Dicky Annasa,
Shamim Ahmed Hiraa,
Sehwan Songb,
Jong-Seong Baec,
Sungkyun Parkb and
Kang Hyun Park*ad
aDepartment of Chemistry, Pusan National University, Busan, 46241, South Korea. E-mail: chemistry@pusan.ac.kr
bDepartment of Physics, Pusan National University, Busan, 46241, South Korea
cBusan Center, Korea Basic Science Institute, Busan 46742, South Korea
dSoulDot Co., Ltd, Pusan National University, Busandaehak-ro 63beon-gil, Geumjeong-gu, Busan 46241, Korea
First published on 6th October 2021
Mixed metal–metal oxide/C (Ag–Cu–Cu2O/C) nanocomposites were synthesized by the heat treatment of a metal–organic framework under a N2 flow using the one-pot synthesis method. The as-prepared nanocomposites were characterized using a range of techniques, such as TEM, elemental mapping, XRD, N2 sorption, UV-Vis DRS, and XPS. The nanoparticles were successfully formed with high dispersion in porous carbon materials and high crystallinity based on the analysis results. The Ag–Cu–Cu2O/C nanocomposites (35 nm) showed high photocatalytic activity and good recyclability toward the borylation of aryl halides under a xenon arc lamp. This result can enhance the interest in photocatalysis for various applications, particularly in organic reactions, using a simple and efficient synthesis method.
Support materials, such as carbon, zeolites, graphene, silica, and metal–organic frameworks, are used to load the metal and metal oxides nanocomposites in their surface to produce a heterogeneous catalyst. These support materials minimize aggregation between materials and increase stability when used as a catalyst in various reactions. Carbon is a commonly used support material because of its high mechanical properties, high electrical properties, high thermal properties, an high surface area.9–11 In addition to being used as a support material to increase the catalytic activity, the interactions between carbon and metal or metal oxides nanocomposites are limited to physical interactions between the carbon and the materials, and that there is a synergistic effect when these materials are used in catalytic reactions.12
Recently, metal–organic frameworks (MOFs), which are porous materials and contain an organic linker and metal ions or clusters, have attracted considerable attention in various fields, such as gas storage, gas adsorption, drug delivery, sensors, and heterogeneous catalysis.13–16 These materials provide high surface area, tunable porosities, large pore size, and straightforward synthesis.17 Although MOFs are used in various fields, they are unstable and tend to collapse during high thermal, resulting in a decrease in catalytic activity.18 The reduction of metal cations in MOFs to metal nanoparticles and metal oxide nanoparticles can be achieved by thermal reduction and chemical reduction or a combination of both methods.19,20 As a result, these nanocomposites have good stability and high catalytic activity. In addition, it also generates a synergistic effect between metal/metal oxide and support material.
The Cu3(BTC)2 (BTC = 1,3,5-benzenetricarboxylate) is one of the Cu-MOF classes. Previous reports have shown that the calcination of Cu-MOF resulted in mixed Cu, Cu2O, and C under N2 gas conditions, which showed a high catalytic activity.12,21 The Cu metal and copper oxide (Cu2O and CuO) are important as catalysts in organic reactions. In particular, when a combination of both phases is attached to the support material, the catalytic activity will be higher than their single metal/metal oxide counterparts, especially under visible light.12 Moreover, the photocatalytic activity under visible light can be enhanced by adding other noble metal nanoparticles, such as Ag nanoparticles, because its surface plasmon resonance (SPR) improves the absorption of visible light.22–26
