | PhCO2H | + | 7 | 91 |
| 14 | 3 + PhCO2H | + | 30 | 67 |
| 15d | 3 | + | 19 | 81 |
| 16e | 3 | + | 25 | 75 |
| 17f. | 3 | + | 77 | 22 |
| 18f. | 3 | − | 21 | 75 |
| 19b,f | 3 | + | 0 | 100 |
| 20g | 3 | + | 2 | 98 |
Reaction conditions: 1a (15 mmol) and photosensitizer (0.75 mmol) were used with O2 balloon under MW (8 W) irradiation and white light irradiation from Xe lamp (30 mW/cm2 at 450 nm) at 50 °C for 20 h.
aPS = photosensitizer.
bDetermined using 1H NMR with 1,3,5-trimethoxybenzene as the internal standard.
cIn the dark.
dWhite light (15 mW/cm2 at 450 nm).
eIn toluene (1 mL).
f48 h.
gIn the presence of Co(acac)3 (0.75 mmol).
With the optimized conditions in hand, various sulfoxides were examined for this reaction (Fig. 1) using toluene as a solvent. Compounds 1b (dibutyl sulfoxide) and 1c (dioctyl sulfoxide) were oxidized to give 2b and 2c in 90% and 70% yields, respectively. Cyclic sulfoxides 1d and 1e and dibenzyl sulfoxide 1f. were also converted to the corresponding sulfones in 50–56% yields. Aromatic substrates like methyl phenyl sulfoxide (1g) and diphenyl sulfoxide (1h) were oxidized to give the corresponding products in 45% and 10% yields, respectively. Thus, alkyl sulfoxides are oxidized efficiently in this reaction, while the product yields decrease with increasing number of phenyl groups in the substrate. This further implies that the electron density of the sulfur atom and/or the competition between 3 and the phenyl groups for light absorption affect the yields. This is also true when 1a or 1f. Is used as the substrate. For substrates 1b–1h, benzaldehyde was obtained as the byproduct and is probably derived from toluene.
Figure 1.
Substrate scope.aReaction conditions: 1 (5.0 mmol) and 3 (0.25 mmol) were used in dry-toluene (2.0 mL) with O2 balloon under white light irradiation using a Xe lamp (30 mW/cm2 at 450 nm) and MW irradiation (8 W) at 50 °C. Yields were determined using 1H NMR with 1,3,5-trimethoxybenzene as the internal standard. The Numbers in parentheses mean the rate of substrate recovery. a,b1a (15 mmol) and 3 (0.75 mmol) were used without any solvent. c1.0 mL of dry-toluene was used.
To gain insights into the mechanism, MW was irradiated as an individual electric field using a single-mode cavity (employing E-max in TM010 mode; for detail, see Supplementary Figs. S4–S5 online)8,30–32 for 3 h under the optimized conditions mentioned in Fig. 2. Compound 2a was obtained in 11% yield in this mode, while it was obtained in 4% yield under thermal heating conditions. This suggested that the electric field component of the MW contributed to the progress of this reaction.
Figure 2.
Effect of the electric field component of MW.
To investigate the reaction mechanism, electronic absorption spectrum of ethynylbenzene was acquired in DMSO. Ethynylbenzene showed an absorption band in the region 260–320 nm, which is beyond the absorption edge of DMSO (Supplementary Table S2 and Fig. S7a online). This indicated that the ethynylbenzene could be effectively photoexcited in DMSO. The absorption band of 3 in this region was assigned to the π–π* transition33. The π– π* transition corresponding to the S0-S1 transition was further confirmed by density functional theory at the B3LYP/6-31G* level (Supplementary Table S1 and Fig. S6 online).
Based on the above observations, a plausible mechanism of oxidation was proposed (Fig. 3). Upon UV light absorption, 3 is excited from the S0 (singlet ground) state to the S1 (excited) state, which is converted to the T1 state through intersystem crossing. In the T1 state, 3 reacts with triplet dioxygen to excite the singlet oxygen, which subsequently oxidizes the sulfoxide, and then relaxes to the S0 state. The lifetime of the T1 state of ethynylbenzene is the key to the success of this reaction. Johnson and Sears reported that the T1 state of ethynylbenzene is extremely resistant to intersystem crossing to the ground state34. The significance of the T1 state seems to be reflected in the result shown in Table 1, Entry 9 as the phosphorescence lifetimes of the iodo-substituted ethynylbenzene, whose lifetimes decrease markedly with increasing mass of the iodine atom35. The results in control experiments using various halo substituted ethynylbenzenes also support this hypothesis (Table S1). Moreover, MW is known to make a significant perturbation to triplet spin state population with elongate its lifetime36. Photon energy of MW of 2.45 GHz frequency is ~10 μeV, and this is of the same order as the energy difference between the original T1 state and the two sublevels (9 and 12 μeV, calculated from the reported zero field parameters D and E)37. Such variation in population in the T1 state is known in the field of optically detected magnetic resonance (ODMR) spectroscopy38. The longer lifetime T1 state under the MW irradiation makes the encounter with O2 more efficient and thus, the oxidation proceeds more efficiently (Fig. 3a) compared to that involving the short-lived T1 state without irradiation of MW (Fig. 3b). The increased yield under MW irradiation can be attributed to this effect. The mechanism involving singlet oxygen was supported by a detection of singlet oxygen luminescence (21% quantum yield) in the presence of ethynylbenzene measured in toluene (Figure S16) and the result shown in Table 1, entry 20 (The measurements were carried out in toluene and in DMSO with benzophenone as the standard (quantum yield of singlet oxygen generation (Φ = 29%39). The measurement in toluene showed a luminescence signal of singlet oxygen, whose quantum yield was calculated to 21% (Figure S16), whereas that in DMSO, no signal was observed.).