In this study, Ag–Cu–Cu2O/C nanocomposites were prepared using a one-pot synthesis method derived from Cu-MOF (Cu3(BTC)2) under N2 gas. Through this approach, the nanoparticles have small particles size, not easily to aggregate, and using simple and efficient synthesis method. These nanocomposites were applied as a catalyst in the borylation of aryl halides under visible light irradiation (Scheme 1). This reaction was chosen because it can produce arylboronic esters which are an important class of benchmark reagents with broad utility for organic synthesis. This is because these arylboronic esters have several advantages, such as air stability, easy of handling, having a wide functional group, etc. In addition, the chemical structure of arylboronic esters is reported to be used in pharmaceutical fields, such as anticancer, proteasome inhibitor, and antimitotic agent.27,28 Light irradiation is used in this reaction because it can activate aryl carbon–halogen bond dissociation, mild reaction conditions, and short reaction time.29–32
Scheme 1 Brief scheme for the synthesis of the Ag–Cu–Cu2O/C nanocomposites as catalyst for borylation of aryl halide. |
XRD was used to verify the crystallinity structure of the Ag–Cu–Cu2O/C nanocomposites and confirm with the reference data for Ag, Cu, and Cu2O. Fig. 2a presents the XRD pattern of Cu-BTC, which confirmed the formation of MOF. Cu–Cu2O/C nanocomposites were synthesized for comparison. The XRD pattern of these nanocomposites confirmed the presence of Cu2O with XRD peaks at 29.66, 36.58, 42.48, and 61.56° 2θ corresponding to the (110), (111), (200), and (220) planes of Cu2O nanoparticles, respectively (JCPDS # 78-2076) and Cu nanoparticles with diffraction peaks at 43.46, 50.58, and 74.27° 2θ, corresponding to the (111), (200) and (220) planes of Cu nanoparticles, respectively (JCPDS # 04-0836). The Ag–Cu–Cu2O/C nanocomposites showed a similar XRD pattern with the addition of Ag nanoparticles with peaks at 38.21, 44.38, 64.61, and 77.60° 2θ corresponding to the (111), (200), (220) and (311) planes, respectively (JCPDS # 89-3722) (Fig. 2b). Although the Ag–Cu–Cu2O/C nanocomposites had a similar XRD pattern to the Cu–Cu2O/C nanocomposites, they had different peak intensities, particularly the Cu2O peak intensities. In the Ag–Cu–Cu2O/C nanocomposites, the XRD peaks for Cu2O had a lower intensity compared to Cu–Cu2O/C nanocomposites due to the reduction process when silver was added to the synthesis process, and more Cu nanoparticles were produced.
The nitrogen adsorption and desorption isotherms of material were conducted using Brunauer–Emmett–Teller (BET) analysis to characterize the porosity of the material. The Ag–Cu–Cu2O/C nanocomposites exhibited type IV isotherm, which indicates that a mesoporous structure had formed (Fig. 3a). From this analysis, the surface area of the material was 39.63 m2 g−1. The average pore size of nanocomposites, which were analyzed using the Barrett–Joyner–Halenda (BJH) method, was 14.25 nm, which was determined from the adsorption and desorption of the isotherm (Fig. 3b).
Fig. 3 (a) N2 isotherms and (b) pore size distribution of Ag–Cu–Cu2O/C nanocomposites calculated using the BJH method. |
The chemical states and compositions of metal/metal oxides were analyzed by XPS. The XPS survey spectrum in Fig. 4a revealed Cu, Ag, C, and O in the Ag–Cu–Cu2O/C nanocomposites. The Cu 2p XPS spectra of the Ag–Cu–Cu2O/C nanocomposites indicated two major peaks at 932.28 eV (2p3/2) and 952.08 eV (2p1/2). The 2p3/2 peak confirmed that the copper exists only as Cu0 and Cu1+. No Cu2+ was observed in the material (Fig. 4c). The Ag 3d peaks appeared at 368.08 eV (3d5/2) and 373.97 eV (3d3/2). The binding energy of Ag 3d5/2 peak was consistent with the Ag0 reference peak (Fig. 4d). These results were well matched with the XRD patterns. In addition, the C 1s XPS spectra were obtained. The deconvolution of the C 1s spectra showed some peaks at 284.50, 286.23, 288.59, and 291.02 eV, which were assigned to C–C, C–O–C, O–CO, and π–π*, respectively (Fig. 4b). In addition, the optical properties of nanocomposites were characterized using UV-Vis DRS spectrophotometer. The Ag–Cu–Cu2O/C nanocomposites showed a strong absorbance and can absorb the light in the UV to visible region with the calculated band gap of 0.72 eV to excite electrons from the valence band to the conduction band (Fig. 5a).
Fig. 4 (a) XPS survey spectra of Ag–Cu–Cu2O/C nanocomposites and XPS spectra of (b) C 1s, (c) Cu 2p, and (d) Ag 3d of Ag–Cu–Cu2O/C nanocomposites. |
Fig. 5 (a) UV-Vis DRS of Ag–Cu–Cu2O/C nanocomposites and (b) the calculated band gap energy of Ag–Cu–Cu2O/C nanocomposites. |
Entry | Amount of catalyst | Base | Solvent | t (h) | Yieldb (%) |
---|---|---|---|---|---|
a Reaction conditions: 4-iodotoluene (1.2 mmol), bis(pinacolato)diboron (0.6 mmol), catalyst (2 mol%), base (2 equivalent), and xenon arc lamp with the intensity of 200 mW cm−2.b Yields determined by GC-MS. | |||||
1 | 1 mol% | (CH3)3COK | THF | 6 | 51 |
2 | 1 mol% | (CH3)3COK | Toluene | 6 | 62 |
3 | 1 mol% | (CH3)3COK | DMF | 6 | 83 |
4 | 1 mol% | (CH3)3COK | DMSO | 6 | 70 |
5 | 1 mol% | (CH3)3COK | Methanol | 6 | 42 |
6 | 1 mol% | (CH3)3COK | Ethanol | 6 | 41 |
7 | 1 mol% | (CH3)3COK | Dioxane | 6 | 27 |
8 | 1 mol% | NaOH | DMF | 6 | 73 |
9 | 1 mol% | KOH | DMF | 6 | 75 |
10 | 1 mol% | Cs2CO3 | DMF | 6 | 64 |
11 | 1 mol% | NaOMe | DMF | 6 | 36 |
12 | 2 mol% | (CH3)3COK | DMF | 6 | 96 |
13 | 3 mol% | (CH3)3COK | DMF | 6 | 97 |
14 | 2 mol% | (CH3)3COK | DMF | 3 | 71 |
15 | 2 mol% | (CH3)3COK | DMF | 1 | 43 |
Different bases were also used for this reaction. When strong bases, such as NaOH and KOH, were used, the yields decreased to 73 and 75%, respectively (Table 1, entries 8 and 9). This suggests that a strong base is not effective in this reaction. In addition, Cs2CO3 could not give a good result with a low yield (64%) (Table 1, entry 10). The lowest yield was afforded when NaOMe was used as a base (36%) (Table 1, entry 11). Thus, (CH3)3COK is the best base for this reaction compared to the other bases. The amount of catalyst was also screened. When the catalyst amount was increased to 2 and 3 mol%, the conversion increased to 96 and 97% (Table 1, entries 12 and 13). On the other hand, because there was almost no difference in yield between 2 and 3 mol% of catalyst, 2 mol% of catalyst was used as the optimal amount of catalyst in a further reaction. In addition, the yield also decreases to 71 and 43% when the reaction time was decreased to three and one hour, respectively (Table 1, entries 14 and 15). Thus, the following conditions were used for further experiments: DMF as the solvent, (CH3)3COK as the base, 2 mol% catalyst, 40 °C reaction temperature, and six-hour reaction time.
Furthermore, the photocatalytic activity of borylation of aryl halide was screened using various aryl halides under the optimal conditions. Under the optimal conditions, the reactions produced moderate to excellent yields. The methyl group as an electron-donating group at the para position of aryl halide afforded a high product yield of 96% (Table 2, entry 1). Another electron-donating group attached to the aryl halide, such as p-OH, also resulted in a high yield (93%) (Table 2, entry 5). Electron-withdrawing groups, such as m-OCH3, p-OCH3, and p-COCH3, also showed a high yield of approximately 95, 91, and 94%, respectively (Table 2, entries 2–4). On the other hand, the m-CF3 showed a moderate yield (84%) in this reaction (Table 2, entry 9). The use of iodoalkane groups, such as iodopropane and iodopentane, produced the highest yield of 98 and 99%, respectively (Table 2, entries 6 and 7). The heteroatomic group, such as 6-iodoquinoline, was also used in this reaction, and it showed a moderate yield of 85% (Table 2, entry 8). In addition, two cyanide groups at the meta and para positions showed moderate conversion with 82% yield (Table 2, entry 10). These results showed that this catalyst could be used for the borylation of various aryl halides under optimal conditions and xenon lamp irradiation.
For comparison, other catalysts were screened for this reaction under optimal conditions. The activity of Cu-BTC was analyzed and showed the lowest yield of 35% (Table 3, entry 2). Similar results also occurred when CuO and Cu2O were used as the catalysts for this reaction (38 and 43%) (Table 3, entries 4 and 5). This suggests that these materials are unsuitable for catalyzing the borylation of aryl halides even when a mixture of CuO and Cu2O was used (Table 3, entry 8). Moreover, moderate yields were also obtained when single Ag NPS and Cu NPS were used with 65 and 72%, respectively (Table 3, entries 6 and 7). The yield increased moderately when a mixture of Ag and Cu NPS was used (77%) (Table 3, entry 9). Cu–Cu2O/C nanoparticles derived from Cu-BTC were also synthesized for comparison using the same method as Ag–Cu–Cu2O/C without the addition of Ag. The results showed moderate conversion (81%) (Table 3, entry 3), indicating a synergistic effect between Ag, Cu, Cu2O, and C because of the high yield when Ag–Cu–Cu2O/C was used as a catalyst (Table 3, entry 1). In addition, the experiments without using light irradiation (dark experiment) and catalyst were conducted with low yields (Table 3, entries 10 and 11). Table 4 compares the borylation of aryl halides using the reported catalysts. The Ag–Cu–Cu2O/C nanocomposites had a better catalytic activity with a small amount of catalyst and a short reaction time than the reported catalysts.