Figure 3.

Proposed energy dissipation pathways. Green arrows indicate the direction of energy transfer as the oxidation progresses. Thickness of the arrows corresponds to the feasibility of the process. (a) Mechanism under MW irradiation using ethynylbenzene. (b) Energy dissipation pathways of ethynylbenzene and O2 in the absence of MW.
Summary
In summary, we developed the MW-assisted photo-induced auto-oxidation of sulfoxides using ethynylbenzene as a photosensitizer. The oxidation is initiated by the π–π* transition, and the electric field of the MW is considered to prolong the lifetime of the T1 state that catalyzes the subsequent reaction. This speculation is supported by the correlation between the yields obtained using the iodo-substituted ethynylbenzene and the atomic weight of the corresponding iodine. Extended lifetimes of the T1 state upon MW irradiation have been utilized only in ODMR spectroscopy, and thus, this study is expected to bridge this spectroscopic technique with organic reactions and pioneer a new interdisciplinary area. Further investigation by survey of ethynylbenzene derivatives will be undertaken for improving the conversion of the substrates.
Methods
General
A 10 mL quartz vial or 6 mL glass vial (NT-16H, purchased from the Maruemu Corporation) were used, which was placed in a MW reactor (Discover, purchased from CEM Japan Corporation, or MR-2G-200R, purchased from Ryowa-electronics Corporation) or in an aluminum block on a hot plate under an irradiation of white light emitted from a Xe lamp (purchased from Asahi spectra).
General procedure for the oxidation using MW reactor
To a mixture of ethynylbenzene (0.75 mmol) and dry-DMSO 1a (15 mmol) in the 10 mL quartz vial, quartz beads were added (3.0 mm, 7 pcs). The vial was filled with O2, and closed with a silicone rubber cap which was connected via a PTFE tube to an O2 balloon. The vial was placed in the MW reactor (Discover) equipped with a quartz rod which guides white light emitted from the Xe lamp to the reactor, and heated at 50 ºC using MW (8 W) under an irradiation of the white light (30 mW/cm2, fixed at 450 nm) with blowing with a compressor. After a certain reaction time, the resulting mixture was analyzed by 1H NMR (500 MHz, CDCl3) to calculate a yield of 2a and a recovery of 1a using 1,3,5-trimethoxybenzene (δ 3.77, 9H) as the internal standard. In the cases of substrates 1b–1f, 5.0 mmol of a substrate in dry-toluene (1b: 1.0 mL, the others: 2.0 mL) was used instead of 1a without the quartz beads.
General procedure for the oxidation under conventional thermal heating conditions
The 6 mL glass vial containing a mixture of ethynylbenzene (0.75 mmol) and dry-DMSO (15 mmol) was filled with O2, and closed with a septum cap equipped with a quartz rod which guides white light emitted from the Xe lamp to the vial. To the vial, a needle which was connected via a silicone tube to an O2 balloon was inserted through the septum. The vial was placed in the aluminum block on a hot plate and heated at 50 °C under an irradiation of the white light (30 mW/cm2, fixed at 450 nm). After a certain reaction time, the resulting mixture was analyzed by 1H NMR (500 MHz, CDCl3) to calculate a yield of 2a and a recovery of 1a using 1,3,5-trimethoxybenzene (δ 3.77, 9H) as the internal standard.
General procedure for the oxidation under an electric field mode of MW
To a mixture of ethynylbenzene (0.31 mmol) and dry-DMSO 1a (6.1 mmol) in the 10 mL quartz vial, quartz beads were added (3.0 mm, 7 pcs). The vial was filled with O2, and closed with a silicone rubber cap which was connected via a PTFE tube to an O2 balloon. The vial was placed at the maximum points of the electric field in the MW single mode cavity equipped with an IR thermometer, a wave detector, a double-stub tuner connected to the MW generator (MR-2G-200R, 2.5 GHz), and a quartz rod which guides white light emitted from the Xe lamp to the reactor, and then heated at 50 ºC with MW (0.6 W) under an irradiation of the white light (30 mW/cm2, fixed at 450 nm) with blowing with DC fan (San-Ace, Sanyo Denki Corporation). After 3 h, the resulting mixture was analyzed by 1H NMR (500 MHz, CDCl3) to calculate a yield of 2a and a recovery of 1a using 1,3,5-trimethoxybenzene (δ 3.77, 9H) as the internal standard.
Supplementary Information
Acknowledgements
This work was supported by Nagoya University (GTR program), JSPS KAKENHI Grant Number JP 20K15327, and RIKEN. HOKUSAI (RIKEN) provided the computational facilities for the DFT calculations.
Author contributions
Y.M.A.Y. designed and organized the project of microwave-assisted photocatalysis. Y.M. conducted the experiments, synthesized the substrates, and analyzed by NMR. Y.M. and A.M. carried out UV–Vis analysis of ethynylbenzene. A.M., T.M., M.U. and H.T. conceived and conducted the DFT calculations. Y.M. wrote the manuscript with support by Y.M.A.Y., A.M., M.U. and H.T. All authors provided feedback and contributed to the final manuscript.
Competing interests
The authors declare no competing interests.
Footnotes
Publisher's note
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Supplementary Information
The online version contains supplementary material available at 10.1038/s41598-021-99322-9.
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