Entry | Amount of catalyst | Catalyst | Solvent | t (h) | Yieldb (%) |
---|---|---|---|---|---|
a Reaction conditions: 4-iodotoluene (1.2 mmol), bis(pinacolato)diboron (0.6 mmol), catalyst (2 mol%), base (2 equivalent), and xenon arc lamp with the intensity of 200 mW cm−2.b Yields determined by GC-MS.c Yield without using light irradiation (dark experiment). | |||||
1 | 2 mol% | Ag–Cu–Cu2O/C | DMF | 6 | 96 |
2 | 2 mol% | Cu-BTC | DMF | 6 | 35 |
3 | 2 mol% | Cu–Cu2O/C | DMF | 6 | 81 |
4 | 2 mol% | CuO | DMF | 6 | 38 |
5 | 2 mol% | Cu2O | DMF | 6 | 43 |
6 | 2 mol% | Ag NPS | DMF | 6 | 65 |
7 | 2 mol% | Cu NPS | DMF | 6 | 72 |
8 | 2 mol% | 4 + 5 | DMF | 6 | 44 |
9 | 2 mol% | 6 + 7 | DMF | 6 | 77 |
10 | 2 mol% | Ag–Cu–Cu2O/C | DMF | 6 | 21c |
11 | — | — | DMF | 6 | 5 |
Catalyst | Method | Amount of catalyst | Reaction time (h) | Yield (%) | Ref. |
---|---|---|---|---|---|
Pd(PPh3)4 | Light irradiation | 3 mol% | 8 | 56 | 33 |
fac-Ir(ppy)3 | Light irradiation | 2.0 μmol | 16 | 79 | 34 |
DTC | Light irradiation | 10 mol% | 16 | 95 | 35 |
Fe[N(Si(CH3)3)2]2 | Without light | 10 mol% | 24 | 95 | 36 |
Cu–Cu2O/C | Light irradiation | 2 mol% | 6 | 81 | This work |
Ag–Cu–Cu2O/C | Light irradiation | 2 mol% | 6 | 96 | This work |
The recyclability test of Ag–Cu–Cu2O/C nanoparticles was conducted using 4-iodotoluene and bis(pinacolato)diboron under the optimized conditions. The catalyst was separated from the mixture, washed several times with methanol, and collected by centrifugation. The catalyst was dried in a vacuum oven at 80 °C and reused for seven cycles. Fig. 6 shows that the Ag–Cu–Cu2O/C nanoparticles have high photocatalytic activity without any significant decrease in photocatalytic activity with a >90% yield. Furthermore, the stability and durability of the nanoparticles were investigated after seven cycles using TEM characterization. After use, the nanoparticles maintained their particle size and did not undergo severe particle aggregation (Fig. 7).
Fig. 7 TEM image of the recovered Ag–Cu–Cu2O/C nanoparticles after 7 cycles reaction. The bar represents 100 nm. |
The photocatalysis reaction is the catalyst activity in the reaction process induced by UV-Vis light. Through this process, electrons and holes were generated and acted as charge carriers. Generally, photocatalysis using heterogeneous semiconductor catalysts, such as ZnO, CuO, Cu2O, and TiO2, are promising materials used in many fields.37–41 Moreover, the addition of metal nanoparticles, such as Ag and Cu, which have surface plasmon resonance (SPR) to absorb visible light, can form a Schottky barrier that suppresses the recombination of photogenerated electron–hole pairs at the interface between the metal and semiconductor.42–46 Electrons are excited from the valence band to the conduction band when the semiconductor material is excited by UV-Vis light. The excited electrons are transferred to the metal nanoparticles to suppress the recombination of photogenerated electron–hole pairs.47 This process generates radical species that are used in the borylation of aryl halide reactions. Based on previous studies reported by Mazzarella et al. (2019), the borylation of aryl halide reactions under light conditions was exploited in SN2-based radical generation.35 The catalyst can activate aryl halide as electrophile group via SN2 reaction. Then, aryl halide-catalyst intermediate undergoes the homolytic cleavage of C–X bond due to the light irradiation. Thus, it provides access to alkyl boronate esters to react with the aryl radical to form the product. Therefore, the formation of radicals from the photogenerated electron–hole pairs of Ag–Cu–Cu2O/C nanocomposites is necessary for the borylation of aryl halide reactions.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/d1ra05586k |
This journal is © The Royal Society of Chemistry 2021 |